CERN Accélérateur de science

002655508 001__ 2655508
002655508 005__ 20240314170926.0
002655508 0248_ $$aoai:cds.cern.ch:2655508$$pcerncds:CERN$$pcerncds:CERN:FULLTEXT$$pcerncds:FULLTEXT
002655508 0247_ $$2DOI$$9arXiv$$a10.1140/epjc/s10052-019-7181-x$$qpublication
002655508 037__ $$9arXiv$$aarXiv:1902.00377$$chep-ex
002655508 037__ $$9arXiv:reportnumber$$aCERN-EP-2018-262
002655508 035__ $$9arXiv$$aoai:arXiv.org:1902.00377
002655508 035__ $$9Inspire$$a1718132
002655508 041__ $$aeng
002655508 088__ $$9ATLAS-EXOT-2016-08-003
002655508 100__ $$aAaboud, Morad$$iINSPIRE-00511697$$tGRID:grid.189504.1$$uOujda U.$$vDepartment of Physics - Boston U. - Boston - MA - USA
002655508 245__ $$9arXiv$$aSearches for scalar leptoquarks and differential cross-section measurements in dilepton-dijet events in proton-proton collisions at a centre-of-mass energy of $\sqrt{s}$ = 13 TeV with the ATLAS experiment
002655508 260__ $$c2019-09-03
002655508 269__ $$aGeneva$$bCERN$$c01 Feb 2019
002655508 300__ $$a62 p
002655508 500__ $$9arXiv$$a62 pages in total, author list starting page 46, 19 figures, 5
  tables, published in EPJC. All figures including auxiliary figures are
  available at
  https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2016-08/
002655508 520__ $$aSearches for scalar leptoquarks pair-produced in proton-proton collisions at  $\sqrt{s}=13$ TeV at the Large Hadron Collider are performed by the ATLAS experiment. A data set corresponding to an integrated luminosity of 36.1 fb$^{-1}$ is used. Final states containing two electrons or two muons and two or more jets are studied, as are states with one electron or muon, missing transverse momentum and two or more jets. No statistically significant excess above the Standard Model expectation is observed. The observed and expected lower limits on the leptoquark mass at 95% confidence level extend up to 1.25 TeV for first- and second-generation leptoquarks, as postulated in the  minimal Buchm\"uller-R\"uckl-Wyler model, assuming a branching ratio into a charged lepton and a quark of 50%. In addition, measurements of particle-level fiducial and differential cross sections are presented for the $Z\rightarrow ee$, $Z\rightarrow\mu\mu$ and $t\bar{t}$ processes in several regions related to the search control regions. Predictions from a range of generators are compared with the measurements, and good agreement is seen for many of the observables.  However, the predictions for the $Z\rightarrow\ell\ell$ measurements in observables sensitive to jet energies disagree with the data.
002655508 520__ $$9Springer$$aSearches for scalar leptoquarks pair-produced in proton–proton collisions at $\sqrt{s}=13$  TeV at the Large Hadron Collider are performed by the ATLAS experiment. A data set corresponding to an integrated luminosity of 36.1 fb$^{-1}$ is used. Final states containing two electrons or two muons and two or more jets are studied, as are states with one electron or muon, missing transverse momentum and two or more jets. No statistically significant excess above the Standard Model expectation is observed. The observed and expected lower limits on the leptoquark mass at 95% confidence level extend up to 1.29 TeV and 1.23 TeV for first- and second-generation leptoquarks, respectively, as postulated in the minimal Buchmüller–Rückl–Wyler model, assuming a branching ratio into a charged lepton and a quark of 50%. In addition, measurements of particle-level fiducial and differential cross sections are presented for the $Z\rightarrow ee$ , $Z\rightarrow \mu \mu $ and $t\bar{t}$ processes in several regions related to the search control regions. Predictions from a range of generators are compared with the measurements, and good agreement is seen for many of the observables. However, the predictions for the $Z\rightarrow \ell \ell $ measurements in observables sensitive to jet energies disagree with the data.
002655508 520__ $$9arXiv$$aSearches for scalar leptoquarks pair-produced in proton-proton collisions at $\sqrt{s}=13$ TeV at the Large Hadron Collider are performed by the ATLAS experiment. A data set corresponding to an integrated luminosity of 36.1 fb$^{-1}$ is used. Final states containing two electrons or two muons and two or more jets are studied, as are states with one electron or muon, missing transverse momentum and two or more jets. No statistically significant excess above the Standard Model expectation is observed. The observed and expected lower limits on the leptoquark mass at 95% confidence level extend up to 1.29 TeV and 1.23 TeV for first- and second-generation leptoquarks, respectively, as postulated in the minimal Buchm\"uller-R\"uckl-Wyler model, assuming a branching ratio into a charged lepton and a quark of 50%. In addition, measurements of particle-level fiducial and differential cross sections are presented for the $Z\rightarrow ee$, $Z\rightarrow\mu\mu$ and $t\bar{t}$ processes in several regions related to the search control regions. Predictions from a range of generators are compared with the measurements, and good agreement is seen for many of the observables. However, the predictions for the $Z\rightarrow\ell\ell$ measurements in observables sensitive to jet energies disagree with the data.
002655508 540__ $$3Preprint$$aCC-BY-4.0$$uhttp://creativecommons.org/licenses/by/4.0/
002655508 540__ $$3Publication$$aCC-BY-4.0$$bSpringer
002655508 542__ $$3Preprint$$dCERN$$g2018
002655508 65017 $$2SzGeCERN$$aParticle Physics - Experiment
002655508 65017 $$2arXiv$$ahep-ex
002655508 6531_ $$9CERN$$aexotics
002655508 6531_ $$9CERN$$aparticle and resonance production
002655508 6531_ $$9CERN$$aexperimental results
002655508 693__ $$aCERN LHC$$eATLAS
002655508 690C_ $$aATLAS_Papers
002655508 690C_ $$aCERN
002655508 690C_ $$aARTICLE
002655508 700__ $$aAad, Georges$$iINSPIRE-00210391$$jORCID:0000-0002-6665-4934$$uMarseille, CPPM
002655508 700__ $$aAbbott, Brad$$iINSPIRE-00060668$$jORCID:0000-0002-5888-2734$$uOklahoma U.
002655508 700__ $$aAbdinov, Ovsat$$iINSPIRE-00210427$$uBaku, Inst. Phys.
002655508 700__ $$aAbeloos, Baptiste$$iINSPIRE-00436210$$uOrsay, LAL
002655508 700__ $$aAbhayasinghe, Deshan Kavishka$$iINSPIRE-00584514$$uRoyal Holloway, U. of London
002655508 700__ $$aAbidi, Syed Haider$$iINSPIRE-00537233$$jORCID:0000-0002-8496-9294$$uToronto U.
002655508 700__ $$aAbouzeid, Ossama$$iINSPIRE-00286103$$jORCID:0000-0002-8279-9324$$uBohr Inst.
002655508 700__ $$aAbraham, Nicola$$iINSPIRE-00443060$$uSussex U.
002655508 700__ $$aAbramowicz, Halina$$iINSPIRE-00060790$$jORCID:0000-0001-5329-6640$$uTel Aviv U.
002655508 700__ $$aAbreu, Henso$$iINSPIRE-00143063$$uTechnion
002655508 700__ $$aAbulaiti, Yiming$$iINSPIRE-00339001$$jORCID:0000-0003-0403-3697$$uArgonne
002655508 700__ $$aAcharya, Bobby Samir$$iINSPIRE-00060856$$jORCID:0000-0002-8588-9157$$uINFN, Udine$$uICTP, Trieste$$uKing's Coll. London
002655508 700__ $$aAdachi, Shunsuke$$iINSPIRE-00524597$$jORCID:0000-0002-0400-7555$$uTokyo U., ICEPP
002655508 700__ $$aAdamczyk, Leszek$$iINSPIRE-00172476$$jORCID:0000-0002-5859-2075$$uAGH-UST, Cracow
002655508 700__ $$aAdelman, Jahred$$iINSPIRE-00041460$$jORCID:0000-0002-1041-3496$$uNorthern Illinois U.
002655508 700__ $$aAdersberger, Michael$$iINSPIRE-00537240$$uMunich U.
002655508 700__ $$aAdiguzel, Aytul$$iINSPIRE-00307180$$jORCID:0000-0001-6644-0517$$uBogazici U.$$uIstanbul U.
002655508 700__ $$aAdye, Tim$$iINSPIRE-00060997$$jORCID:0000-0003-0627-5059$$uRutherford
002655508 700__ $$aAffolder, Tony$$iINSPIRE-00061029$$jORCID:0000-0002-9058-7217$$uUC, Santa Cruz
002655508 700__ $$aAfik, Yoav$$iINSPIRE-00564969$$uTechnion
002655508 700__ $$aAgheorghiesei, Catalin$$iINSPIRE-00534492$$jORCID:0000-0003-3695-1847$$uCuza U., Iasi
002655508 700__ $$aAguilar Saavedra, Juan Antonio$$iINSPIRE-00061050$$jORCID:0000-0002-5475-8920$$uGranada U., Theor. Phys. Astrophys.$$uLIP, Lisbon$$uMadrid, IFT
002655508 700__ $$aAhmadov, Faig$$iINSPIRE-00332895$$jORCID:0000-0003-3644-540X$$uDubna, JINR$$uBaku, Inst. Phys.
002655508 700__ $$aAielli, Giulio$$iINSPIRE-00210494$$jORCID:0000-0002-0573-8114$$uINFN, Rome2$$uRome U., Tor Vergata
002655508 700__ $$aAkatsuka, Shunichi$$iINSPIRE-00535642$$jORCID:0000-0002-1681-6405$$uKyoto U.
002655508 700__ $$aAkesson, Torsten Paul Ake$$iINSPIRE-00061248$$jORCID:0000-0003-4141-5408$$uLund U.
002655508 700__ $$aAkilli, Ece$$iINSPIRE-00546139$$jORCID:0000-0003-1309-5937$$uGeneva U.
002655508 700__ $$aAkimov, Andrei$$iINSPIRE-00210520$$uLebedev Inst.
002655508 700__ $$aAlberghi, Gian Luigi$$iINSPIRE-00366589$$jORCID:0000-0003-2388-987X$$uINFN, Bologna$$uBologna U.
002655508 700__ $$aAlbert, Justin$$iINSPIRE-00145104$$jORCID:0000-0003-0253-2505$$uVictoria U.
002655508 700__ $$aAlbicocco, Pietro$$iINSPIRE-00549776$$jORCID:0000-0001-6430-1038$$uFrascati
002655508 700__ $$aAlconada Verzini, Maria Josefina$$iINSPIRE-00339017$$jORCID:0000-0003-2212-7830$$uLa Plata U.
002655508 700__ $$aAlderweireldt, Sara Caroline$$iINSPIRE-00245271$$jORCID:0000-0002-8224-7036$$uNijmegen U.
002655508 700__ $$aAleksa, Martin$$iINSPIRE-00210567$$jORCID:0000-0002-1936-9217$$uCERN
002655508 700__ $$aAleksandrov, Igor$$iINSPIRE-00210579$$uDubna, JINR
002655508 700__ $$aAlexa, Calin$$iINSPIRE-00061476$$jORCID:0000-0003-0922-7669$$uBucharest, IFIN-HH
002655508 700__ $$aAlexopoulos, Theodoros$$iINSPIRE-00061543$$uNatl. Tech. U., Athens
002655508 700__ $$aAlhroob, Muhammad$$iINSPIRE-00210593$$jORCID:0000-0001-7569-7111$$uOklahoma U.
002655508 700__ $$aAli, Babar$$iINSPIRE-00518637$$jORCID:0000-0001-8653-5556$$uPrague, Tech. U.
002655508 700__ $$aAlimonti, Gianluca$$iINSPIRE-00004775$$jORCID:0000-0002-7128-9046$$uINFN, Milan
002655508 700__ $$aAlison, John$$iINSPIRE-00210617$$jORCID:0000-0003-0843-1641$$uChicago U., EFI
002655508 700__ $$aAlkire, Steven Patrick$$iINSPIRE-00400408$$uWashington U., Seattle
002655508 700__ $$aAllaire, Corentin$$iINSPIRE-00574032$$uOrsay, LAL
002655508 700__ $$aAllbrooke, Benedict$$iINSPIRE-00235773$$uSussex U.
002655508 700__ $$aAllen, Benjamin William$$iINSPIRE-00439268$$jORCID:0000-0002-1783-2685$$uOregon U.
002655508 700__ $$aAllport, Phillip$$iINSPIRE-00147775$$jORCID:0000-0001-7303-2570$$uBirmingham U.
002655508 700__ $$aAloisio, Alberto$$iINSPIRE-00210642$$jORCID:0000-0002-3883-6693$$uINFN, Naples$$uNaples U.
002655508 700__ $$aAlonso, Alejandro$$iINSPIRE-00210666$$jORCID:0000-0003-1259-0573$$uBohr Inst.
002655508 700__ $$aAlonso, Francisco$$iINSPIRE-00291080$$jORCID:0000-0001-9431-8156$$uLa Plata U.
002655508 700__ $$aAlpigiani, Cristiano$$iINSPIRE-00358374$$jORCID:0000-0002-7641-5814$$uWashington U., Seattle
002655508 700__ $$aAlshehri, Azzah Aziz$$iINSPIRE-00439334$$uGlasgow U.
002655508 700__ $$aAlstaty, Mahmoud$$iINSPIRE-00441244$$uMarseille, CPPM
002655508 700__ $$aAlvarez Gonzalez, Barbara$$iINSPIRE-00022061$$uCERN
002655508 700__ $$aAlvarez Piqueras, Damian$$iINSPIRE-00376986$$jORCID:0000-0002-5193-1492$$uValencia U., IFIC
002655508 700__ $$aAlviggi, Mariagrazia$$iINSPIRE-00210678$$jORCID:0000-0003-0026-982X$$uINFN, Naples$$uNaples U.
002655508 700__ $$aAmadio, Brian Thomas$$iINSPIRE-00399314$$uLBL, Berkeley
002655508 700__ $$aAmaral Coutinho, Yara$$iINSPIRE-00074762$$jORCID:0000-0002-1798-7230$$uRio de Janeiro Federal U.
002655508 700__ $$aAmbroz, Luca$$iINSPIRE-00574960$$jORCID:0000-0002-0987-6637$$uOxford U.
002655508 700__ $$aAmelung, Christoph$$iINSPIRE-00210696$$uBrandeis U.
002655508 700__ $$aAmidei, Dante Eric$$iINSPIRE-00061910$$uMichigan U.
002655508 700__ $$aAmor Dos Santos, Susana Patricia$$iINSPIRE-00291676$$jORCID:0000-0001-7566-6067$$uLIP, Lisbon$$uCoimbra U.
002655508 700__ $$aAmoroso, Simone$$iINSPIRE-00002752$$jORCID:0000-0001-5450-0447$$uDESY
002655508 700__ $$aAmrouche, Cherifa Sabrina$$iINSPIRE-00580932$$uGeneva U.
002655508 700__ $$aAnastopoulos, Christos$$iINSPIRE-00210733$$jORCID:0000-0003-1587-5830$$uSheffield U.
002655508 700__ $$aAncu, Lucian Stefan$$iINSPIRE-00025195$$uGeneva U.
002655508 700__ $$aAndari, Nansi$$iINSPIRE-00143085$$jORCID:0000-0002-4935-4753$$uIRFU, Saclay
002655508 700__ $$aAndeen, Timothy$$iINSPIRE-00005735$$jORCID:0000-0002-4413-871X$$uTexas U.
002655508 700__ $$aAnders, Christoph Falk$$iINSPIRE-00210745$$jORCID:0000-0001-6632-6327$$uHeidelberg U.
002655508 700__ $$aAnders, John Kenneth$$iINSPIRE-00399325$$jORCID:0000-0002-1846-0262$$uBern U., LHEP
002655508 700__ $$aAnderson, Kelby$$iINSPIRE-00210757$$uChicago U., EFI
002655508 700__ $$aAndreazza, Attilio$$iINSPIRE-00062128$$jORCID:0000-0001-5161-5759$$uINFN, Milan$$uMilan U.
002655508 700__ $$aAndrei, George Victor$$iINSPIRE-00210769$$uKirchhoff Inst. Phys.
002655508 700__ $$aAnelli, Christopher Ryan$$iINSPIRE-00353180$$uVictoria U.
002655508 700__ $$aAngelidakis, Stylianos$$iINSPIRE-00009427$$jORCID:0000-0002-8274-6118$$uClermont-Ferrand U.
002655508 700__ $$aAngelozzi, Ivan$$iINSPIRE-00366961$$uFOM, Amsterdam
002655508 700__ $$aAngerami, Aaron$$iINSPIRE-00210782$$jORCID:0000-0001-7834-8750$$uNevis Labs, Columbia U.
002655508 700__ $$aAnisenkov, Alexey$$iINSPIRE-00291854$$jORCID:0000-0002-7201-5936$$uNovosibirsk State U.$$uNovosibirsk, IYF
002655508 700__ $$aAnnovi, Alberto$$iINSPIRE-00041435$$jORCID:0000-0002-4649-4398$$uINFN, Pisa
002655508 700__ $$aAntel, Claire$$iINSPIRE-00517126$$jORCID:0000-0001-9683-0890$$uKirchhoff Inst. Phys.
002655508 700__ $$aAnthony, Matthew Thomas$$iINSPIRE-00577424$$jORCID:0000-0002-5270-0143$$uSheffield U.
002655508 700__ $$aAntonelli, Mario$$iINSPIRE-00210812$$jORCID:0000-0002-2293-5726$$uFrascati
002655508 700__ $$aAntrim, Daniel Joseph$$iINSPIRE-00524603$$jORCID:0000-0001-8084-7786$$uUC, Irvine
002655508 700__ $$aAnulli, Fabio$$iINSPIRE-00062462$$jORCID:0000-0003-2734-130X$$uINFN, Rome
002655508 700__ $$aAoki, Masato$$iINSPIRE-00001575$$jORCID:0000-0001-7498-0097$$uKEK, Tsukuba
002655508 700__ $$aAparisi Pozo, Javier Alberto$$iINSPIRE-00640204$$uValencia U., IFIC
002655508 700__ $$aAperio Bella, Ludovica$$iINSPIRE-00286141$$jORCID:0000-0003-3942-1702$$uCERN
002655508 700__ $$aArabidze, Giorgi$$iINSPIRE-00305586$$uMichigan State U.
002655508 700__ $$aAraque Espinosa, Juan Pedro$$iINSPIRE-00359999$$jORCID:0000-0003-2927-9378$$uLIP, Lisbon
002655508 700__ $$aAraujo Ferraz, Victor$$iINSPIRE-00389281$$jORCID:0000-0003-1177-7563$$uRio de Janeiro Federal U.
002655508 700__ $$aAraujo Pereira, Rodrigo$$iINSPIRE-00578151$$uRio de Janeiro Federal U.
002655508 700__ $$aArce, Ayana$$iINSPIRE-00005140$$jORCID:0000-0002-7255-0832$$uDuke U.
002655508 700__ $$aArdell, Rose Elisabeth$$iINSPIRE-00517130$$jORCID:0000-0002-1213-6736$$uRoyal Holloway, U. of London
002655508 700__ $$aArduh, Francisco Anuar$$iINSPIRE-00371726$$uLa Plata U.
002655508 700__ $$aArguin, Jean-Francois$$iINSPIRE-00049740$$jORCID:0000-0003-0229-3858$$uMontreal U.
002655508 700__ $$aArgyropoulos, Spyridon$$iINSPIRE-00335900$$jORCID:0000-0001-7748-1429$$uIowa U.
002655508 700__ $$aArmbruster, Aaron James$$iINSPIRE-00210861$$jORCID:0000-0002-9007-530X$$uCERN
002655508 700__ $$aArmitage, Lewis James$$iINSPIRE-00404370$$uQueen Mary, U. of London
002655508 700__ $$aArmstrong, Alexander III$$iINSPIRE-00586270$$jORCID:0000-0001-8505-4232$$uUC, Irvine
002655508 700__ $$aArnaez, Olivier$$iINSPIRE-00210873$$jORCID:0000-0002-6096-0893$$uToronto U.
002655508 700__ $$aArnold, Hannah$$iINSPIRE-00367502$$jORCID:0000-0003-3578-2228$$uFOM, Amsterdam
002655508 700__ $$aArratia, Miguel$$iINSPIRE-00360674$$jORCID:0000-0001-6877-3315$$uCambridge U.
002655508 700__ $$aArslan, Ozan$$iINSPIRE-00348465$$uBonn U.
002655508 700__ $$aArtamonov, Andrei$$iINSPIRE-00320346$$uMoscow, ITEP
002655508 700__ $$aArtoni, Giacomo$$iINSPIRE-00286089$$jORCID:0000-0002-3477-4499$$uOxford U.
002655508 700__ $$aArtz, Sebastian$$iINSPIRE-00414333$$uMainz U.
002655508 700__ $$aAsai, Shoji$$iINSPIRE-00210270$$uTokyo U., ICEPP
002655508 700__ $$aAsbah, Nedaa$$iINSPIRE-00339731$$uHarvard U., Phys. Dept.
002655508 700__ $$aAshkenazi, Adi$$iINSPIRE-00364725$$uTel Aviv U.
002655508 700__ $$aAsimakopoulou, Eleni Myrto$$iINSPIRE-00579660$$jORCID:0000-0003-2127-373X$$uUppsala U., Inst. Theor. Phys.
002655508 700__ $$aAsquith, Lily$$iINSPIRE-00180651$$jORCID:0000-0001-8035-7162$$uSussex U.
002655508 700__ $$aAssamagan, Ketevi$$iINSPIRE-00152949$$uBrookhaven
002655508 700__ $$aAstalos, Robert$$iINSPIRE-00332100$$jORCID:0000-0001-5095-605X$$uComenius U.
002655508 700__ $$aAtkin, Ryan Justin$$iINSPIRE-00574976$$jORCID:0000-0002-1972-1006$$uCape Town U.
002655508 700__ $$aAtkinson, Markus$$iINSPIRE-00289610$$uIllinois U., Urbana
002655508 700__ $$aAtlay, Naim Bora$$iINSPIRE-00345712$$uSiegen U.
002655508 700__ $$aAugsten, Kamil$$iINSPIRE-00013348$$jORCID:0000-0001-8324-0576$$uPrague, Tech. U.
002655508 700__ $$aAvolio, Giuseppe$$iINSPIRE-00210941$$jORCID:0000-0003-2664-3437$$uCERN
002655508 700__ $$aAvramidou, Rachel Maria$$iINSPIRE-00210953$$jORCID:0000-0002-1645-1290$$uHefei, CUST
002655508 700__ $$aAyoub, Mohamad Kassem$$iINSPIRE-00389471$$jORCID:0000-0001-5265-2674$$uBeijing, Inst. High Energy Phys.
002655508 700__ $$aAzuelos, Georges$$iINSPIRE-00063480$$jORCID:0000-0003-4241-022X$$uMontreal U.$$uTRIUMF
002655508 700__ $$aBaas, Alessandra$$iINSPIRE-00365509$$jORCID:0000-0002-2224-2305$$uKirchhoff Inst. Phys.
002655508 700__ $$aBaca, Matthew John$$iINSPIRE-00389380$$uBirmingham U.
002655508 700__ $$aBachacou, Henri$$iINSPIRE-00210989$$jORCID:0000-0002-2256-4515$$uIRFU, Saclay
002655508 700__ $$aBachas, Konstantinos$$iINSPIRE-00210990$$jORCID:0000-0002-9047-6517$$uINFN, Lecce$$uSalento U.
002655508 700__ $$aBackes, Moritz$$iINSPIRE-00211007$$jORCID:0000-0003-2409-9829$$uOxford U.
002655508 700__ $$aBagnaia, Paolo$$iINSPIRE-00063838$$jORCID:0000-0003-4578-2651$$uINFN, Rome$$uRome U.
002655508 700__ $$aBahmani, Marzieh$$iINSPIRE-00551811$$jORCID:0000-0003-4173-0926$$uCracow, INP
002655508 700__ $$aBaluch Bahrasemani, Sina$$iINSPIRE-00544674$$uSimon Fraser U.
002655508 700__ $$aBailey, Adam$$iINSPIRE-00481026$$jORCID:0000-0002-3301-2986$$uValencia U., IFIC
002655508 700__ $$aBaines, John$$iINSPIRE-00063905$$jORCID:0000-0003-0770-2702$$uRutherford
002655508 700__ $$aBajic, Milena$$iINSPIRE-00524612$$jORCID:0000-0002-3055-2549$$uBohr Inst.
002655508 700__ $$aBakalis, Christos$$iINSPIRE-00584527$$uNatl. Tech. U., Athens
002655508 700__ $$aBaker, Keith$$iINSPIRE-00063962$$uYale U.
002655508 700__ $$aBakker, Pepijn Johannes$$iINSPIRE-00567803$$uFOM, Amsterdam
002655508 700__ $$aBakshi Gupta, Debottam$$iINSPIRE-00551849$$uLouisiana Tech. U.
002655508 700__ $$aBaldin, Evgenii$$iINSPIRE-00057771$$jORCID:0000-0002-9854-975X$$uNovosibirsk State U.$$uNovosibirsk, IYF
002655508 700__ $$aBalek, Petr$$iINSPIRE-00295870$$jORCID:0000-0002-0942-1966$$uWeizmann Inst.
002655508 700__ $$aBalli, Fabrice$$iINSPIRE-00000243$$jORCID:0000-0003-0844-4207$$uIRFU, Saclay
002655508 700__ $$aBalunas, William Keaton$$iINSPIRE-00421104$$uPennsylvania U.
002655508 700__ $$aBalz, Johannes$$iINSPIRE-00583960$$uMainz U.
002655508 700__ $$aBanas, Elzbieta$$iINSPIRE-00211068$$uCracow, INP
002655508 700__ $$aBandyopadhyay, Anjishnu$$iINSPIRE-00524626$$jORCID:0000-0002-5256-839X$$uBonn U.
002655508 700__ $$aBanerjee, Swagato$$iINSPIRE-00064260$$jORCID:0000-0001-8852-2409$$uWisconsin U., Madison$$uLouisville U.
002655508 700__ $$aBannoura, Arwa$$iINSPIRE-00360042$$jORCID:0000-0002-7166-8118$$uWuppertal U.
002655508 700__ $$aBarak, Liron$$iINSPIRE-00229245$$jORCID:0000-0002-3436-2726$$uTel Aviv U.
002655508 700__ $$aBarbe, William Mickael$$iINSPIRE-00578787$$jORCID:0000-0003-1969-7226$$uClermont-Ferrand U.
002655508 700__ $$aBarberio, Elisabetta Luigia$$iINSPIRE-00064366$$jORCID:0000-0002-3111-0910$$uMelbourne U.
002655508 700__ $$aBarberis, Dario$$iINSPIRE-00064378$$jORCID:0000-0002-3938-4553$$uINFN, Genoa$$uGenoa U.
002655508 700__ $$aBarbero, Marlon$$iINSPIRE-00211139$$uMarseille, CPPM
002655508 700__ $$aBarillari, Teresa$$iINSPIRE-00064533$$uMunich, Max Planck Inst.
002655508 700__ $$aBarisits, Martin-Stefan$$iINSPIRE-00473067$$uCERN
002655508 700__ $$aBarkeloo, Jason Tylor Colt$$iINSPIRE-00542403$$uOregon U.
002655508 700__ $$aBarklow, Timothy$$iINSPIRE-00064576$$jORCID:0000-0002-7709-037X$$uSLAC
002655508 700__ $$aBarlow, Nick$$iINSPIRE-00042309$$uCambridge U.
002655508 700__ $$aBarnea, Rotem$$iINSPIRE-00573610$$uTechnion
002655508 700__ $$aBarnes, Sarah Louise$$iINSPIRE-00362038$$uShanghai Jiao Tong U.
002655508 700__ $$aBarnett, Bruce$$iINSPIRE-00211160$$jORCID:0000-0002-5361-2823$$uRutherford
002655508 700__ $$aBarnett, Michael$$iINSPIRE-00064676$$jORCID:0000-0002-7210-9887$$uLBL, Berkeley
002655508 700__ $$aBlenessy, Zuzana$$iINSPIRE-00265099$$jORCID:0000-0002-5107-3395$$uHefei, CUST
002655508 700__ $$aBaroncelli, Antonio$$iINSPIRE-00064709$$jORCID:0000-0001-7090-7474$$uINFN, Rome3
002655508 700__ $$aBarone, Gaetano$$iINSPIRE-00235799$$jORCID:0000-0001-5163-5936$$uBrandeis U.
002655508 700__ $$aBarr, Alan$$iINSPIRE-00064725$$jORCID:0000-0002-3533-3740$$uOxford U.
002655508 700__ $$aBarranco Navarro, Laura$$iINSPIRE-00441300$$jORCID:0000-0002-3380-8167$$uValencia U., IFIC
002655508 700__ $$aBarreiro, Fernando$$iINSPIRE-00064758$$jORCID:0000-0002-3021-0258$$uMadrid, Autonoma U.
002655508 700__ $$aBarreiro Guimaraes da Costa, Joao$$iINSPIRE-00087323$$jORCID:0000-0003-2387-0386$$uBeijing, Inst. High Energy Phys.
002655508 700__ $$aBartoldus, Rainer$$iINSPIRE-00064943$$jORCID:0000-0001-5317-9794$$uSLAC
002655508 700__ $$aBarton, Adam Edward$$iINSPIRE-00229256$$jORCID:0000-0001-9696-9497$$uLancaster U.
002655508 700__ $$aBartos, Pavol$$iINSPIRE-00304670$$jORCID:0000-0003-1419-3213$$uComenius U.
002655508 700__ $$aBasalaev, Artem$$iINSPIRE-00399337$$uSt. Petersburg, INP
002655508 700__ $$aBassalat, Ahmed$$iINSPIRE-00347533$$jORCID:0000-0002-0129-1423$$uOrsay, LAL
002655508 700__ $$aBates, Richard$$iINSPIRE-00065082$$jORCID:0000-0002-6923-5372$$uGlasgow U.
002655508 700__ $$aBatista, Santiago Juan$$iINSPIRE-00381632$$uToronto U.
002655508 700__ $$aBatlamous, Souad$$iINSPIRE-00571460$$uMohammed V U., Agdal
002655508 700__ $$aBatley, Richard$$iINSPIRE-00211190$$jORCID:0000-0001-7658-7766$$uCambridge U.
002655508 700__ $$aBattaglia, Marco$$iINSPIRE-00065121$$uUC, Santa Cruz
002655508 700__ $$aBauce, Matteo$$iINSPIRE-00243631$$jORCID:0000-0002-9148-4658$$uINFN, Rome$$uRome U.
002655508 700__ $$aBauer, Florian$$iINSPIRE-00657399$$jORCID:0000-0003-2258-2892$$uIRFU, Saclay
002655508 700__ $$aBauer, Kevin Thomas$$iINSPIRE-00569383$$uUC, Irvine
002655508 700__ $$aBawa, Harinder Singh$$iINSPIRE-00316070$$uSLAC$$uFresno State
002655508 700__ $$aBeacham, James Baker$$iINSPIRE-00344428$$jORCID:0000-0003-3623-3335$$uOhio State U.
002655508 700__ $$aBeau, Tristan$$iINSPIRE-00149690$$jORCID:0000-0002-2022-2140$$uParis U., VI-VII
002655508 700__ $$aBeauchemin, Pierre-Hugues$$iINSPIRE-00034698$$jORCID:0000-0003-4889-8748$$uTufts U.
002655508 700__ $$aBechtle, Philip$$iINSPIRE-00055190$$uBonn U.
002655508 700__ $$aBeck, Helge Christoph$$iINSPIRE-00560810$$uGottingen U., II. Phys. Inst.
002655508 700__ $$aBeck, Hans Peter$$iINSPIRE-00065459$$jORCID:0000-0001-7212-1096$$uBern U., LHEP$$uFribourg U.
002655508 700__ $$aBecker, Anne Kathrin$$iINSPIRE-00286180$$jORCID:0000-0002-6691-6498$$uFreiburg U.
002655508 700__ $$aBecker, Maurice$$iINSPIRE-00395743$$uMainz U.
002655508 700__ $$aBecot, Cyril$$iINSPIRE-00362269$$jORCID:0000-0003-0473-512X$$uDESY
002655508 700__ $$aBeddall, Ayda$$iINSPIRE-00211268$$uGaziantep U.
002655508 700__ $$aBeddall, Andrew$$iINSPIRE-00065527$$jORCID:0000-0002-8451-9672$$uIstanbul, Bahcesehir U.
002655508 700__ $$aBednyakov, Vadim$$iINSPIRE-00065561$$jORCID:0000-0003-4864-8909$$uDubna, JINR
002655508 700__ $$aBedognetti, Matteo$$iINSPIRE-00439426$$jORCID:0000-0003-1345-2770$$uFOM, Amsterdam
002655508 700__ $$aBee, Christopher$$iINSPIRE-00065575$$jORCID:0000-0001-6294-6561$$uSUNY, Stony Brook
002655508 700__ $$aBeermann, Thomas Alfons$$iINSPIRE-00346910$$uCERN
002655508 700__ $$aBegalli, Marcia$$iINSPIRE-00065602$$uRio de Janeiro Federal U.
002655508 700__ $$aBegel, Michael$$iINSPIRE-00065614$$jORCID:0000-0002-1634-4399$$uBrookhaven
002655508 700__ $$aBehera, Arabinda$$iINSPIRE-00538717$$uSUNY, Stony Brook
002655508 700__ $$aBehr, Katharina$$iINSPIRE-00348133$$jORCID:0000-0002-5501-4640$$uDESY
002655508 700__ $$aBell, Andrew Stuart$$iINSPIRE-00441191$$uUniversity Coll. London
002655508 700__ $$aBella, Gideon$$iINSPIRE-00211305$$jORCID:0000-0002-4009-0990$$uTel Aviv U.
002655508 700__ $$aBellagamba, Lorenzo$$iINSPIRE-00065777$$jORCID:0000-0001-7098-9393$$uINFN, Bologna
002655508 700__ $$aBellerive, Alain$$iINSPIRE-00065818$$jORCID:0000-0001-6775-0111$$uCarleton U.
002655508 700__ $$aBellomo, Massimiliano$$iINSPIRE-00211329$$uTechnion
002655508 700__ $$aBellos, Panagiotis$$iINSPIRE-00586679$$uAthens Natl. Capodistrian U.
002655508 700__ $$aBelotskiy, Konstantin$$iINSPIRE-00211335$$uMoscow Phys. Eng. Inst.
002655508 700__ $$aBelyaev, Nikita$$iINSPIRE-00421168$$jORCID:0000-0002-1131-7121$$uMoscow Phys. Eng. Inst.
002655508 700__ $$aBenary, Odette$$iINSPIRE-00211360$$uTel Aviv U.
002655508 700__ $$aBenchekroun, Driss$$iINSPIRE-00211372$$jORCID:0000-0001-5196-8327$$uCasablanca U.
002655508 700__ $$aBender, Michael$$iINSPIRE-00387486$$uMunich U.
002655508 700__ $$aBenekos, Nektarios$$iINSPIRE-00066029$$jORCID:0000-0001-7831-8762$$uNatl. Tech. U., Athens
002655508 700__ $$aBenhammou, Yan$$iINSPIRE-00211400$$jORCID:0000-0002-0392-1783$$uTel Aviv U.
002655508 700__ $$aBenhar Noccioli, Eleonora$$iINSPIRE-00286227$$uYale U.
002655508 700__ $$aBenitez, Jose$$iINSPIRE-00016190$$jORCID:0000-0002-2633-6712$$uIowa U.
002655508 700__ $$aBenjamin, Douglas$$iINSPIRE-00066086$$jORCID:0000-0001-9338-4581$$uDuke U.
002655508 700__ $$aBenoit, Mathieu$$iINSPIRE-00211411$$jORCID:0000-0002-8623-1699$$uGeneva U.
002655508 700__ $$aBensinger, James$$iINSPIRE-00066127$$uBrandeis U.
002655508 700__ $$aBentvelsen, Stan$$iINSPIRE-00066169$$uFOM, Amsterdam
002655508 700__ $$aBeresford, Lydia$$iINSPIRE-00389718$$jORCID:0000-0002-3080-1824$$uOxford U.
002655508 700__ $$aBeretta, Matteo$$iINSPIRE-00211424$$uFrascati
002655508 700__ $$aBerge, David$$iINSPIRE-00326772$$jORCID:0000-0002-2918-1824$$uDESY
002655508 700__ $$aBergeaas Kuutmann, Elin$$iINSPIRE-00305615$$jORCID:0000-0002-1253-8583$$uUppsala U., Inst. Theor. Phys.
002655508 700__ $$aBerger, Nicolas$$iINSPIRE-00066350$$jORCID:0000-0002-7963-9725$$uAnnecy, LAPP
002655508 700__ $$aBergsten, Laura Jean$$iINSPIRE-00565676$$jORCID:0000-0002-0398-2228$$uBrandeis U.
002655508 700__ $$aBeringer, Juerg$$iINSPIRE-00066414$$jORCID:0000-0002-9975-1781$$uLBL, Berkeley
002655508 700__ $$aBerlendis, Simon Paul$$iINSPIRE-00441396$$jORCID:0000-0003-1911-772X$$uArizona U.
002655508 700__ $$aBernard, Nathan Rogers$$iINSPIRE-00383935$$jORCID:0000-0002-4250-6267$$uMassachusetts U., Amherst
002655508 700__ $$aBernardi, Gregorio$$iINSPIRE-00066505$$jORCID:0000-0002-2837-2442$$uParis U., VI-VII
002655508 700__ $$aBernius, Catrin$$iINSPIRE-00211450$$jORCID:0000-0003-3433-1687$$uSLAC
002655508 700__ $$aBernlochner, Florian Urs$$iINSPIRE-00144634$$jORCID:0000-0001-8153-2719$$uBonn U.
002655508 700__ $$aBerry, Tracey$$iINSPIRE-00041406$$uRoyal Holloway, U. of London
002655508 700__ $$aBerta, Peter$$iINSPIRE-00349738$$jORCID:0000-0003-0780-0345$$uMainz U.
002655508 700__ $$aBertella, Claudia$$iINSPIRE-00235836$$jORCID:0000-0002-3160-147X$$uBeijing, Inst. High Energy Phys.
002655508 700__ $$aBertoli, Gabriele$$iINSPIRE-00370978$$uStockholm U.$$uStockholm U., OKC
002655508 700__ $$aBertram, Iain Alexander$$iINSPIRE-00066653$$jORCID:0000-0003-4073-4941$$uLancaster U.
002655508 700__ $$aBesjes, Geert-jan$$iINSPIRE-00286235$$jORCID:0000-0003-3113-2455$$uBohr Inst.
002655508 700__ $$aBessidskaia Bylund, Olga$$iINSPIRE-00348474$$uWuppertal U.
002655508 700__ $$aBessner, Martin Florian$$iINSPIRE-00368451$$jORCID:0000-0003-1776-0439$$uDESY
002655508 700__ $$aBesson, Nathalie$$iINSPIRE-00211485$$jORCID:0000-0001-9248-6252$$uIRFU, Saclay
002655508 700__ $$aBethani, Agni$$iINSPIRE-00202655$$jORCID:0000-0002-8150-7043$$uManchester U.
002655508 700__ $$aBethke, Siegfried$$iINSPIRE-00179262$$jORCID:0000-0003-0073-3821$$uMunich, Max Planck Inst.
002655508 700__ $$aBetti, Alessandra$$iINSPIRE-00564976$$jORCID:0000-0003-0839-9311$$uBonn U.
002655508 700__ $$aBevan, Adrian John$$iINSPIRE-00042361$$jORCID:0000-0002-4105-9629$$uQueen Mary, U. of London
002655508 700__ $$aBeyer, Julien-christopher$$iINSPIRE-00547588$$jORCID:0000-0002-2942-1330$$uMunich, Max Planck Inst.
002655508 700__ $$aBianchi, Riccardo-Maria$$iINSPIRE-00211497$$jORCID:0000-0001-7345-7798$$uPittsburgh U.
002655508 700__ $$aBiebel, Otmar$$iINSPIRE-00066953$$jORCID:0000-0002-8663-6856$$uMunich U.
002655508 700__ $$aBiedermann, Dustin$$iINSPIRE-00392746$$jORCID:0000-0003-4368-2630$$uHumboldt U., Berlin
002655508 700__ $$aBielski, Rafal$$iINSPIRE-00437899$$jORCID:0000-0002-2079-5344$$uCERN
002655508 700__ $$aBierwagen, Katharina$$iINSPIRE-00235864$$jORCID:0000-0002-0799-2626$$uMainz U.
002655508 700__ $$aBiesuz, Nicolo Vladi$$iINSPIRE-00441490$$jORCID:0000-0003-3004-0946$$uINFN, Pisa$$uPisa U.
002655508 700__ $$aBiglietti, Michela$$iINSPIRE-00211510$$jORCID:0000-0001-5442-1351$$uINFN, Rome3
002655508 700__ $$aBilloud, Thomas Remy Victor$$iINSPIRE-00512807$$jORCID:0000-0002-6280-3306$$uMontreal U.
002655508 700__ $$aBindi, Marcello$$iINSPIRE-00172094$$jORCID:0000-0001-6172-545X$$uGottingen U., II. Phys. Inst.
002655508 700__ $$aBingul, Ahmet$$iINSPIRE-00211539$$jORCID:0000-0002-2455-8039$$uGaziantep U.
002655508 700__ $$aBini, Cesare$$iINSPIRE-00211540$$jORCID:0000-0001-6674-7869$$uINFN, Rome$$uRome U.
002655508 700__ $$aBiondi, Silvia$$iINSPIRE-00407321$$jORCID:0000-0002-1492-6715$$uINFN, Bologna$$uBologna U.
002655508 700__ $$aBirman, Mattias$$iINSPIRE-00639184$$jORCID:0000-0002-3835-0968$$uWeizmann Inst.
002655508 700__ $$aBisanz, Tobias$$iINSPIRE-00470148$$uGottingen U., II. Phys. Inst.
002655508 700__ $$aBiswal, Jyoti Prakash$$iINSPIRE-00401043$$jORCID:0000-0001-8361-2309$$uTel Aviv U.
002655508 700__ $$aBittrich, Carsten$$iINSPIRE-00524633$$uDresden, Tech. U.
002655508 700__ $$aBjergaard, David Martin$$iINSPIRE-00002187$$jORCID:0000-0003-2106-3046$$uDuke U.
002655508 700__ $$aBlack, James$$iINSPIRE-00334293$$uSLAC
002655508 700__ $$aBlack, Kevin$$iINSPIRE-00175789$$jORCID:0000-0001-7320-5080$$uBoston U.
002655508 700__ $$aBlazek, Tomas$$iINSPIRE-00235878$$jORCID:0000-0002-2645-0283$$uComenius U.
002655508 700__ $$aBloch, Ingo$$iINSPIRE-00060307$$jORCID:0000-0002-6696-5169$$uDESY
002655508 700__ $$aBlocker, Craig$$iINSPIRE-00067509$$jORCID:0000-0001-6898-5633$$uBrandeis U.
002655508 700__ $$aBlue, Andrew$$iINSPIRE-00524643$$jORCID:0000-0002-7716-5626$$uGlasgow U.
002655508 700__ $$aBlumenschein, Ulrike$$iINSPIRE-00211570$$jORCID:0000-0002-6134-0303$$uQueen Mary, U. of London
002655508 700__ $$aBlunier, Sylvain$$iINSPIRE-00412983$$uChile U., Catolica
002655508 700__ $$aBobbink, Gerjan$$iINSPIRE-00211581$$jORCID:0000-0001-8462-351X$$uFOM, Amsterdam
002655508 700__ $$aBobrovnikov, Victor$$iINSPIRE-00229343$$jORCID:0000-0002-2003-0261$$uNovosibirsk State U.$$uNovosibirsk, IYF
002655508 700__ $$aBocchetta, Simona Serena$$iINSPIRE-00235887$$uLund U.
002655508 700__ $$aBocci, Andrea$$iINSPIRE-00048999$$jORCID:0000-0001-6700-6077$$uDuke U.
002655508 700__ $$aBoerner, Daniela$$iINSPIRE-00439393$$jORCID:0000-0003-4087-1575$$uWuppertal U.
002655508 700__ $$aBogavac, Danijela$$iINSPIRE-00407355$$jORCID:0000-0003-2138-9062$$uMunich U.
002655508 700__ $$aBogdanchikov, Alexander$$iINSPIRE-00229367$$jORCID:0000-0002-8635-9342$$uNovosibirsk State U.$$uNovosibirsk, IYF
002655508 700__ $$aBohm, Christian$$iINSPIRE-00324763$$uStockholm U.
002655508 700__ $$aBoisvert, Veronique$$iINSPIRE-00067915$$jORCID:0000-0002-7736-0173$$uRoyal Holloway, U. of London
002655508 700__ $$aBokan, Petar$$iINSPIRE-00451520$$jORCID:0000-0002-2668-889X$$uUppsala U., Inst. Theor. Phys.
002655508 700__ $$aBold, Tomasz$$iINSPIRE-00172488$$jORCID:0000-0002-2432-411X$$uAGH-UST, Cracow
002655508 700__ $$aBoldyrev, Alexey$$iINSPIRE-00340190$$jORCID:0000-0002-7872-6819$$uLomonosov Moscow State U.
002655508 700__ $$aBolz, Arthur Eugen$$iINSPIRE-00535007$$jORCID:0000-0002-4033-9223$$uHeidelberg U.
002655508 700__ $$aBomben, Marco$$iINSPIRE-00052711$$jORCID:0000-0002-9807-861X$$uParis U., VI-VII
002655508 700__ $$aBona, Marcella$$iINSPIRE-00049930$$jORCID:0000-0002-9660-580X$$uQueen Mary, U. of London
002655508 700__ $$aBonilla, Johan Sebastian$$iINSPIRE-00551830$$jORCID:0000-0002-6982-6121$$uOregon U.
002655508 700__ $$aBoonekamp, Maarten$$iINSPIRE-00211647$$uIRFU, Saclay
002655508 700__ $$aBorisov, Anatoly$$iINSPIRE-00226538$$uSerpukhov, IHEP
002655508 700__ $$aBorissov, Guennadi$$iINSPIRE-00068300$$jORCID:0000-0002-4226-9521$$uLancaster U.
002655508 700__ $$aBortfeldt, Jonathan$$iINSPIRE-00295897$$jORCID:0000-0002-0777-985X$$uCERN
002655508 700__ $$aBortoletto, Daniela$$iINSPIRE-00068366$$jORCID:0000-0002-1287-4712$$uOxford U.
002655508 700__ $$aBortolotto, Valerio$$iINSPIRE-00235896$$uINFN, Rome2$$uRome U., Tor Vergata
002655508 700__ $$aBoscherini, Davide$$iINSPIRE-00172014$$jORCID:0000-0001-9207-6413$$uINFN, Bologna
002655508 700__ $$aBosman, Martine$$iINSPIRE-00227227$$jORCID:0000-0002-7290-643X$$uBarcelona, IFAE
002655508 700__ $$aBossio Sola, Jonathan David$$iINSPIRE-00441594$$jORCID:0000-0002-7134-8077$$uBuenos Aires U.
002655508 700__ $$aBouaouda, Khalil$$iINSPIRE-00584544$$uCasablanca U.
002655508 700__ $$aBoudreau, Joseph$$iINSPIRE-00068562$$uPittsburgh U.
002655508 700__ $$aBouhova-Thacker, Evelina Vassileva$$iINSPIRE-00211684$$jORCID:0000-0002-5103-1558$$uLancaster U.
002655508 700__ $$aBoumediene, Djamel Eddine$$iINSPIRE-00050723$$uClermont-Ferrand U.
002655508 700__ $$aBourdarios, Claire$$iINSPIRE-00068610$$jORCID:0000-0002-2634-4958$$uOrsay, LAL
002655508 700__ $$aBoutle, Sarah Kate$$iINSPIRE-00174075$$jORCID:0000-0002-8732-2963$$uGlasgow U.
002655508 700__ $$aBoveia, Antonio$$iINSPIRE-00041392$$jORCID:0000-0002-6647-6699$$uOhio State U.
002655508 700__ $$aBoyd, James$$iINSPIRE-00226553$$jORCID:0000-0001-7360-0726$$uCERN
002655508 700__ $$aBoye, Diallo$$iINSPIRE-00641083$$uJohannesburg U.
002655508 700__ $$aBoyko, Igor$$iINSPIRE-00211696$$jORCID:0000-0002-3355-4662$$uDubna, JINR
002655508 700__ $$aBozson, Adam James$$iINSPIRE-00550290$$jORCID:0000-0003-2354-4812$$uRoyal Holloway, U. of London
002655508 700__ $$aBracinik, Juraj$$iINSPIRE-00068874$$jORCID:0000-0001-5762-3477$$uBirmingham U.
002655508 700__ $$aBrahimi, Nihal$$iINSPIRE-00578795$$jORCID:0000-0003-0992-3509$$uMarseille, CPPM
002655508 700__ $$aBrandt, Andrew$$iINSPIRE-00300274$$uTexas U., Arlington
002655508 700__ $$aBrandt, Gerhard$$iINSPIRE-00032742$$uWuppertal U.
002655508 700__ $$aBrandt, Oleg$$iINSPIRE-00184109$$jORCID:0000-0001-5219-1417$$uKirchhoff Inst. Phys.
002655508 700__ $$aBraren, Frued$$iINSPIRE-00567085$$uDESY
002655508 700__ $$aBratzler, Uwe$$iINSPIRE-00211726$$uTokyo Metropolitan U.
002655508 700__ $$aBrau, Benjamin$$iINSPIRE-00069043$$jORCID:0000-0001-9726-4376$$uMassachusetts U., Amherst
002655508 700__ $$aBrau, James$$iINSPIRE-00069055$$jORCID:0000-0003-1292-9725$$uOregon U.
002655508 700__ $$aBreaden Madden, William Dmitri$$iINSPIRE-00438010$$uGlasgow U.
002655508 700__ $$aBrendlinger, Kurt$$iINSPIRE-00338116$$jORCID:0000-0002-9096-780X$$uDESY
002655508 700__ $$aBrennan, Amelia Jean$$iINSPIRE-00345743$$jORCID:0000-0002-8250-3351$$uMelbourne U.
002655508 700__ $$aBrenner, Lydia$$iINSPIRE-00386479$$jORCID:0000-0001-5350-7081$$uDESY
002655508 700__ $$aBrenner, Richard$$iINSPIRE-00211740$$uUppsala U., Inst. Theor. Phys.
002655508 700__ $$aBressler, Shikma$$iINSPIRE-00211751$$jORCID:0000-0003-4194-2734$$uWeizmann Inst.
002655508 700__ $$aBrickwedde, Bernard$$iINSPIRE-00580228$$jORCID:0000-0003-3518-3057$$uMainz U.
002655508 700__ $$aBriglin, Daniel Lawrence$$iINSPIRE-00536605$$jORCID:0000-0002-3048-8153$$uBirmingham U.
002655508 700__ $$aBritton, Dave$$iINSPIRE-00069310$$jORCID:0000-0001-9998-4342$$uGlasgow U.
002655508 700__ $$aBritzger, Daniel Andreas$$iINSPIRE-00306448$$jORCID:0000-0002-9246-7366$$uHeidelberg U.
002655508 700__ $$aBrock, Ian$$iINSPIRE-00069330$$jORCID:0000-0003-0903-8948$$uBonn U.
002655508 700__ $$aBrock, Raymond$$iINSPIRE-00069341$$uMichigan State U.
002655508 700__ $$aBrooijmans, Gustaaf$$iINSPIRE-00069444$$jORCID:0000-0002-3354-1810$$uNevis Labs, Columbia U.
002655508 700__ $$aBrooks, Timothy$$iINSPIRE-00235925$$jORCID:0000-0002-4659-7960$$uRoyal Holloway, U. of London
002655508 700__ $$aBrooks, William$$iINSPIRE-00069460$$jORCID:0000-0001-6161-3570$$uSanta Maria U., Valparaiso
002655508 700__ $$aBrost, Elizabeth$$iINSPIRE-00345015$$jORCID:0000-0002-6800-9808$$uNorthern Illinois U.
002655508 700__ $$aBroughton, James$$iINSPIRE-00445214$$jORCID:0000-0002-0797-5578$$uBirmingham U.
002655508 700__ $$aBruckman de Renstrom, Pawel$$iINSPIRE-00180299$$uCracow, INP
002655508 700__ $$aBruncko, Dusan$$iINSPIRE-00179454$$jORCID:0000-0003-0208-2372$$uKosice, IEF
002655508 700__ $$aBruni, Alessia$$iINSPIRE-00069652$$jORCID:0000-0003-4806-0718$$uINFN, Bologna
002655508 700__ $$aBruni, Graziano$$iINSPIRE-00172026$$jORCID:0000-0001-5667-7748$$uINFN, Bologna
002655508 700__ $$aBruni, Lucrezia Stella$$iINSPIRE-00512810$$jORCID:0000-0001-7616-0236$$uFOM, Amsterdam
002655508 700__ $$aBruno, Salvatore$$iINSPIRE-00563514$$jORCID:0000-0001-5422-8228$$uINFN, Rome2$$uRome U., Tor Vergata
002655508 700__ $$aBrunt, Benjamin Hylton$$iINSPIRE-00439507$$jORCID:0000-0002-9769-4154$$uCambridge U.
002655508 700__ $$aBruschi, Marco$$iINSPIRE-00211789$$jORCID:0000-0002-4319-4023$$uINFN, Bologna
002655508 700__ $$aBruscino, Nello$$iINSPIRE-00405244$$jORCID:0000-0002-6168-689X$$uPittsburgh U.
002655508 700__ $$aBryant, Patrick$$iINSPIRE-00438028$$uChicago U., EFI
002655508 700__ $$aBryngemark, Lene$$iINSPIRE-00329497$$jORCID:0000-0002-8420-3408$$uDESY
002655508 700__ $$aBuanes, Trygve$$iINSPIRE-00229479$$uBergen U.
002655508 700__ $$aBuat, Quentin$$iINSPIRE-00235948$$jORCID:0000-0001-7318-5251$$uCERN
002655508 700__ $$aBuchholz, Peter$$iINSPIRE-00069835$$jORCID:0000-0002-4049-0134$$uSiegen U.
002655508 700__ $$aBuckley, Andrew$$iINSPIRE-00211807$$jORCID:0000-0001-8355-9237$$uGlasgow U.
002655508 700__ $$aBudagov, Ioulian$$iINSPIRE-00211819$$uDubna, JINR
002655508 700__ $$aBugge, Magnar Kopangen$$iINSPIRE-00298334$$jORCID:0000-0002-8650-8125$$uOslo U.
002655508 700__ $$aBuehrer, Felix$$iINSPIRE-00356527$$jORCID:0000-0002-9274-5004$$uFreiburg U.
002655508 700__ $$aBulekov, Oleg$$iINSPIRE-00211832$$uMoscow Phys. Eng. Inst.
002655508 700__ $$aBullock, Daniel$$iINSPIRE-00399438$$uTexas U., Arlington
002655508 700__ $$aBurch, Tyler James$$iINSPIRE-00533027$$jORCID:0000-0002-3234-9042$$uNorthern Illinois U.
002655508 700__ $$aBurdin, Sergey$$iINSPIRE-00022855$$jORCID:0000-0003-4831-4132$$uLiverpool U.
002655508 700__ $$aBurgard, Carsten Daniel$$iINSPIRE-00423318$$uFOM, Amsterdam
002655508 700__ $$aBurger, Angela Maria$$iINSPIRE-00530530$$jORCID:0000-0003-0685-4122$$uAnnecy, LAPP
002655508 700__ $$aBurghgrave, Blake$$iINSPIRE-00354209$$jORCID:0000-0001-5686-0948$$uNorthern Illinois U.
002655508 700__ $$aBurka, Klaudia$$iINSPIRE-00438133$$jORCID:0000-0003-4819-9226$$uCracow, INP
002655508 700__ $$aBurke, Stephen$$iINSPIRE-00211870$$jORCID:0000-0002-1962-8493$$uRutherford
002655508 700__ $$aBurmeister, Ingo$$iINSPIRE-00348374$$uDortmund U.
002655508 700__ $$aBurr, Jonathan Thomas$$iINSPIRE-00512821$$jORCID:0000-0001-6726-6362$$uOxford U.
002655508 700__ $$aBuescher, Daniel$$iINSPIRE-00368463$$uFreiburg U.
002655508 700__ $$aBuescher, Volker$$iINSPIRE-00070225$$jORCID:0000-0001-9196-0629$$uMainz U.
002655508 700__ $$aBuschmann, Eric$$iINSPIRE-00571471$$uGottingen U., II. Phys. Inst.
002655508 700__ $$aBussey, Peter$$iINSPIRE-00070265$$jORCID:0000-0003-0988-7878$$uGlasgow U.
002655508 700__ $$aButler, John$$iINSPIRE-00179876$$jORCID:0000-0003-2834-836X$$uBoston U.
002655508 700__ $$aButtar, Craig$$iINSPIRE-00160192$$jORCID:0000-0003-0188-6491$$uGlasgow U.
002655508 700__ $$aButterworth, Jonathan$$iINSPIRE-00070318$$jORCID:0000-0002-5905-5394$$uUniversity Coll. London
002655508 700__ $$aButti, Pierfrancesco$$iINSPIRE-00358725$$uCERN
002655508 700__ $$aButtinger, William$$iINSPIRE-00229496$$jORCID:0000-0002-5116-1897$$uCERN
002655508 700__ $$aBuzatu, Adrian$$iINSPIRE-00025104$$jORCID:0000-0001-5519-9879$$uTaiwan, Inst. Phys.
002655508 700__ $$aBuzykaev, Aleksey$$iINSPIRE-00003784$$uNovosibirsk State U.$$uNovosibirsk, IYF
002655508 700__ $$aCabras, Grazia$$iINSPIRE-00577439$$jORCID:0000-0002-8467-8235$$uINFN, Bologna$$uBologna U.
002655508 700__ $$aCabrera Urban, Susana$$iINSPIRE-00211900$$jORCID:0000-0001-7640-7913$$uValencia U., IFIC
002655508 700__ $$aCaforio, Davide$$iINSPIRE-00211911$$jORCID:0000-0001-7808-8442$$uPrague, Tech. U.
002655508 700__ $$aCai, Huacheng$$iINSPIRE-00568379$$jORCID:0000-0001-7575-3603$$uIllinois U., Urbana
002655508 700__ $$aCairo, Valentina Maria$$iINSPIRE-00403090$$jORCID:0000-0002-0758-7575$$uSUNY, Albany
002655508 700__ $$aCakir, Orhan$$iINSPIRE-00211923$$jORCID:0000-0002-9016-138X$$uAnkara U.
002655508 700__ $$aCalace, Noemi$$iINSPIRE-00408949$$jORCID:0000-0002-1494-9538$$uGeneva U.
002655508 700__ $$aCalafiura, Paolo$$iINSPIRE-00070566$$jORCID:0000-0002-1692-1678$$uLBL, Berkeley
002655508 700__ $$aCalandri, Alessandro$$iINSPIRE-00366978$$uMarseille, CPPM
002655508 700__ $$aCalderini, Giovanni$$iINSPIRE-00070597$$jORCID:0000-0002-9495-9145$$uParis U., VI-VII
002655508 700__ $$aCalfayan, Philippe$$iINSPIRE-00032964$$jORCID:0000-0003-1600-464X$$uIndiana U.
002655508 700__ $$aCallea, Giuseppe$$iINSPIRE-00514504$$jORCID:0000-0001-5969-3786$$uINFN, Cosenza$$uCalabria U.
002655508 700__ $$aCaloba, Luiz$$iINSPIRE-00211947$$uRio de Janeiro Federal U.
002655508 700__ $$aCalvente Lopez, Sergio$$iINSPIRE-00511707$$jORCID:0000-0002-7668-5275$$uMadrid, Autonoma U.
002655508 700__ $$aCalvet, David$$iINSPIRE-00070696$$jORCID:0000-0002-9953-5333$$uClermont-Ferrand U.
002655508 700__ $$aCalvet, Samuel$$iINSPIRE-00019519$$jORCID:0000-0002-2531-3463$$uClermont-Ferrand U.
002655508 700__ $$aCalvet, Thomas Philippe$$iINSPIRE-00438295$$jORCID:0000-0002-3342-3566$$uSUNY, Stony Brook
002655508 700__ $$aCalvetti, Milene$$iINSPIRE-00575709$$jORCID:0000-0003-0125-2165$$uINFN, Pisa$$uPisa U.
002655508 700__ $$aCamacho Toro, Reina$$iINSPIRE-00235957$$jORCID:0000-0002-9192-8028$$uParis U., VI-VII
002655508 700__ $$aCamarda, Stefano$$iINSPIRE-00012655$$jORCID:0000-0003-0479-7689$$uCERN
002655508 700__ $$aCamarri, Paolo$$iINSPIRE-00226571$$jORCID:0000-0002-5732-5645$$uINFN, Rome2$$uRome U., Tor Vergata
002655508 700__ $$aCameron, David$$iINSPIRE-00226583$$jORCID:0000-0001-6097-2256$$uOslo U.
002655508 700__ $$aCaminal Armadans, Roger$$iINSPIRE-00337611$$jORCID:0000-0001-9847-8309$$uMassachusetts U., Amherst
002655508 700__ $$aCamincher, Clement$$iINSPIRE-00438457$$jORCID:0000-0001-5929-1357$$uCERN
002655508 700__ $$aCampana, Simone$$iINSPIRE-00211959$$uCERN
002655508 700__ $$aCampanelli, Mario$$iINSPIRE-00070797$$jORCID:0000-0001-6746-3374$$uUniversity Coll. London
002655508 700__ $$aCamplani, Alessandra$$iINSPIRE-00452211$$jORCID:0000-0002-6386-9788$$uBohr Inst.
002655508 700__ $$aCampoverde, Angel$$iINSPIRE-00349667$$jORCID:0000-0003-1968-1216$$uSiegen U.
002655508 700__ $$aCanale, Vincenzo$$iINSPIRE-00211960$$jORCID:0000-0003-2303-9306$$uINFN, Naples$$uNaples U.
002655508 700__ $$aCano Bret, Marc$$iINSPIRE-00361241$$jORCID:0000-0002-8880-434X$$uShanghai Jiao Tong U.
002655508 700__ $$aCantero, Josu$$iINSPIRE-00211972$$jORCID:0000-0001-8449-1019$$uOklahoma State U.
002655508 700__ $$aCao, Tingting$$iINSPIRE-00334314$$jORCID:0000-0001-6784-0694$$uTel Aviv U.
002655508 700__ $$aCao, Yumeng$$iINSPIRE-00571488$$uIllinois U., Urbana
002655508 700__ $$aCapeans Garrido, Maria Del Mar$$iINSPIRE-00083814$$jORCID:0000-0001-7727-9175$$uCERN
002655508 700__ $$aCaprini, Irinel$$iINSPIRE-00070986$$jORCID:0000-0003-3343-3200$$uBucharest, IFIN-HH
002655508 700__ $$aCaprini, Mihai$$iINSPIRE-00211990$$jORCID:0000-0002-6806-6730$$uBucharest, IFIN-HH
002655508 700__ $$aCapua, Marcella$$iINSPIRE-00053925$$jORCID:0000-0002-2443-6525$$uINFN, Cosenza$$uCalabria U.
002655508 700__ $$aCarbone, Ryne Michael$$iINSPIRE-00424300$$jORCID:0000-0002-8462-5424$$uNevis Labs, Columbia U.
002655508 700__ $$aCardarelli, Roberto$$iINSPIRE-00212037$$jORCID:0000-0003-4541-4189$$uINFN, Rome2
002655508 700__ $$aCardillo, Fabio$$iINSPIRE-00407956$$jORCID:0000-0002-4478-3524$$uSheffield U.
002655508 700__ $$aCarli, Ina$$iINSPIRE-00235989$$jORCID:0000-0002-0411-1141$$uCharles U.
002655508 700__ $$aCarli, Tancredi$$iINSPIRE-00212045$$uCERN
002655508 700__ $$aCarlino, Gianpaolo$$iINSPIRE-00212057$$jORCID:0000-0002-3924-0445$$uINFN, Naples
002655508 700__ $$aCarlson, Benjamin Taylor$$iINSPIRE-00340092$$jORCID:0000-0002-7550-7821$$uPittsburgh U.
002655508 700__ $$aCarminati, Leonardo$$iINSPIRE-00212069$$jORCID:0000-0003-4535-2926$$uINFN, Milan$$uMilan U.
002655508 700__ $$aCarney, Rebecca$$iINSPIRE-00524651$$jORCID:0000-0001-5659-4440$$uStockholm U.$$uStockholm U., OKC
002655508 700__ $$aCaron, Sascha$$iINSPIRE-00057327$$jORCID:0000-0003-2941-2829$$uNijmegen U.
002655508 700__ $$aCarquin, Edson$$iINSPIRE-00023484$$jORCID:0000-0002-7863-1166$$uSanta Maria U., Valparaiso
002655508 700__ $$aCarra, Sonia$$iINSPIRE-00543668$$jORCID:0000-0001-8650-942X$$uINFN, Milan$$uMilan U.
002655508 700__ $$aCarrillo Montoya, German David$$iINSPIRE-00212072$$uCERN
002655508 700__ $$aCasadei, Diego$$iINSPIRE-00212084$$jORCID:0000-0002-3343-3529$$uJohannesburg U.
002655508 700__ $$aCasado, Maria Pilar$$iINSPIRE-00071410$$jORCID:0000-0002-0394-5646$$uBarcelona, IFAE$$uBarcelona, Autonoma U.
002655508 700__ $$aCasha, Albert Francis$$iINSPIRE-00567365$$uToronto U.
002655508 700__ $$aCasper, David William$$iINSPIRE-00071474$$jORCID:0000-0002-7618-1683$$uUC, Irvine
002655508 700__ $$aCastelijn, Remco$$iINSPIRE-00443025$$uFOM, Amsterdam
002655508 700__ $$aCastillo, Florencia Luciana$$iINSPIRE-00584559$$uValencia U., IFIC
002655508 700__ $$aCastillo Gimenez, Victoria$$iINSPIRE-00212120$$jORCID:0000-0002-8245-1790$$uValencia U., IFIC
002655508 700__ $$aCastro, Nuno Filipe$$iINSPIRE-00036257$$jORCID:0000-0001-8491-4376$$uLIP, Lisbon$$uMinho U.
002655508 700__ $$aCatinaccio, Andrea$$iINSPIRE-00212343$$jORCID:0000-0001-8774-8887$$uCERN
002655508 700__ $$aCatmore, James$$iINSPIRE-00212355$$uOslo U.
002655508 700__ $$aCattai, Ariella$$iINSPIRE-00320450$$uCERN
002655508 700__ $$aCaudron, Julien$$iINSPIRE-00308115$$jORCID:0000-0002-3530-6531$$uBonn U.
002655508 700__ $$aCavaliere, Viviana$$iINSPIRE-00010976$$jORCID:0000-0002-4297-8539$$uBrookhaven
002655508 700__ $$aCavallaro, Emanuele$$iINSPIRE-00451731$$jORCID:0000-0002-0570-2162$$uBarcelona, IFAE
002655508 700__ $$aCavalli, Donatella$$iINSPIRE-00212386$$jORCID:0000-0001-8465-0980$$uINFN, Milan
002655508 700__ $$aCavalli-Sforza, Matteo$$iINSPIRE-00071735$$jORCID:0000-0002-3291-3555$$uBarcelona, IFAE
002655508 700__ $$aCavasinni, Vincenzo$$iINSPIRE-00212398$$jORCID:0000-0001-6203-9347$$uINFN, Pisa$$uPisa U.
002655508 700__ $$aCelebi, Emre$$iINSPIRE-00406045$$uIstanbul Bilgi U.
002655508 700__ $$aCeradini, Filippo$$iINSPIRE-00071916$$jORCID:0000-0003-1153-6778$$uINFN, Rome3$$uRome III U.
002655508 700__ $$aCerda Alberich, Leonor$$iINSPIRE-00431162$$jORCID:0000-0002-5567-4278$$uValencia U., IFIC
002655508 700__ $$aSantiago Cerqueira, Augusto$$iINSPIRE-00212405$$uJuiz de Fora U.
002655508 700__ $$aCerri, Alessandro$$iINSPIRE-00050967$$jORCID:0000-0002-1904-6661$$uSussex U.
002655508 700__ $$aCerrito, Lucio$$iINSPIRE-00050901$$jORCID:0000-0002-8077-7850$$uINFN, Rome2$$uRome U., Tor Vergata
002655508 700__ $$aCerutti, Fabio$$iINSPIRE-00212418$$jORCID:0000-0001-9669-9642$$uLBL, Berkeley
002655508 700__ $$aCervelli, Alberto$$iINSPIRE-00025073$$jORCID:0000-0002-0518-1459$$uINFN, Bologna$$uBologna U.
002655508 700__ $$aCetin, Serkant Ali$$iINSPIRE-00186619$$jORCID:0000-0001-5050-8441$$uIstanbul Bilgi U.
002655508 700__ $$aChafaq, Aziz$$iINSPIRE-00212424$$uCasablanca U.
002655508 700__ $$aChakraborty, Dhiman$$iINSPIRE-00071985$$jORCID:0000-0002-9865-4146$$uNorthern Illinois U.
002655508 700__ $$aChan, Stephen Kam-wah$$iINSPIRE-00445289$$uHarvard U., Phys. Dept.
002655508 700__ $$aChan, Wing Sheung$$iINSPIRE-00534577$$jORCID:0000-0003-2150-1296$$uFOM, Amsterdam
002655508 700__ $$aChan, Yat Long$$iINSPIRE-00436344$$uHong Kong, Chinese U.
002655508 700__ $$aChapman, John Derek$$iINSPIRE-00029402$$jORCID:0000-0002-2926-8962$$uCambridge U.
002655508 700__ $$aChargeishvili, Bakar$$iINSPIRE-00641098$$jORCID:0000-0002-5376-2397$$uTbilisi State U.
002655508 700__ $$aCharlton, Dave$$iINSPIRE-00072301$$jORCID:0000-0003-0211-2041$$uBirmingham U.
002655508 700__ $$aChau, Chav Chhiv$$iINSPIRE-00362051$$jORCID:0000-0002-8049-771X$$uCarleton U.
002655508 700__ $$aChavez Barajas, Carlos Alberto$$iINSPIRE-00235990$$uSussex U.
002655508 700__ $$aChe, Siinn$$iINSPIRE-00425189$$jORCID:0000-0003-2709-7546$$uOhio State U.
002655508 700__ $$aChegwidden, Andrew$$iINSPIRE-00358737$$uMichigan State U.
002655508 700__ $$aChekanov, Sergei$$iINSPIRE-00072460$$jORCID:0000-0001-7314-7247$$uArgonne
002655508 700__ $$aChekulaev, Sergey$$iINSPIRE-00212450$$uTRIUMF
002655508 700__ $$aChelkov, Gueorgui$$iINSPIRE-00212473$$jORCID:0000-0002-3468-9761$$uDubna, JINR$$uTomsk State U.$$uMoscow, MIPT
002655508 700__ $$aChelstowska, Magda Anna$$iINSPIRE-00236000$$jORCID:0000-0003-1030-2099$$uCERN
002655508 700__ $$aChen, Cheng$$iINSPIRE-00465266$$uHefei, CUST
002655508 700__ $$aChen, Chunhui$$iINSPIRE-00058105$$jORCID:0000-0003-1589-9955$$uIowa State U.
002655508 700__ $$aChen, Hucheng$$iINSPIRE-00304146$$jORCID:0000-0002-9936-0115$$uBrookhaven
002655508 700__ $$aChen, Jing$$iINSPIRE-00551857$$jORCID:0000-0002-2554-2725$$uHefei, CUST
002655508 700__ $$aChen, Jue$$iINSPIRE-00573342$$jORCID:0000-0001-7293-6420$$uNevis Labs, Columbia U.
002655508 700__ $$aChen, Shion$$iINSPIRE-00417808$$jORCID:0000-0001-7987-9764$$uPennsylvania U.
002655508 700__ $$aChen, Shenjian$$iINSPIRE-00072626$$jORCID:0000-0003-0447-5348$$uNanjing U.
002655508 700__ $$aChen, Xin$$iINSPIRE-00145153$$uTsinghua U., Beijing$$uCICQM, Beijing
002655508 700__ $$aChen, Ye$$iINSPIRE-00377001$$jORCID:0000-0002-9218-3152$$uKobe U.
002655508 700__ $$aChen, Yu-heng$$iINSPIRE-00574040$$jORCID:0000-0002-2720-1115$$uDESY
002655508 700__ $$aCheng, Hok Chuen$$iINSPIRE-00357007$$jORCID:0000-0002-8912-4389$$uMichigan U.
002655508 700__ $$aCheng, Huajie$$iINSPIRE-00438626$$jORCID:0000-0001-6456-7178$$uBeijing, GUCAS
002655508 700__ $$aCheplakov, Alexander$$iINSPIRE-00001054$$jORCID:0000-0002-0967-2351$$uDubna, JINR
002655508 700__ $$aCheremushkina, Evgenia$$iINSPIRE-00371738$$uSerpukhov, IHEP
002655508 700__ $$aCherkaoui El Moursli, Rajaa$$iINSPIRE-00212497$$jORCID:0000-0002-5842-2818$$uMohammed V U., Agdal
002655508 700__ $$aCheu, Elliott$$iINSPIRE-00072813$$jORCID:0000-0002-2562-9724$$uArizona U.
002655508 700__ $$aCheung, Kingman$$iINSPIRE-00072840$$jORCID:0000-0003-2176-4053$$uTaiwan, Natl. Tsing Hua U.
002655508 700__ $$aChevalier, Laurent$$iINSPIRE-00212532$$jORCID:0000-0003-3762-7264$$uIRFU, Saclay
002655508 700__ $$aChiarella, Vitaliano$$iINSPIRE-00332290$$jORCID:0000-0002-4210-2924$$uFrascati
002655508 700__ $$aChiarelli, Giorgio$$iINSPIRE-00072892$$jORCID:0000-0001-9851-4816$$uINFN, Pisa
002655508 700__ $$aChiodini, Gabriele$$iINSPIRE-00212573$$jORCID:0000-0002-2458-9513$$uINFN, Lecce
002655508 700__ $$aChisholm, Andrew$$iINSPIRE-00236049$$jORCID:0000-0001-9214-8528$$uCERN
002655508 700__ $$aChitan, Adrian$$iINSPIRE-00236054$$uBucharest, IFIN-HH
002655508 700__ $$aChiu, I-huan$$iINSPIRE-00575711$$jORCID:0000-0003-4924-0278$$uTokyo U., ICEPP
002655508 700__ $$aChiu, Yu Him Justin$$iINSPIRE-00534627$$jORCID:0000-0002-9487-9348$$uVictoria U.
002655508 700__ $$aChizhov, Mihail$$iINSPIRE-00227239$$jORCID:0000-0001-5841-3316$$uDubna, JINR
002655508 700__ $$aChoi, Kyungeon$$iINSPIRE-00180982$$uIndiana U.
002655508 700__ $$aChomont, Arthur Rene$$iINSPIRE-00445232$$uOrsay, LAL
002655508 700__ $$aChouridou, Sofia$$iINSPIRE-00212583$$uAristotle U., Thessaloniki
002655508 700__ $$aChow, Yun Sang$$iINSPIRE-00570908$$uFOM, Amsterdam
002655508 700__ $$aChristodoulou, Valentinos$$iINSPIRE-00407394$$uUniversity Coll. London
002655508 700__ $$aChu, Ming Chung$$iINSPIRE-00436262$$jORCID:0000-0002-1971-0403$$uHong Kong, Chinese U.
002655508 700__ $$aChudoba, Jiri$$iINSPIRE-00150160$$jORCID:0000-0002-6425-2579$$uPrague, Inst. Phys.
002655508 700__ $$aChuinard, Annabelle Julia$$iINSPIRE-00378509$$jORCID:0000-0003-1788-9814$$uMcGill U.
002655508 700__ $$aChwastowski, Janusz$$iINSPIRE-00172390$$jORCID:0000-0002-6190-8376$$uCracow, INP
002655508 700__ $$aChytka, Ladislav$$iINSPIRE-00355090$$uPalacky U.
002655508 700__ $$aCinca, Diane$$iINSPIRE-00212637$$jORCID:0000-0003-0944-8998$$uDortmund U.
002655508 700__ $$aCindro, Vladimir$$iINSPIRE-00073566$$jORCID:0000-0002-2037-7185$$uStefan Inst., Ljubljana
002655508 700__ $$aCioara, Irina Antonela$$iINSPIRE-00395821$$jORCID:0000-0002-9224-3784$$uBonn U.
002655508 700__ $$aCiocio, Alessandra$$iINSPIRE-00073579$$jORCID:0000-0002-3081-4879$$uLBL, Berkeley
002655508 700__ $$aCirotto, Francesco$$iINSPIRE-00414488$$jORCID:0000-0001-6556-856X$$uINFN, Naples$$uNaples U.
002655508 700__ $$aCitron, Zvi Hirsh$$iINSPIRE-00241320$$jORCID:0000-0003-1831-6452$$uWeizmann Inst.
002655508 700__ $$aCitterio, Mauro$$iINSPIRE-00339611$$jORCID:0000-0002-0842-0654$$uINFN, Milan
002655508 700__ $$aClark, Allan G$$iINSPIRE-00073664$$uGeneva U.
002655508 700__ $$aClark, Michael Ryan$$iINSPIRE-00443146$$jORCID:0000-0003-3081-9001$$uNevis Labs, Columbia U.
002655508 700__ $$aClark, Philip James$$iINSPIRE-00144539$$jORCID:0000-0002-3777-0880$$uEdinburgh U.
002655508 700__ $$aClement, Christophe$$iINSPIRE-00147062$$jORCID:0000-0003-3122-3605$$uStockholm U.$$uStockholm U., OKC
002655508 700__ $$aCoadou, Yann$$iINSPIRE-00054627$$jORCID:0000-0001-8195-7004$$uMarseille, CPPM
002655508 700__ $$aCobal, Marina$$iINSPIRE-00073873$$jORCID:0000-0003-3309-0762$$uINFN, Udine$$uUdine U.
002655508 700__ $$aCoccaro, Andrea$$iINSPIRE-00212651$$jORCID:0000-0003-2368-4559$$uINFN, Genoa$$uGenoa U.
002655508 700__ $$aCochran, James H$$iINSPIRE-00145182$$uIowa State U.
002655508 700__ $$aCohen, Hadar Yosef$$iINSPIRE-00549167$$uTel Aviv U.
002655508 700__ $$aCoimbra, Artur Cardoso$$iINSPIRE-00581421$$jORCID:0000-0003-2301-1637$$uWeizmann Inst.
002655508 700__ $$aColasurdo, Luca$$iINSPIRE-00397129$$jORCID:0000-0003-3901-8884$$uNijmegen U.
002655508 700__ $$aCole, Brian$$iINSPIRE-00049517$$jORCID:0000-0002-5092-2148$$uNevis Labs, Columbia U.
002655508 700__ $$aColijn, Auke-Pieter$$iINSPIRE-00212675$$uFOM, Amsterdam
002655508 700__ $$aCollot, Johann$$iINSPIRE-00074106$$jORCID:0000-0002-9412-7090$$uLPSC, Grenoble
002655508 700__ $$aConde Muino, Patricia$$iINSPIRE-00212700$$jORCID:0000-0002-9187-7478$$uLIP, Lisbon$$uIST, Lisbon (main)
002655508 700__ $$aConiavitis, Elias$$iINSPIRE-00004566$$jORCID:0000-0002-2148-8012$$uFreiburg U.
002655508 700__ $$aConnell, Simon Henry$$iINSPIRE-00148123$$jORCID:0000-0001-6000-7245$$uJohannesburg U.
002655508 700__ $$aConnelly, Ian$$iINSPIRE-00352736$$jORCID:0000-0001-9127-6827$$uManchester U.
002655508 700__ $$aConstantinescu, Serban$$iINSPIRE-00212724$$uBucharest, IFIN-HH
002655508 700__ $$aConventi, Francesco$$iINSPIRE-00212748$$uINFN, Naples$$uNaples, Inst. U. Navale
002655508 700__ $$aCooper-Sarkar, Amanda$$iINSPIRE-00074346$$uOxford U.
002655508 700__ $$aCormier, Felix$$iINSPIRE-00530543$$uBritish Columbia U.
002655508 700__ $$aCormier, Kyle James Read$$iINSPIRE-00512833$$uToronto U.
002655508 700__ $$aCorpe, Louie Dartmoor$$uUniversity Coll. London
002655508 700__ $$aCorradi, Massimo$$iINSPIRE-00001854$$jORCID:0000-0001-8729-466X$$uINFN, Rome$$uRome U.
002655508 700__ $$aCorrigan, Eric Edward$$iINSPIRE-00569399$$jORCID:0000-0003-2485-0248$$uLund U.
002655508 700__ $$aCorriveau, Francois$$iINSPIRE-00074601$$jORCID:0000-0002-4970-7600$$uMcGill U.$$uIPP, Canada
002655508 700__ $$aCortes-Gonzalez, Arely$$iINSPIRE-00212778$$jORCID:0000-0002-3279-3370$$uCERN
002655508 700__ $$aCosta, Maria Jose$$iINSPIRE-00212791$$jORCID:0000-0002-2064-2954$$uValencia U., IFIC
002655508 700__ $$aCostanzo, Davide$$iINSPIRE-00212803$$jORCID:0000-0003-4920-6264$$uSheffield U.
002655508 700__ $$aCottin, Giovanna$$iINSPIRE-00334334$$jORCID:0000-0002-5308-5808$$uCambridge U.
002655508 700__ $$aCowan, Glen$$iINSPIRE-00145177$$jORCID:0000-0001-8363-9827$$uRoyal Holloway, U. of London
002655508 700__ $$aCox, Brian$$iINSPIRE-00074854$$uManchester U.
002655508 700__ $$aCrane, Jonathan$$iINSPIRE-00540506$$jORCID:0000-0002-1446-2826$$uManchester U.
002655508 700__ $$aCranmer, Kyle$$iINSPIRE-00074922$$jORCID:0000-0002-5769-7094$$uNew York U.
002655508 700__ $$aCrawley, Samuel Joseph$$iINSPIRE-00399580$$uGlasgow U.
002655508 700__ $$aCreager, Rachael Ann$$iINSPIRE-00524662$$jORCID:0000-0001-8065-6402$$uPennsylvania U.
002655508 700__ $$aCree, Graham$$iINSPIRE-00349746$$uCarleton U.
002655508 700__ $$aCrépé-Renaudin, Sabine$$iINSPIRE-00074993$$jORCID:0000-0001-5980-5805$$uLPSC, Grenoble
002655508 700__ $$aCrescioli, Francesco$$iINSPIRE-00030662$$uParis U., VI-VII
002655508 700__ $$aCristinziani, Markus$$iINSPIRE-00058643$$jORCID:0000-0003-3893-9171$$uBonn U.
002655508 700__ $$aCroft, Vincent$$iINSPIRE-00366990$$jORCID:0000-0002-8731-4525$$uNew York U.
002655508 700__ $$aCrosetti, Giovanni$$iINSPIRE-00212870$$jORCID:0000-0001-5990-4811$$uINFN, Cosenza$$uCalabria U.
002655508 700__ $$aCueto Gomez, Ana Rosario$$iINSPIRE-00517145$$jORCID:0000-0003-1494-7898$$uMadrid, Autonoma U.
002655508 700__ $$aCuhadar Donszelmann, Tulay$$iINSPIRE-00043040$$uSheffield U.
002655508 700__ $$aCukierman, Aviv Ruben$$iINSPIRE-00524677$$jORCID:0000-0002-7834-1716$$uSLAC
002655508 700__ $$aCuth, Jakub$$iINSPIRE-00384079$$uMainz U.
002655508 700__ $$aCzekierda, Sabina$$iINSPIRE-00548796$$jORCID:0000-0003-2878-7266$$uCracow, INP
002655508 700__ $$aCzodrowski, Patrick$$iINSPIRE-00236101$$jORCID:0000-0003-0723-1437$$uCERN
002655508 700__ $$aDa Cunha Sargedas De Sousa, Mario Jose$$iINSPIRE-00339043$$jORCID:0000-0001-7991-593X$$uShandong U.
002655508 700__ $$aDa Via, Cinzia$$iINSPIRE-00212924$$jORCID:0000-0001-6154-7323$$uManchester U.
002655508 700__ $$aDabrowski, Wladyslaw$$iINSPIRE-00178895$$jORCID:0000-0001-9061-9568$$uAGH-UST, Cracow
002655508 700__ $$aDado, Tomas$$iINSPIRE-00508032$$jORCID:0000-0002-7050-2669$$uComenius U.$$uGottingen U., II. Phys. Inst.
002655508 700__ $$aDahbi, Salah-eddine$$iINSPIRE-00563520$$jORCID:0000-0002-5222-7894$$uMohammed V U., Agdal
002655508 700__ $$aDai, Tiesheng$$iINSPIRE-00212987$$jORCID:0000-0002-9607-5124$$uMichigan U.
002655508 700__ $$aDallaire, Frederick$$iINSPIRE-00334341$$uMontreal U.
002655508 700__ $$aDallapiccola, Carlo$$iINSPIRE-00075606$$jORCID:0000-0002-1391-2477$$uMassachusetts U., Amherst
002655508 700__ $$aDam, Mogens$$iINSPIRE-00075612$$jORCID:0000-0001-6278-9674$$uBohr Inst.
002655508 700__ $$aD'amen, Gabriele$$iINSPIRE-00508870$$jORCID:0000-0002-9742-3709$$uINFN, Bologna$$uBologna U.
002655508 700__ $$aDamp, Johannes Frederic$$iINSPIRE-00584568$$jORCID:0000-0002-7290-1372$$uMainz U.
002655508 700__ $$aDandoy, Jeffrey Rogers$$iINSPIRE-00396074$$jORCID:0000-0002-9271-7126$$uPennsylvania U.
002655508 700__ $$aDaneri, Maria Florencia$$iINSPIRE-00548804$$jORCID:0000-0002-2335-793X$$uBuenos Aires U.
002655508 700__ $$aDang, Nguyen Phuong$$iINSPIRE-00410760$$jORCID:0000-0002-9488-6118$$uWisconsin U., Madison$$uLouisville U.
002655508 700__ $$aDann, Nicholas Stuart$$iINSPIRE-00443230$$jORCID:0000-0002-2127-732X$$uManchester U.
002655508 700__ $$aDanninger, Matthias$$iINSPIRE-00324867$$jORCID:0000-0002-7807-7484$$uBritish Columbia U.
002655508 700__ $$aDao, Valerio$$iINSPIRE-00213005$$jORCID:0000-0003-1645-8393$$uCERN
002655508 700__ $$aDarbo, Giovanni$$iINSPIRE-00213017$$jORCID:0000-0003-2165-0638$$uINFN, Genoa
002655508 700__ $$aDarmora, Smita$$iINSPIRE-00337045$$uTexas U., Arlington
002655508 700__ $$aDartsi, Olympia$$iINSPIRE-00576861$$uAnnecy, LAPP
002655508 700__ $$aDattagupta, Aparajita$$iINSPIRE-00221224$$uOregon U.
002655508 700__ $$aDaubney, Thomas$$iINSPIRE-00535012$$uDESY
002655508 700__ $$aD'Auria, Saverio$$iINSPIRE-00212973$$jORCID:0000-0003-3393-6318$$uGlasgow U.
002655508 700__ $$aDavey, Will$$iINSPIRE-00213030$$jORCID:0000-0002-8140-8619$$uBonn U.
002655508 700__ $$aDavid, Claire$$iINSPIRE-00342591$$jORCID:0000-0002-1794-1443$$uDESY
002655508 700__ $$aDavidek, Tomas$$iINSPIRE-00075913$$jORCID:0000-0002-3770-8307$$uCharles U.
002655508 700__ $$aDavis, Douglas$$iINSPIRE-00529350$$jORCID:0000-0003-2679-1288$$uDuke U.
002655508 700__ $$aDawe, Edmund$$iINSPIRE-00213080$$jORCID:0000-0003-0202-3284$$uMelbourne U.
002655508 700__ $$aDawson, Ian$$iINSPIRE-00213091$$jORCID:0000-0002-5177-8950$$uSheffield U.
002655508 700__ $$aDe, Kaushik$$iINSPIRE-00300320$$uTexas U., Arlington
002655508 700__ $$aDe Asmundis, Riccardo$$iINSPIRE-00213110$$jORCID:0000-0002-7268-8401$$uINFN, Naples
002655508 700__ $$aDe Benedetti, Abraham$$iINSPIRE-00018357$$uOklahoma U.
002655508 700__ $$aDe Beurs, Marcus$$iINSPIRE-00639204$$uFOM, Amsterdam
002655508 700__ $$aDe Castro, Stefano$$iINSPIRE-00213121$$jORCID:0000-0003-2178-5620$$uINFN, Bologna$$uBologna U.
002655508 700__ $$aDe Cecco, Sandro$$iINSPIRE-00041280$$jORCID:0000-0003-4907-8610$$uINFN, Rome$$uRome U.
002655508 700__ $$aDe Groot, Nicolo$$iINSPIRE-00213157$$jORCID:0000-0001-6850-4078$$uNijmegen U.
002655508 700__ $$ade Jong, Paul$$iINSPIRE-00093889$$jORCID:0000-0002-5330-2614$$uFOM, Amsterdam
002655508 700__ $$aDe la Torre, Hector$$iINSPIRE-00236142$$jORCID:0000-0002-4516-5269$$uMichigan State U.
002655508 700__ $$aDe Lorenzi, Francesco$$iINSPIRE-00257970$$uIowa State U.
002655508 700__ $$aDe Maria, Antonio$$iINSPIRE-00470316$$jORCID:0000-0001-6651-845X$$uGottingen U., II. Phys. Inst.$$uPisa U.
002655508 700__ $$aDe Pedis, Daniele$$iINSPIRE-00213170$$jORCID:0000-0002-8151-581X$$uINFN, Rome
002655508 700__ $$aDe Salvo, Alessandro$$iINSPIRE-00213182$$jORCID:0000-0001-8099-7821$$uINFN, Rome
002655508 700__ $$aDe Sanctis, Umberto$$iINSPIRE-00213194$$jORCID:0000-0003-4704-525X$$uINFN, Rome2$$uRome U., Tor Vergata
002655508 700__ $$aDe Santis, Maurizio$$iINSPIRE-00585188$$uINFN, Rome2$$uRome U., Tor Vergata
002655508 700__ $$aDe Santo, Antonella$$iINSPIRE-00076214$$uSussex U.
002655508 700__ $$aDe Vasconcelos Corga, Kevin$$iINSPIRE-00535026$$uMarseille, CPPM
002655508 700__ $$aDe Vivie De Regie, Jean-Baptiste$$iINSPIRE-00213200$$jORCID:0000-0001-9163-2211$$uOrsay, LAL
002655508 700__ $$aDebenedetti, Chiara$$iINSPIRE-00236155$$jORCID:0000-0002-6570-0898$$uUC, Santa Cruz
002655508 700__ $$aDedovich, Dmitri$$iINSPIRE-00213224$$uDubna, JINR
002655508 700__ $$aDehghanian, Nooshin$$iINSPIRE-00452091$$uAlberta U.
002655508 700__ $$aDel Gaudio, Michela$$iINSPIRE-00507162$$jORCID:0000-0002-7876-7530$$uINFN, Cosenza$$uCalabria U.
002655508 700__ $$aDel Peso, Jose$$iINSPIRE-00173501$$jORCID:0000-0001-7090-4134$$uMadrid, Autonoma U.
002655508 700__ $$aDelabat Diaz, Yasiel$$iINSPIRE-00581436$$uDESY
002655508 700__ $$aDelgove, David$$iINSPIRE-00396179$$jORCID:0000-0001-7836-5876$$uOrsay, LAL
002655508 700__ $$aDeliot, Frederic$$iINSPIRE-00076511$$jORCID:0000-0003-0777-6031$$uIRFU, Saclay
002655508 700__ $$aDelitzsch, Chris Malena$$iINSPIRE-00364737$$jORCID:0000-0001-7021-3333$$uArizona U.
002655508 700__ $$aDella Pietra, Massimo$$iINSPIRE-00213261$$jORCID:0000-0003-4446-3368$$uINFN, Naples$$uNaples U.
002655508 700__ $$aDella Volpe, Domenico$$iINSPIRE-00134280$$jORCID:0000-0001-8530-7447$$uGeneva U.
002655508 700__ $$aDell'Acqua, Andrea$$iINSPIRE-00213248$$jORCID:0000-0003-2453-7745$$uCERN
002655508 700__ $$aDell'Asta, Lidia$$iINSPIRE-00213250$$jORCID:0000-0002-9601-4225$$uBoston U.
002655508 700__ $$aDelmastro, Marco$$iINSPIRE-00213273$$jORCID:0000-0003-2992-3805$$uAnnecy, LAPP
002655508 700__ $$aDelporte, Charles$$iINSPIRE-00540513$$uOrsay, LAL
002655508 700__ $$aDelsart, Pierre-Antoine$$iINSPIRE-00213285$$jORCID:0000-0002-9556-2924$$uLPSC, Grenoble
002655508 700__ $$aDemarco, David$$iINSPIRE-00381792$$jORCID:0000-0002-8921-8828$$uToronto U.
002655508 700__ $$aDemers, Sarah$$iINSPIRE-00177331$$uYale U.
002655508 700__ $$aDemichev, Mikhail$$iINSPIRE-00213297$$jORCID:0000-0002-7730-3072$$uDubna, JINR
002655508 700__ $$aDenisov, Sergey$$iINSPIRE-00076710$$uSerpukhov, IHEP
002655508 700__ $$aDenysiuk, Denys$$iINSPIRE-00436410$$jORCID:0000-0003-4124-1831$$uFOM, Amsterdam
002655508 700__ $$aD'eramo, Louis$$iINSPIRE-00550307$$jORCID:0000-0002-4910-5378$$uParis U., VI-VII
002655508 700__ $$aDerendarz, Dominik$$iINSPIRE-00229900$$jORCID:0000-0001-5660-3095$$uCracow, INP
002655508 700__ $$aDerkaoui, Jamal Eddine$$iINSPIRE-00213315$$uOujda U.
002655508 700__ $$aDerue, Frederic$$iINSPIRE-00051568$$jORCID:0000-0002-3505-3503$$uParis U., VI-VII
002655508 700__ $$aDervan, Paul$$iINSPIRE-00076798$$jORCID:0000-0003-3929-8046$$uLiverpool U.
002655508 700__ $$aDesch, Klaus Kurt$$iINSPIRE-00076819$$jORCID:0000-0001-5836-6118$$uBonn U.
002655508 700__ $$aDeterre, Cecile$$iINSPIRE-00220614$$jORCID:0000-0001-8371-4401$$uDESY
002655508 700__ $$aDette, Karola$$iINSPIRE-00439451$$jORCID:0000-0002-9593-6201$$uToronto U.
002655508 700__ $$aDevesa, Maria Roberta$$iINSPIRE-00550441$$uBuenos Aires U.
002655508 700__ $$aDeviveiros, Pier-Olivier$$iINSPIRE-00326955$$jORCID:0000-0002-8906-5884$$uCERN
002655508 700__ $$aDewhurst, Alastair$$iINSPIRE-00213327$$jORCID:0000-0002-2062-8052$$uRutherford
002655508 700__ $$aDhaliwal, Saminder$$iINSPIRE-00213340$$uBrandeis U.
002655508 700__ $$aDi Bello, Francesco Armando$$iINSPIRE-00547602$$jORCID:0000-0002-9870-2021$$uGeneva U.
002655508 700__ $$aDi Ciaccio, Anna$$iINSPIRE-00213364$$jORCID:0000-0001-8289-5183$$uINFN, Rome2$$uRome U., Tor Vergata
002655508 700__ $$aDi Ciaccio, Lucia$$iINSPIRE-00213376$$jORCID:0000-0003-0751-8083$$uAnnecy, LAPP
002655508 700__ $$aDi Clemente, William Kennedy$$iINSPIRE-00431482$$uPennsylvania U.
002655508 700__ $$aDi Donato, Camilla$$iINSPIRE-00297740$$jORCID:0000-0003-2213-9284$$uINFN, Naples$$uNaples U.
002655508 700__ $$aDi Girolamo, Alessandro$$iINSPIRE-00213388$$jORCID:0000-0002-9508-4256$$uCERN
002655508 700__ $$aDi Micco, Biagio$$iINSPIRE-00236191$$jORCID:0000-0002-4067-1592$$uINFN, Rome3$$uRome III U.
002655508 700__ $$aDi Nardo, Roberto$$iINSPIRE-00213420$$jORCID:0000-0003-1111-3783$$uMassachusetts U., Amherst
002655508 700__ $$aDi Petrillo, Karri Folan$$iINSPIRE-00534580$$jORCID:0000-0001-8001-4602$$uHarvard U., Phys. Dept.
002655508 700__ $$aDi Sipio, Riccardo$$iINSPIRE-00213443$$jORCID:0000-0002-5951-9558$$uToronto U.
002655508 700__ $$aDi Valentino, David$$iINSPIRE-00352611$$jORCID:0000-0002-9931-0994$$uCarleton U.
002655508 700__ $$aDiaconu, Cristinel$$iINSPIRE-00184938$$jORCID:0000-0002-6193-5091$$uMarseille, CPPM
002655508 700__ $$aDiamond, Miriam$$iINSPIRE-00389950$$uToronto U.
002655508 700__ $$aDe Almeida Dias, Flavia$$iINSPIRE-00176100$$jORCID:0000-0001-6882-5402$$uBohr Inst.
002655508 700__ $$aDias DO Vale, Tiago$$iINSPIRE-00577450$$jORCID:0000-0001-8855-3520$$uLIP, Lisbon
002655508 700__ $$aDiaz, Marco Aurelio$$iINSPIRE-00077083$$uChile U., Catolica
002655508 700__ $$aDickinson, Jennet$$iINSPIRE-00549173$$jORCID:0000-0001-5450-5328$$uLBL, Berkeley
002655508 700__ $$aDiehl, Edward$$iINSPIRE-00213467$$jORCID:0000-0002-7611-355X$$uMichigan U.
002655508 700__ $$aDietrich, Janet$$iINSPIRE-00213479$$jORCID:0000-0001-7061-1585$$uHumboldt U., Berlin
002655508 700__ $$aDíez Cornell, Sergio$$iINSPIRE-00474514$$uDESY
002655508 700__ $$aDimitrievska, Aleksandra$$iINSPIRE-00358147$$jORCID:0000-0003-0086-0599$$uLBL, Berkeley
002655508 700__ $$aDingfelder, Jochen$$iINSPIRE-00049343$$uBonn U.
002655508 700__ $$aDittus, Fido$$iINSPIRE-00077326$$jORCID:0000-0002-1760-8237$$uCERN
002655508 700__ $$aDjama, Fares$$iINSPIRE-00077370$$jORCID:0000-0003-1881-3360$$uMarseille, CPPM
002655508 700__ $$aDjobava, Tamar$$iINSPIRE-00213527$$jORCID:0000-0002-9414-8350$$uTbilisi State U.
002655508 700__ $$aDjuvsland, Julia Isabell$$iINSPIRE-00338727$$jORCID:0000-0002-6488-8219$$uKirchhoff Inst. Phys.
002655508 700__ $$aBarros do Vale, Maria Aline$$iINSPIRE-00213539$$jORCID:0000-0002-0836-6483$$uSao Joao del-Rei Fed. U.
002655508 700__ $$aDobre, Monica$$iINSPIRE-00184940$$jORCID:0000-0002-0841-7180$$uBucharest, IFIN-HH
002655508 700__ $$aDodsworth, David$$iINSPIRE-00534595$$uBrandeis U.
002655508 700__ $$aDoglioni, Caterina$$iINSPIRE-00213578$$jORCID:0000-0002-1509-0390$$uLund U.
002655508 700__ $$aDolejsi, Jiri$$iINSPIRE-00077599$$jORCID:0000-0001-5821-7067$$uCharles U.
002655508 700__ $$aDolezal, Zdenek$$iINSPIRE-00077602$$jORCID:0000-0002-5662-3675$$uCharles U.
002655508 700__ $$aDonadelli, Marisilvia$$iINSPIRE-00241441$$jORCID:0000-0001-8329-4240$$uSao Paulo U.
002655508 700__ $$aDonini, Julien$$iINSPIRE-00041261$$jORCID:0000-0002-8998-0839$$uClermont-Ferrand U.
002655508 700__ $$aD'onofrio, Adelina$$iINSPIRE-00575723$$uQueen Mary, U. of London
002655508 700__ $$aD'Onofrio, Monica$$iINSPIRE-00041292$$uLiverpool U.
002655508 700__ $$aDopke, Jens$$iINSPIRE-00213647$$jORCID:0000-0002-0683-9910$$uRutherford
002655508 700__ $$aDoria, Alessandra$$iINSPIRE-00077860$$jORCID:0000-0002-5381-2649$$uINFN, Naples
002655508 700__ $$aDova, Maria-Teresa$$iINSPIRE-00077959$$jORCID:0000-0001-6113-0878$$uLa Plata U.
002655508 700__ $$aDoyle, Tony$$iINSPIRE-00078002$$jORCID:0000-0001-6322-6195$$uGlasgow U.
002655508 700__ $$aDrechsler, Eric$$iINSPIRE-00390060$$jORCID:0000-0002-8773-7640$$uGottingen U., II. Phys. Inst.
002655508 700__ $$aDreyer, Etienne$$iINSPIRE-00574985$$jORCID:0000-0001-8955-9510$$uSimon Fraser U.
002655508 700__ $$aDreyer, Timo$$iINSPIRE-00580267$$jORCID:0000-0002-7465-7887$$uGottingen U., II. Phys. Inst.
002655508 700__ $$aDu, Yanyan$$iINSPIRE-00433072$$uShandong U.
002655508 700__ $$aDuarte Campderros, Jorge$$iINSPIRE-00308625$$jORCID:0000-0003-0687-5214$$uTel Aviv U.
002655508 700__ $$aDubinin, Filipp$$iINSPIRE-00569409$$jORCID:0000-0003-2182-2727$$uLebedev Inst.
002655508 700__ $$aDubovsky, Michal$$iINSPIRE-00565680$$uComenius U.
002655508 700__ $$aDubreuil, Arnaud$$iINSPIRE-00445353$$jORCID:0000-0001-6161-8793$$uGeneva U.
002655508 700__ $$aDuchovni, Ehud$$iINSPIRE-00152081$$jORCID:0000-0002-7276-6342$$uWeizmann Inst.
002655508 700__ $$aDuckeck, Guenter$$iINSPIRE-00213690$$jORCID:0000-0002-7756-7801$$uMunich U.
002655508 700__ $$aDucourthial, Audrey$$iINSPIRE-00537258$$jORCID:0000-0001-7936-2853$$uParis U., VI-VII
002655508 700__ $$aDucu, Otilia Anamaria$$iINSPIRE-00349755$$jORCID:0000-0001-5914-0524$$uMontreal U.$$uBucharest, IFIN-HH
002655508 700__ $$aDuda, Dominik$$iINSPIRE-00291889$$jORCID:0000-0002-5916-3467$$uMunich, Max Planck Inst.
002655508 700__ $$aDudarev, Alexey$$iINSPIRE-00213702$$jORCID:0000-0002-8713-8162$$uCERN
002655508 700__ $$aDudder, Andreas Christian$$iINSPIRE-00518600$$jORCID:0000-0002-6531-6351$$uMainz U.
002655508 700__ $$aDuffield, Emily Marie$$iINSPIRE-00506863$$uLBL, Berkeley
002655508 700__ $$aDuflot, Laurent$$iINSPIRE-00078379$$jORCID:0000-0002-4871-2176$$uOrsay, LAL
002655508 700__ $$aDuehrssen, Michael$$iINSPIRE-00213726$$jORCID:0000-0002-5833-7058$$uCERN
002655508 700__ $$aDulsen, Carsten$$iINSPIRE-00561460$$jORCID:0000-0003-4813-8757$$uWuppertal U.
002655508 700__ $$aDumancic, Mirta$$iINSPIRE-00441682$$jORCID:0000-0003-2234-4157$$uWeizmann Inst.
002655508 700__ $$aDumitriu, Ana Elena$$iINSPIRE-00540528$$uBucharest, IFIN-HH$$uMarseille, CPPM
002655508 700__ $$aDuncan, Anna Kathryn$$iINSPIRE-00534608$$jORCID:0000-0002-7284-3862$$uGlasgow U.
002655508 700__ $$aDunford, Monica$$iINSPIRE-00029703$$jORCID:0000-0002-7667-260X$$uKirchhoff Inst. Phys.
002655508 700__ $$aDuperrin, Arnaud$$iINSPIRE-00078558$$jORCID:0000-0002-5789-9825$$uMarseille, CPPM
002655508 700__ $$aDuran Yildiz, Hatice$$iINSPIRE-00213740$$jORCID:0000-0003-3469-6045$$uAnkara U.
002655508 700__ $$aDueren, Michael$$iINSPIRE-00078621$$jORCID:0000-0002-6066-4744$$uGiessen U.
002655508 700__ $$aDurglishvili, Archil$$iINSPIRE-00362063$$jORCID:0000-0003-4157-592X$$uTbilisi State U.
002655508 700__ $$aDuschinger, Dirk$$iINSPIRE-00384038$$uDresden, Tech. U.
002655508 700__ $$aDutta, Baishali$$iINSPIRE-00431294$$jORCID:0000-0001-7277-0440$$uDESY
002655508 700__ $$aDuvnjak, Damir$$iINSPIRE-00439515$$uAdelaide U., Sch. Chem. Phys.
002655508 700__ $$aDyndal, Mateusz$$iINSPIRE-00359621$$jORCID:0000-0001-9632-6352$$uDESY
002655508 700__ $$aDysch, Samuel$$iINSPIRE-00584575$$jORCID:0000-0002-7412-9187$$uManchester U.
002655508 700__ $$aDziedzic, Bartosz Sebastian$$iINSPIRE-00548812$$jORCID:0000-0002-0805-9184$$uCracow, INP
002655508 700__ $$aEckardt, Christoph$$iINSPIRE-00397250$$uDESY
002655508 700__ $$aEcker, Katharina Maria$$iINSPIRE-00387516$$uMunich, Max Planck Inst.
002655508 700__ $$aEdgar, Ryan Christopher$$iINSPIRE-00265484$$uMichigan U.
002655508 700__ $$aEifert, Till$$iINSPIRE-00305775$$jORCID:0000-0002-7535-6058$$uCERN
002655508 700__ $$aEigen, Gerald$$iINSPIRE-00079187$$jORCID:0000-0003-3529-5171$$uBergen U.
002655508 700__ $$aEinsweiler, Kevin$$iINSPIRE-00213832$$jORCID:0000-0002-4391-9100$$uLBL, Berkeley
002655508 700__ $$aEkelof, Tord$$iINSPIRE-00079263$$jORCID:0000-0002-7341-9115$$uUppsala U., Inst. Theor. Phys.
002655508 700__ $$aEl Kacimi, Mohamed$$iINSPIRE-00213844$$uCadi Ayyad U., Marrakech
002655508 700__ $$aEl Kosseifi, Rima$$iINSPIRE-00547614$$uMarseille, CPPM
002655508 700__ $$aEllajosyula, Venugopal$$iINSPIRE-00438789$$uMarseille, CPPM
002655508 700__ $$aEllert, Mattias$$iINSPIRE-00079322$$jORCID:0000-0001-5265-3175$$uUppsala U., Inst. Theor. Phys.
002655508 700__ $$aEllinghaus, Frank$$iINSPIRE-00241510$$jORCID:0000-0003-3596-5331$$uWuppertal U.
002655508 700__ $$aElliot, Alison$$iINSPIRE-00379232$$jORCID:0000-0003-0921-0314$$uQueen Mary, U. of London
002655508 700__ $$aEllis, Nicolas$$iINSPIRE-00079357$$jORCID:0000-0002-1920-4930$$uCERN
002655508 700__ $$aElmsheuser, Johannes$$iINSPIRE-00039089$$jORCID:0000-0001-8899-051X$$uBrookhaven
002655508 700__ $$aElsing, Markus$$iINSPIRE-00213874$$jORCID:0000-0002-1213-0545$$uCERN
002655508 700__ $$aEmeliyanov, Dmitry$$iINSPIRE-00213886$$jORCID:0000-0002-1363-9175$$uRutherford
002655508 700__ $$aEnari, Yuji$$iINSPIRE-00079531$$jORCID:0000-0002-9916-3349$$uTokyo U., ICEPP
002655508 700__ $$aEnnis, Joseph Stanford$$iINSPIRE-00524680$$jORCID:0000-0002-1919-0823$$uWarwick U.
002655508 700__ $$aEpland, Matthew Berg$$iINSPIRE-00562211$$jORCID:0000-0001-5340-7240$$uDuke U.
002655508 700__ $$aErdmann, Johannes$$iINSPIRE-00213911$$jORCID:0000-0002-8073-2740$$uDortmund U.
002655508 700__ $$aEreditato, Antonio$$iINSPIRE-00079760$$jORCID:0000-0002-5423-8079$$uBern U., LHEP
002655508 700__ $$aErrede, Steven$$iINSPIRE-00079889$$uIllinois U., Urbana
002655508 700__ $$aEscalier, Marc$$iINSPIRE-00025013$$jORCID:0000-0003-4270-2775$$uOrsay, LAL
002655508 700__ $$aEscobar, Carlos$$iINSPIRE-00213977$$jORCID:0000-0003-4442-4537$$uValencia U., IFIC
002655508 700__ $$aEstrada Pastor, Oscar$$iINSPIRE-00542411$$jORCID:0000-0001-8210-1064$$uValencia U., IFIC
002655508 700__ $$aEtienvre, Anne-Isabelle$$iINSPIRE-00240439$$uIRFU, Saclay
002655508 700__ $$aEtzion, Erez$$iINSPIRE-00080055$$jORCID:0000-0001-6871-7794$$uTel Aviv U.
002655508 700__ $$aEvans, Hal$$iINSPIRE-00080060$$jORCID:0000-0003-2183-3127$$uIndiana U.
002655508 700__ $$aEzhilov, Alexey$$iINSPIRE-00367680$$jORCID:0000-0002-7520-293X$$uSt. Petersburg, INP
002655508 700__ $$aEzzi, Mohammed$$iINSPIRE-00364752$$jORCID:0000-0001-7944-2554$$uMohammed V U., Agdal
002655508 700__ $$aFabbri, Federica$$iINSPIRE-00445370$$jORCID:0000-0001-8474-0978$$uGlasgow U.
002655508 700__ $$aFabbri, Laura$$iINSPIRE-00283861$$jORCID:0000-0002-4002-8353$$uINFN, Bologna$$uBologna U.
002655508 700__ $$aFabiani, Veronica$$iINSPIRE-00551862$$jORCID:0000-0002-7635-7095$$uNijmegen U.
002655508 700__ $$aFacini, Gabriel John$$iINSPIRE-00019223$$jORCID:0000-0002-4056-4578$$uUniversity Coll. London
002655508 700__ $$aFaisca Rodrigues Pereira, Rui Miguel$$iINSPIRE-00577465$$jORCID:0000-0003-1411-5354$$uLIP, Lisbon
002655508 700__ $$aFakhrutdinov, Rinat$$iINSPIRE-00214014$$uSerpukhov, IHEP
002655508 700__ $$aFalciano, Speranza$$iINSPIRE-00214026$$jORCID:0000-0002-7118-341X$$uINFN, Rome
002655508 700__ $$aFalke, Peter Johannes$$iINSPIRE-00578806$$jORCID:0000-0002-2004-476X$$uAnnecy, LAPP
002655508 700__ $$aFalke, Saskia$$iINSPIRE-00578810$$jORCID:0000-0002-0264-1632$$uAnnecy, LAPP
002655508 700__ $$aFaltova, Jana$$iINSPIRE-00221190$$jORCID:0000-0003-4278-7182$$uCharles U.
002655508 700__ $$aFang, Yaquan$$iINSPIRE-00214038$$uBeijing, Inst. High Energy Phys.
002655508 700__ $$aFanti, Marcello$$iINSPIRE-00214040$$jORCID:0000-0002-8773-145X$$uINFN, Milan$$uMilan U.
002655508 700__ $$aFarbin, Amir$$iINSPIRE-00214051$$jORCID:0000-0003-0000-2439$$uTexas U., Arlington
002655508 700__ $$aFarilla, Addolorata$$iINSPIRE-00214063$$jORCID:0000-0002-3983-0728$$uINFN, Rome3
002655508 700__ $$aFarina, Edoardo Maria$$iINSPIRE-00508881$$jORCID:0000-0003-3037-9288$$uINFN, Pavia$$uPavia U.
002655508 700__ $$aFarooque, Trisha$$iINSPIRE-00013478$$jORCID:0000-0003-1363-9324$$uMichigan State U.
002655508 700__ $$aFARRELL, Steven$$iINSPIRE-00014247$$jORCID:0000-0003-1854-4113$$uLBL, Berkeley
002655508 700__ $$aFarrington, Sinead$$iINSPIRE-00060080$$jORCID:0000-0001-5350-9271$$uWarwick U.
002655508 700__ $$aFarthouat, Philippe$$iINSPIRE-00080462$$jORCID:0000-0002-4779-5432$$uCERN
002655508 700__ $$aFassi, Farida$$iINSPIRE-00308854$$jORCID:0000-0002-6423-7213$$uMohammed V U., Agdal
002655508 700__ $$aFassnacht, Patrick$$iINSPIRE-00080473$$jORCID:0000-0002-1516-1195$$uCERN
002655508 700__ $$aFassouliotis, Dimitrios$$iINSPIRE-00214081$$jORCID:0000-0003-1289-2141$$uAthens Natl. Capodistrian U.
002655508 700__ $$aFaucci Giannelli, Michele$$iINSPIRE-00352701$$jORCID:0000-0003-3731-820X$$uEdinburgh U.
002655508 700__ $$aFavareto, Andrea$$iINSPIRE-00286492$$jORCID:0000-0003-3070-8707$$uINFN, Genoa$$uGenoa U.
002655508 700__ $$aFawcett, William James$$iINSPIRE-00389502$$jORCID:0000-0003-2596-8264$$uCambridge U.
002655508 700__ $$aFayard, Louis$$iINSPIRE-00143071$$jORCID:0000-0002-2190-9091$$uOrsay, LAL
002655508 700__ $$aFedin, Oleg$$iINSPIRE-00305797$$uSt. Petersburg, INP$$uSt. Petersburg Polytechnic Inst.
002655508 700__ $$aFedorko, Woiciech$$iINSPIRE-00041224$$jORCID:0000-0002-5138-3473$$uBritish Columbia U.
002655508 700__ $$aFeickert, Matthew$$iINSPIRE-00353992$$jORCID:0000-0003-4124-7862$$uSouthern Methodist U.
002655508 700__ $$aFeigl, Simon$$iINSPIRE-00356540$$jORCID:0000-0002-0154-1525$$uOslo U.
002655508 700__ $$aFeligioni, Lorenzo$$iINSPIRE-00039073$$jORCID:0000-0002-1403-0951$$uMarseille, CPPM
002655508 700__ $$aFeng, Cunfeng$$iINSPIRE-00214142$$jORCID:0000-0001-9138-3200$$uShandong U.
002655508 700__ $$aFeng, Eric$$iINSPIRE-00214154$$jORCID:0000-0002-3946-8941$$uCERN
002655508 700__ $$aFeng, Minyu$$iINSPIRE-00551871$$jORCID:0000-0002-0698-1482$$uDuke U.
002655508 700__ $$aFenton, Michael James$$iINSPIRE-00546149$$jORCID:0000-0003-1002-6880$$uGlasgow U.
002655508 700__ $$aFenyuk, Alexander$$iINSPIRE-00214166$$uSerpukhov, IHEP
002655508 700__ $$aFeremenga, Last$$iINSPIRE-00228200$$uTexas U., Arlington
002655508 700__ $$aFerrando, James$$iINSPIRE-00027519$$jORCID:0000-0002-1007-7816$$uDESY
002655508 700__ $$aFerrari, Arnaud$$iINSPIRE-00300636$$jORCID:0000-0003-2887-5311$$uUppsala U., Inst. Theor. Phys.
002655508 700__ $$aFerrari, Pamela$$iINSPIRE-00214210$$jORCID:0000-0002-1387-153X$$uFOM, Amsterdam
002655508 700__ $$aFerrari, Roberto$$iINSPIRE-00214221$$jORCID:0000-0001-5566-1373$$uINFN, Pavia
002655508 700__ $$aFerreira de Lima, Danilo Enoque$$iINSPIRE-00286519$$jORCID:0000-0002-6606-3595$$uHeidelberg U.
002655508 700__ $$aFerrer, Antonio$$iINSPIRE-00080972$$jORCID:0000-0003-0532-711X$$uValencia U., IFIC
002655508 700__ $$aFerrere, Didier$$iINSPIRE-00188574$$jORCID:0000-0002-5687-9240$$uGeneva U.
002655508 700__ $$aFerretti, Claudio$$iINSPIRE-00028525$$jORCID:0000-0002-5562-7893$$uMichigan U.
002655508 700__ $$aFiedler, Frank$$iINSPIRE-00081065$$jORCID:0000-0002-4610-5612$$uMainz U.
002655508 700__ $$aFilipcic, Andrej$$iINSPIRE-00081160$$uStefan Inst., Ljubljana
002655508 700__ $$aFilthaut, Frank$$iINSPIRE-00081209$$jORCID:0000-0003-3338-2247$$uNijmegen U.
002655508 700__ $$aFinelli, Kevin Daniel$$iINSPIRE-00337620$$jORCID:0000-0001-7979-9473$$uBoston U.
002655508 700__ $$aFiolhais, Miguel$$iINSPIRE-00214269$$jORCID:0000-0001-9035-0335$$uLIP, Lisbon$$uCoimbra U.$$uBMCC, New York
002655508 700__ $$aFiorini, Luca$$iINSPIRE-00214275$$jORCID:0000-0002-5070-2735$$uValencia U., IFIC
002655508 700__ $$aFischer, Cora$$iINSPIRE-00387867$$jORCID:0000-0002-7777-4587$$uBarcelona, IFAE
002655508 700__ $$aFisher, Wade Cameron$$iINSPIRE-00052479$$jORCID:0000-0003-3043-3045$$uMichigan State U.
002655508 700__ $$aFlaschel, Nils$$iINSPIRE-00371327$$uDESY
002655508 700__ $$aFleck, Ivor$$iINSPIRE-00081605$$jORCID:0000-0003-1461-8648$$uSiegen U.
002655508 700__ $$aFleischmann, Philipp$$iINSPIRE-00214324$$jORCID:0000-0001-6968-340X$$uMichigan U.
002655508 700__ $$aFletcher, Rob Roy Mac Gregor$$iINSPIRE-00405355$$uPennsylvania U.
002655508 700__ $$aFlick, Tobias$$iINSPIRE-00214348$$jORCID:0000-0002-8356-6987$$uWuppertal U.
002655508 700__ $$aFlierl, Bernhard Matthias$$iINSPIRE-00542102$$uMunich U.
002655508 700__ $$aFlores, Lucas Macrorie$$iINSPIRE-00569417$$jORCID:0000-0002-2748-758X$$uPennsylvania U.
002655508 700__ $$aFlores Castillo, Luis$$iINSPIRE-00041212$$uHong Kong, Chinese U.
002655508 700__ $$aFollega, Francesco Maria$$iINSPIRE-00641114$$uTIFPA-INFN, Trento$$uTrento U.
002655508 700__ $$aFomin, Nikolai$$iINSPIRE-00549781$$jORCID:0000-0001-9457-394X$$uBergen U.
002655508 700__ $$aForcolin, Giulio Tiziano$$iINSPIRE-00406118$$jORCID:0000-0002-7201-1898$$uManchester U.
002655508 700__ $$aFormica, Andrea$$iINSPIRE-00081940$$jORCID:0000-0001-8308-2643$$uIRFU, Saclay
002655508 700__ $$aFoerster, Fabian Alexander$$iINSPIRE-00544683$$jORCID:0000-0002-3727-8781$$uBarcelona, IFAE
002655508 700__ $$aForti, Alessandra$$iINSPIRE-00027700$$jORCID:0000-0002-0532-7921$$uManchester U.
002655508 700__ $$aFoster, Andrew Geoffrey$$iINSPIRE-00445427$$jORCID:0000-0001-6293-6611$$uBirmingham U.
002655508 700__ $$aFournier, Daniel$$iINSPIRE-00144690$$uOrsay, LAL
002655508 700__ $$aFox, Harald$$iINSPIRE-00082068$$jORCID:0000-0003-3089-6090$$uLancaster U.
002655508 700__ $$aFracchia, Silvia$$iINSPIRE-00361393$$uSheffield U.
002655508 700__ $$aFrancavilla, Paolo$$iINSPIRE-00305814$$jORCID:0000-0003-1164-6870$$uINFN, Pisa$$uPisa U.
002655508 700__ $$aFranchini, Matteo$$iINSPIRE-00293056$$jORCID:0000-0002-4554-252X$$uINFN, Bologna$$uBologna U.
002655508 700__ $$aFranchino, Silvia$$iINSPIRE-00013179$$jORCID:0000-0002-8159-8010$$uKirchhoff Inst. Phys.
002655508 700__ $$aFrancis, David$$iINSPIRE-00214393$$uCERN
002655508 700__ $$aFranconi, Laura$$iINSPIRE-00371528$$jORCID:0000-0002-0647-6072$$uOslo U.
002655508 700__ $$aFranklin, Melissa$$iINSPIRE-00082230$$jORCID:0000-0002-6595-883X$$uHarvard U., Phys. Dept.
002655508 700__ $$aFrate, Meghan$$iINSPIRE-00408123$$jORCID:0000-0003-2510-364X$$uUC, Irvine
002655508 700__ $$aFraternali, Marco$$iINSPIRE-00214419$$jORCID:0000-0002-6527-8279$$uINFN, Pavia$$uPavia U.
002655508 700__ $$aFreeborn, David$$iINSPIRE-00365510$$jORCID:0000-0002-2117-8145$$uUniversity Coll. London
002655508 700__ $$aFressard-Batraneanu, Silvia Maria$$iINSPIRE-00389614$$uCERN
002655508 700__ $$aFreund, Benjamin$$iINSPIRE-00506444$$jORCID:0000-0002-0407-6083$$uMontreal U.
002655508 700__ $$aSpolidoro Freund, Werner$$iINSPIRE-00571600$$jORCID:0000-0003-4473-1027$$uRio de Janeiro Federal U.
002655508 700__ $$aFrizzell, Dylan Cooper$$iINSPIRE-00714311$$jORCID:0000-0003-0288-5941$$uOklahoma U.
002655508 700__ $$aFroidevaux, Daniel$$iINSPIRE-00082670$$jORCID:0000-0003-3986-3922$$uCERN
002655508 700__ $$aFrost, James$$iINSPIRE-00171541$$uOxford U.
002655508 700__ $$aFukunaga, Chikara$$iINSPIRE-00214432$$jORCID:0000-0002-6377-4391$$uTokyo Metropolitan U.
002655508 700__ $$aFullana Torregrosa, Esteban$$iINSPIRE-00002800$$jORCID:0000-0003-3082-621X$$uValencia U., IFIC
002655508 700__ $$aFusayasu, Takahiro$$iINSPIRE-00241597$$uNagasaki Inst. Appl. Sci.
002655508 700__ $$aFuster, Juan$$iINSPIRE-00214444$$jORCID:0000-0002-1290-2031$$uValencia U., IFIC
002655508 700__ $$aGabizon, Ofir$$iINSPIRE-00214469$$uTechnion
002655508 700__ $$aGabrielli, Alessandro$$iINSPIRE-00342638$$jORCID:0000-0001-5346-7841$$uINFN, Bologna$$uBologna U.
002655508 700__ $$aGabrielli, Andrea$$iINSPIRE-00339066$$uLBL, Berkeley
002655508 700__ $$aGach, Grzegorz Pawel$$iINSPIRE-00184415$$jORCID:0000-0001-7558-5312$$uAGH-UST, Cracow
002655508 700__ $$aGadatsch, Stefan$$iINSPIRE-00342641$$jORCID:0000-0002-5615-5082$$uGeneva U.
002655508 700__ $$aGadow, Paul Philipp$$iINSPIRE-00575735$$jORCID:0000-0003-4475-6734$$uMunich, Max Planck Inst.
002655508 700__ $$aGagliardi, Guido$$iINSPIRE-00214470$$jORCID:0000-0002-3550-4124$$uINFN, Genoa$$uGenoa U.
002655508 700__ $$aGagnon, Louis Guillaume$$iINSPIRE-00441787$$jORCID:0000-0003-3000-8479$$uMontreal U.
002655508 700__ $$aGalea, Cristina$$iINSPIRE-00039048$$uBucharest, IFIN-HH
002655508 700__ $$aGalhardo, Bruno$$iINSPIRE-00291919$$jORCID:0000-0003-0641-301X$$uLIP, Lisbon$$uCoimbra U.
002655508 700__ $$aGallas, Elizabeth$$iINSPIRE-00083337$$jORCID:0000-0002-1259-1034$$uOxford U.
002655508 700__ $$aGallop, Bruce$$iINSPIRE-00214494$$jORCID:0000-0001-7401-5043$$uRutherford
002655508 700__ $$aGallus, Petr$$iINSPIRE-00015179$$jORCID:0000-0002-5011-9849$$uPrague, Tech. U.
002655508 700__ $$aGalster, Gorm Aske Gram$$iINSPIRE-00353273$$uBohr Inst.
002655508 700__ $$aGamboa Goni, Rodrigo$$iINSPIRE-00575741$$jORCID:0000-0003-1026-7633$$uQueen Mary, U. of London
002655508 700__ $$aGan, KK$$iINSPIRE-00083439$$uOhio State U.
002655508 700__ $$aGanguly, Sanmay$$iINSPIRE-00225996$$jORCID:0000-0003-1285-9261$$uWeizmann Inst.
002655508 700__ $$aGao, Jun$$iINSPIRE-00578013$$uHefei, CUST
002655508 700__ $$aGao, Yanyan$$iINSPIRE-00145255$$jORCID:0000-0001-6326-4773$$uLiverpool U.
002655508 700__ $$aGao, Yongsheng$$iINSPIRE-00083520$$uSLAC$$uFresno State
002655508 700__ $$aGarcia, Carmen$$iINSPIRE-00214518$$jORCID:0000-0003-1625-7452$$uValencia U., IFIC
002655508 700__ $$aGarcía Navarro, José Enrique$$iINSPIRE-00022084$$jORCID:0000-0002-0279-0523$$uValencia U., IFIC
002655508 700__ $$aGarcia Pascual, Juan Antonio$$iINSPIRE-00550458$$jORCID:0000-0002-7399-7353$$uBeijing, Inst. High Energy Phys.
002655508 700__ $$aGarcia-Sciveres, Maurice$$iINSPIRE-00083629$$jORCID:0000-0002-5800-4210$$uLBL, Berkeley
002655508 700__ $$aGardner, Robert$$iINSPIRE-00083694$$jORCID:0000-0003-1433-9366$$uChicago U., EFI
002655508 700__ $$aGarelli, Nicoletta$$iINSPIRE-00214520$$jORCID:0000-0003-0534-9634$$uSLAC
002655508 700__ $$aGaronne, Vincent$$iINSPIRE-00214543$$uOslo U.
002655508 700__ $$aGasnikova, Ksenia$$iINSPIRE-00425340$$uDESY
002655508 700__ $$aGaudiello, Andrea$$iINSPIRE-00399154$$jORCID:0000-0001-7721-8217$$uINFN, Genoa$$uGenoa U.
002655508 700__ $$aGaudio, Gabriella$$iINSPIRE-00214561$$jORCID:0000-0002-6833-0933$$uINFN, Pavia
002655508 700__ $$aGavrilenko, Igor$$iINSPIRE-00214609$$jORCID:0000-0001-7219-2636$$uLebedev Inst.
002655508 700__ $$aGavrilyuk, Alexander$$iINSPIRE-00535038$$uMoscow, ITEP
002655508 700__ $$aGay, Colin$$iINSPIRE-00214610$$uBritish Columbia U.
002655508 700__ $$aGaycken, Goetz$$iINSPIRE-00214622$$jORCID:0000-0002-2941-9257$$uBonn U.
002655508 700__ $$aGazis, Evangelos$$iINSPIRE-00084094$$jORCID:0000-0002-9272-4254$$uNatl. Tech. U., Athens
002655508 700__ $$aGee, Norman$$iINSPIRE-00214646$$jORCID:0000-0002-8833-3154$$uRutherford
002655508 700__ $$aGeisen, Jannik$$iINSPIRE-00546150$$jORCID:0000-0003-4644-2472$$uGottingen U., II. Phys. Inst.
002655508 700__ $$aGeisen, Marc$$iINSPIRE-00443406$$uMainz U.
002655508 700__ $$aGeisler, Manuel Patrice$$iINSPIRE-00399680$$uKirchhoff Inst. Phys.
002655508 700__ $$aGellerstedt, Karl$$iINSPIRE-00214664$$uStockholm U.$$uStockholm U., OKC
002655508 700__ $$aGemme, Claudia$$iINSPIRE-00214676$$jORCID:0000-0002-1702-5699$$uINFN, Genoa
002655508 700__ $$aGenest, Marie-Helene$$iINSPIRE-00016112$$jORCID:0000-0002-4098-2024$$uLPSC, Grenoble
002655508 700__ $$aGeng, Cong$$iINSPIRE-00423506$$uMichigan U.
002655508 700__ $$aGentile, Simonetta$$iINSPIRE-00214688$$jORCID:0000-0003-4550-7174$$uINFN, Rome$$uRome U.
002655508 700__ $$aGeorge, Simon$$iINSPIRE-00084316$$jORCID:0000-0003-3565-3290$$uRoyal Holloway, U. of London
002655508 700__ $$aGerbaudo, Davide$$iINSPIRE-00047907$$jORCID:0000-0002-4463-0878$$uBarcelona, IFAE
002655508 700__ $$aGessner, Gregor$$iINSPIRE-00548825$$jORCID:0000-0003-3644-6621$$uDortmund U.
002655508 700__ $$aGhasemi, Sara$$iINSPIRE-00409400$$jORCID:0000-0002-9191-2704$$uSiegen U.
002655508 700__ $$aGhasemi Bostanabad, Meisam$$iINSPIRE-00536611$$jORCID:0000-0003-3492-4538$$uVictoria U.
002655508 700__ $$aGhneimat, Mazuza$$iINSPIRE-00443494$$jORCID:0000-0002-4931-2764$$uBonn U.
002655508 700__ $$aGiacobbe, Benedetto$$iINSPIRE-00214725$$jORCID:0000-0003-2987-7642$$uINFN, Bologna
002655508 700__ $$aGiagu, Stefano$$iINSPIRE-00084627$$jORCID:0000-0001-9192-3537$$uINFN, Rome$$uRome U.
002655508 700__ $$aGiangiacomi, Nico$$iINSPIRE-00562246$$jORCID:0000-0001-7314-0168$$uINFN, Bologna$$uBologna U.
002655508 700__ $$aGiannetti, Paola$$iINSPIRE-00003904$$jORCID:0000-0002-3721-9490$$uINFN, Pisa
002655508 700__ $$aGiannini, Antonio$$iINSPIRE-00641124$$jORCID:0000-0002-5683-814X$$uINFN, Naples$$uNaples U.
002655508 700__ $$aGibson, Stephen$$iINSPIRE-00214737$$uRoyal Holloway, U. of London
002655508 700__ $$aGignac, Matthew$$iINSPIRE-00425540$$jORCID:0000-0003-4155-7844$$uUC, Santa Cruz
002655508 700__ $$aGillberg, Dag Ingemar$$iINSPIRE-00006756$$jORCID:0000-0003-0341-0171$$uCarleton U.
002655508 700__ $$aGilles, Geoffrey$$iINSPIRE-00364250$$uWuppertal U.
002655508 700__ $$aGingrich, Douglas$$iINSPIRE-00084876$$jORCID:0000-0002-2552-1449$$uAlberta U.$$uTRIUMF
002655508 700__ $$aGiordani, MarioPaolo$$iINSPIRE-00084948$$jORCID:0000-0002-0792-6039$$uINFN, Udine$$uUdine U.
002655508 700__ $$aGiorgi, Filippo Maria$$iINSPIRE-00214779$$jORCID:0000-0003-1589-2163$$uINFN, Bologna
002655508 700__ $$aGiraud, Pierre-Francois$$iINSPIRE-00214780$$jORCID:0000-0002-8485-9351$$uIRFU, Saclay
002655508 700__ $$aGiromini, Paolo$$iINSPIRE-00085050$$jORCID:0000-0003-0276-287X$$uHarvard U., Phys. Dept.
002655508 700__ $$aGiugliarelli, Gilberto$$iINSPIRE-00560327$$jORCID:0000-0001-5765-1750$$uINFN, Udine$$uUdine U.
002655508 700__ $$aGiugni, Danilo$$iINSPIRE-00214804$$jORCID:0000-0002-6976-0951$$uINFN, Milan
002655508 700__ $$aGiuli, Francesco$$iINSPIRE-00544699$$jORCID:0000-0002-8506-274X$$uOxford U.
002655508 700__ $$aGiulini, Maddalena$$iINSPIRE-00362075$$jORCID:0000-0002-9148-5474$$uHeidelberg U.
002655508 700__ $$aGkaitatzis, Stamatios$$iINSPIRE-00372074$$jORCID:0000-0001-9420-7499$$uAristotle U., Thessaloniki
002655508 700__ $$aGkialas, Ioannis$$iINSPIRE-00236266$$uAthens Natl. Capodistrian U.$$uAegean U., Chios
002655508 700__ $$aGkougkousis, Evangelos$$iINSPIRE-00380163$$jORCID:0000-0002-2132-2071$$uBarcelona, IFAE
002655508 700__ $$aGkountoumis, Panagiotis$$iINSPIRE-00549793$$jORCID:0000-0003-2331-9922$$uNatl. Tech. U., Athens
002655508 700__ $$aGladilin, Leonid$$iINSPIRE-00173602$$jORCID:0000-0001-9422-8636$$uLomonosov Moscow State U.
002655508 700__ $$aGlasman, Claudia$$iINSPIRE-00173488$$jORCID:0000-0003-2025-3817$$uMadrid, Autonoma U.
002655508 700__ $$aGlatzer, Julian Maximilian Volker$$iINSPIRE-00013837$$jORCID:0000-0003-3078-0733$$uBarcelona, IFAE
002655508 700__ $$aGlaysher, Paul$$iINSPIRE-00359633$$jORCID:0000-0002-5437-971X$$uDESY
002655508 700__ $$aGlazov, Alexandre$$iINSPIRE-00326794$$uDESY
002655508 700__ $$aGoblirsch-Kolb, Maximilian$$iINSPIRE-00339087$$jORCID:0000-0002-2785-9654$$uBrandeis U.
002655508 700__ $$aGodlewski, Jan$$iINSPIRE-00214851$$uCracow, INP
002655508 700__ $$aGoldfarb, Steven$$iINSPIRE-00085461$$jORCID:0000-0002-1677-3097$$uMelbourne U.
002655508 700__ $$aGolling, Tobias$$iINSPIRE-00085610$$jORCID:0000-0001-8535-6687$$uGeneva U.
002655508 700__ $$aGolubkov, Dmitry$$iINSPIRE-00260751$$uSerpukhov, IHEP
002655508 700__ $$aGomes, Agostinho$$iINSPIRE-00226662$$jORCID:0000-0002-5940-9893$$uLIP, Lisbon$$uLisbon U., CFNUL
002655508 700__ $$aGoncalves Gama, Rafael$$iINSPIRE-00377697$$jORCID:0000-0002-8263-4263$$uJuiz de Fora U.
002655508 700__ $$aGoncalo, Ricardo$$iINSPIRE-00171282$$jORCID:0000-0002-3826-3442$$uLIP, Lisbon
002655508 700__ $$aGonella, Giulia$$iINSPIRE-00508891$$jORCID:0000-0002-0524-2477$$uFreiburg U.
002655508 700__ $$aGonella, Laura$$iINSPIRE-00001730$$jORCID:0000-0002-4919-0808$$uBirmingham U.
002655508 700__ $$aGongadze, Alexi$$iINSPIRE-00439573$$jORCID:0000-0001-8183-1612$$uDubna, JINR
002655508 700__ $$aGonnella, Francesco$$iINSPIRE-00571490$$jORCID:0000-0003-0885-1654$$uBirmingham U.
002655508 700__ $$aGonski, Julia Lynne$$iINSPIRE-00567375$$jORCID:0000-0003-2037-6315$$uHarvard U., Phys. Dept.
002655508 700__ $$aGonzalez de la Hoz, Santiago$$iINSPIRE-00214978$$jORCID:0000-0001-5304-5390$$uValencia U., IFIC
002655508 700__ $$aGonzalez-Sevilla, Sergio$$iINSPIRE-00214993$$jORCID:0000-0003-4458-9403$$uGeneva U.
002655508 700__ $$aGoossens, Luc$$iINSPIRE-00215005$$jORCID:0000-0002-2536-4498$$uCERN
002655508 700__ $$aGorbounov, Petr Andreevich$$iINSPIRE-00085929$$uMoscow, ITEP
002655508 700__ $$aGordon, Howard$$iINSPIRE-00085936$$jORCID:0000-0003-4362-019X$$uBrookhaven
002655508 700__ $$aGorini, Benedetto$$iINSPIRE-00215017$$jORCID:0000-0003-4177-9666$$uCERN
002655508 700__ $$aGorini, Edoardo$$iINSPIRE-00085978$$jORCID:0000-0002-7688-2797$$uINFN, Lecce$$uSalento U.
002655508 700__ $$aGorisek, Andrej$$iINSPIRE-00215023$$jORCID:0000-0002-3903-3438$$uStefan Inst., Ljubljana
002655508 700__ $$aGoshaw, Alfred$$iINSPIRE-00086006$$jORCID:0000-0002-5704-0885$$uDuke U.
002655508 700__ $$aGoessling, Claus$$iINSPIRE-00189086$$uDortmund U.
002655508 700__ $$aGostkin, Mikhail Ivanovitch$$iINSPIRE-00215072$$jORCID:0000-0002-4311-3756$$uDubna, JINR
002655508 700__ $$aGottardo, Carlo Alberto$$iINSPIRE-00548838$$jORCID:0000-0003-0348-0364$$uBonn U.
002655508 700__ $$aGoudet, Christophe Raymond$$iINSPIRE-00436282$$uOrsay, LAL
002655508 700__ $$aGoujdami, Driss$$iINSPIRE-00215096$$uCadi Ayyad U., Marrakech
002655508 700__ $$aGoussiou, Anna$$iINSPIRE-00086179$$uWashington U., Seattle
002655508 700__ $$aGovender, Nicolin$$iINSPIRE-00335913$$uJohannesburg U.$$uCHPC, Cape Town
002655508 700__ $$aGoy, Corinne$$iINSPIRE-00215110$$jORCID:0000-0002-1297-8925$$uAnnecy, LAPP
002655508 700__ $$aGozani, Eitan$$iINSPIRE-00423098$$uTechnion
002655508 700__ $$aGrabowska-Bold, Iwona$$iINSPIRE-00172493$$jORCID:0000-0001-9159-1210$$uAGH-UST, Cracow
002655508 700__ $$aGradin, Per Olov Joakim$$iINSPIRE-00413032$$jORCID:0000-0003-2866-8339$$uUppsala U., Inst. Theor. Phys.
002655508 700__ $$aGraham, Emily Charlotte$$iINSPIRE-00571412$$jORCID:0000-0001-7353-2022$$uLiverpool U.
002655508 700__ $$aGramling, Johanna$$iINSPIRE-00245767$$uUC, Irvine
002655508 700__ $$aGramstad, Eirik$$iINSPIRE-00328259$$jORCID:0000-0001-5792-5352$$uOslo U.
002655508 700__ $$aGrancagnolo, Sergio$$iINSPIRE-00041686$$jORCID:0000-0001-8490-8304$$uHumboldt U., Berlin
002655508 700__ $$aGratchev, Vadim$$iINSPIRE-00215138$$uSt. Petersburg, INP
002655508 700__ $$aGravila, Paul Mircea$$iINSPIRE-00443594$$jORCID:0000-0002-0154-577X$$uWest Timisoara U.
002655508 700__ $$aGravili, Francesco Giuseppe$$iINSPIRE-00641139$$uINFN, Lecce$$uSalento U.
002655508 700__ $$aGray, Chloe$$iINSPIRE-00541079$$jORCID:0000-0003-0391-795X$$uGlasgow U.
002655508 700__ $$aGray, Heather$$iINSPIRE-00032771$$jORCID:0000-0002-5293-4716$$uLBL, Berkeley
002655508 700__ $$aGreenwood, Zeno Dixon$$iINSPIRE-00086666$$jORCID:0000-0001-5121-0938$$uLouisiana Tech. U.
002655508 700__ $$aGrefe, Christian$$iINSPIRE-00166555$$jORCID:0000-0001-7050-5301$$uBonn U.
002655508 700__ $$aGregersen, Kristian$$iINSPIRE-00236292$$jORCID:0000-0003-0295-1670$$uLund U.
002655508 700__ $$aGregor, Ingrid-Maria$$iINSPIRE-00086670$$jORCID:0000-0002-5976-7818$$uDESY
002655508 700__ $$aGrenier, Philippe$$iINSPIRE-00050339$$jORCID:0000-0002-9926-5417$$uSLAC
002655508 700__ $$aGrevtsov, Kirill$$iINSPIRE-00436367$$jORCID:0000-0003-2704-6028$$uDESY
002655508 700__ $$aGrieser, Nathan Allen$$iINSPIRE-00642175$$uOklahoma U.
002655508 700__ $$aGriffiths, Justin$$iINSPIRE-00036544$$uTexas U., Arlington
002655508 700__ $$aGrillo, Alexander$$iINSPIRE-00086795$$uUC, Santa Cruz
002655508 700__ $$aGrimm, Kathryn$$iINSPIRE-00301388$$jORCID:0000-0001-6587-7397$$uSLAC$$uCal State, East Bay
002655508 700__ $$aGrinstein, Sebastian$$iINSPIRE-00086810$$jORCID:0000-0002-6460-8694$$uBarcelona, IFAE$$uICREA, Barcelona
002655508 700__ $$aGris, Philippe Luc Yves$$iINSPIRE-00086824$$uClermont-Ferrand U.
002655508 700__ $$aGrivaz, Jean-Francois$$iINSPIRE-00086861$$jORCID:0000-0003-4793-7995$$uOrsay, LAL
002655508 700__ $$aGroh, Sabrina$$iINSPIRE-00381611$$jORCID:0000-0002-3001-3545$$uMainz U.
002655508 700__ $$aGross, Eilam$$iINSPIRE-00086983$$uWeizmann Inst.
002655508 700__ $$aGrosse-Knetter, Jorn$$iINSPIRE-00087004$$jORCID:0000-0003-3085-7067$$uGottingen U., II. Phys. Inst.
002655508 700__ $$aGrossi, Giulio Cornelio$$iINSPIRE-00349774$$uLouisiana Tech. U.
002655508 700__ $$aGrout, Zara Jane$$iINSPIRE-00346926$$jORCID:0000-0003-4505-2595$$uUniversity Coll. London
002655508 700__ $$aGrud, Christopher$$iINSPIRE-00566478$$uMichigan U.
002655508 700__ $$aGrummer, Aidan$$iINSPIRE-00436515$$jORCID:0000-0003-2752-1183$$uNew Mexico U.
002655508 700__ $$aGuan, Liang$$iINSPIRE-00361789$$jORCID:0000-0003-1897-1617$$uMichigan U.
002655508 700__ $$aGuan, Wen$$iINSPIRE-00011690$$jORCID:0000-0002-5548-5194$$uWisconsin U., Madison
002655508 700__ $$aGuenther, Jaroslav$$iINSPIRE-00215268$$jORCID:0000-0003-3189-3959$$uCERN
002655508 700__ $$aGuerguichon, Antinea$$iINSPIRE-00575754$$jORCID:0000-0003-3132-7076$$uOrsay, LAL
002655508 700__ $$aGuescini, Francesco$$iINSPIRE-00339090$$jORCID:0000-0001-5351-2673$$uTRIUMF
002655508 700__ $$aGuest, Daniel$$iINSPIRE-00236307$$jORCID:0000-0002-4305-2295$$uUC, Irvine
002655508 700__ $$aGugel, Ralf$$iINSPIRE-00551880$$jORCID:0000-0002-3349-1163$$uFreiburg U.
002655508 700__ $$aGui, Bin$$iINSPIRE-00262919$$uOhio State U.
002655508 700__ $$aGuillemin, Thibault$$iINSPIRE-00180576$$uAnnecy, LAPP
002655508 700__ $$aGuindon, Stefan$$iINSPIRE-00230412$$jORCID:0000-0001-7595-3859$$uCERN
002655508 700__ $$aGul, Umar$$iINSPIRE-00160612$$uGlasgow U.
002655508 700__ $$aGumpert, Christian$$iINSPIRE-00349786$$uCERN
002655508 700__ $$aGuo, Jun$$iINSPIRE-00047393$$jORCID:0000-0001-8125-9433$$uShanghai Jiao Tong U.
002655508 700__ $$aGuo, Wen$$iINSPIRE-00533031$$jORCID:0000-0001-7285-7490$$uMichigan U.
002655508 700__ $$aGuo, Yicheng$$iINSPIRE-00407534$$jORCID:0000-0003-0299-7011$$uHefei, CUST$$uMichigan U.
002655508 700__ $$aGuo, Ziyu$$iINSPIRE-00579671$$uMarseille, CPPM
002655508 700__ $$aGupta, Ruchi$$iINSPIRE-00204451$$jORCID:0000-0003-1510-3371$$uSouthern Methodist U.
002655508 700__ $$aGurbuz, Saime$$iINSPIRE-00439637$$jORCID:0000-0002-9152-1455$$uBogazici U.
002655508 700__ $$aGustavino, Giuliano$$iINSPIRE-00394284$$jORCID:0000-0002-5938-4921$$uOklahoma U.
002655508 700__ $$aGutelman, Benjamin Jacque$$iINSPIRE-00564988$$uTechnion
002655508 700__ $$aGutierrez, Phillip$$iINSPIRE-00087527$$jORCID:0000-0003-2326-3877$$uOklahoma U.
002655508 700__ $$aGutschow, Christian$$iINSPIRE-00346139$$jORCID:0000-0003-0857-794X$$uUniversity Coll. London
002655508 700__ $$aGuyot, Claude$$iINSPIRE-00087556$$uIRFU, Saclay
002655508 700__ $$aGuzik, Marcin Pawel$$iINSPIRE-00337935$$jORCID:0000-0001-7840-0889$$uAGH-UST, Cracow
002655508 700__ $$aGwenlan, Claire$$iINSPIRE-00173806$$jORCID:0000-0002-3518-0617$$uOxford U.
002655508 700__ $$aGwilliam, Carl$$iINSPIRE-00215301$$jORCID:0000-0002-9401-5304$$uLiverpool U.
002655508 700__ $$aHaas, Andy$$iINSPIRE-00053405$$jORCID:0000-0002-4832-0455$$uNew York U.
002655508 700__ $$aHaber, Carl$$iINSPIRE-00087660$$uLBL, Berkeley
002655508 700__ $$aHadavand, Haleh Khani$$iINSPIRE-00042933$$uTexas U., Arlington
002655508 700__ $$aHaddad, Nacim$$iINSPIRE-00364262$$uMohammed V U., Agdal
002655508 700__ $$aHadef, Asma$$iINSPIRE-00439100$$jORCID:0000-0003-2508-0628$$uHefei, CUST
002655508 700__ $$aHageboeck, Stephan$$iINSPIRE-00346932$$uBonn U.
002655508 700__ $$aHagihara, Mutsuto$$iINSPIRE-00524693$$uTsukuba U.
002655508 700__ $$aHakobyan, Hrachya$$iINSPIRE-00215325$$uYerevan Phys. Inst.
002655508 700__ $$aHaleem, Mahsana$$iINSPIRE-00039197$$uWurzburg U.
002655508 700__ $$aHaley, Joseph$$iINSPIRE-00006781$$jORCID:0000-0002-6938-7405$$uOklahoma State U.
002655508 700__ $$aHalladjian, Garabed$$iINSPIRE-00334418$$jORCID:0000-0001-7162-0301$$uMichigan State U.
002655508 700__ $$aHallewell, Gregory David$$iINSPIRE-00088110$$jORCID:0000-0001-6267-8560$$uMarseille, CPPM
002655508 700__ $$aHamacher, Klaus$$iINSPIRE-00088237$$uWuppertal U.
002655508 700__ $$aHamal, Petr$$iINSPIRE-00286535$$jORCID:0000-0003-3139-7234$$uPalacky U.
002655508 700__ $$aHamano, Kenji$$iINSPIRE-00041649$$jORCID:0000-0002-9438-8020$$uVictoria U.
002655508 700__ $$aHamilton, Andrew$$iINSPIRE-00088319$$uCape Town U.
002655508 700__ $$aHamity, Guillermo Nicolas$$iINSPIRE-00375233$$uSheffield U.
002655508 700__ $$aHan, Kunlin$$iINSPIRE-00571534$$jORCID:0000-0002-1627-4810$$uHefei, CUST$$uOrsay, LAL
002655508 700__ $$aHan, Liang$$iINSPIRE-00037384$$jORCID:0000-0002-6353-9711$$uHefei, CUST
002655508 700__ $$aHan, Shuo$$iINSPIRE-00530966$$jORCID:0000-0001-8383-7348$$uBeijing, GUCAS
002655508 700__ $$aHanagaki, Kazunori$$iINSPIRE-00215349$$jORCID:0000-0003-0676-0441$$uKEK, Tsukuba$$uOsaka U.
002655508 700__ $$aHance, Michael$$iINSPIRE-00215350$$jORCID:0000-0001-8392-0934$$uUC, Santa Cruz
002655508 700__ $$aHandl, David Michael$$iINSPIRE-00568385$$jORCID:0000-0002-0399-6486$$uMunich U.
002655508 700__ $$aHaney, Bijan$$iINSPIRE-00403295$$jORCID:0000-0001-9238-0888$$uPennsylvania U.
002655508 700__ $$aHankache, Robert$$iINSPIRE-00569429$$jORCID:0000-0003-4519-8949$$uParis U., VI-VII
002655508 700__ $$aHanke, Paul$$iINSPIRE-00088446$$uKirchhoff Inst. Phys.
002655508 700__ $$aHansen, Eva$$iINSPIRE-00573624$$jORCID:0000-0002-5019-1648$$uLund U.
002655508 700__ $$aHansen, Jorgen Beck$$iINSPIRE-00215374$$jORCID:0000-0002-3684-8340$$uBohr Inst.
002655508 700__ $$aHansen, Jorn Dines$$iINSPIRE-00088500$$jORCID:0000-0003-3102-0437$$uBohr Inst.
002655508 700__ $$aHansen, Maike Christina$$iINSPIRE-00395987$$uBonn U.
002655508 700__ $$aHansen, Peter Henrik$$iINSPIRE-00215386$$jORCID:0000-0002-6764-4789$$uBohr Inst.
002655508 700__ $$aHara, Kazuhiko$$iINSPIRE-00300064$$jORCID:0000-0003-1629-0535$$uTsukuba U.
002655508 700__ $$aHard, Andrew Straiton$$iINSPIRE-00334429$$jORCID:0000-0002-8273-5945$$uWisconsin U., Madison
002655508 700__ $$aHarenberg, Torsten$$iINSPIRE-00215424$$uWuppertal U.
002655508 700__ $$aHarkusha, Siarhei$$iINSPIRE-00236332$$jORCID:0000-0002-0309-4490$$uMinsk, Inst. Phys.
002655508 700__ $$aHarrison, Paul Fraser$$iINSPIRE-00088800$$uWarwick U.
002655508 700__ $$aHartmann, Nikolai Marcel$$iINSPIRE-00452386$$uMunich U.
002655508 700__ $$aHasegawa, Yoji$$iINSPIRE-00089003$$jORCID:0000-0003-2683-7389$$uShinshu U.
002655508 700__ $$aHasib, Ahmed$$iINSPIRE-00359645$$jORCID:0000-0003-0457-2244$$uEdinburgh U.
002655508 700__ $$aHassani, Samira$$iINSPIRE-00215473$$jORCID:0000-0002-2834-5110$$uIRFU, Saclay
002655508 700__ $$aHaug, Sigve$$iINSPIRE-00215485$$jORCID:0000-0003-0442-3361$$uBern U., LHEP
002655508 700__ $$aHauser, Reiner$$iINSPIRE-00215503$$jORCID:0000-0001-7682-8857$$uMichigan State U.
002655508 700__ $$aHauswald, Lorenz$$iINSPIRE-00387053$$uDresden, Tech. U.
002655508 700__ $$aHavener, Laura Brittany$$iINSPIRE-00436609$$jORCID:0000-0002-4743-2885$$uNevis Labs, Columbia U.
002655508 700__ $$aHavranek, Miroslav$$iINSPIRE-00021242$$uPrague, Tech. U.
002655508 700__ $$aHawkes, Christopher$$iINSPIRE-00089196$$jORCID:0000-0001-9167-0592$$uBirmingham U.
002655508 700__ $$aHawkings, Richard$$iINSPIRE-00148070$$jORCID:0000-0001-9719-0290$$uCERN
002655508 700__ $$aHayden, Daniel$$iINSPIRE-00286543$$jORCID:0000-0001-5220-2972$$uMichigan State U.
002655508 700__ $$aHayes, Christopher$$iINSPIRE-00578825$$jORCID:0000-0002-0298-0351$$uSUNY, Stony Brook
002655508 700__ $$aHays, Chris$$iINSPIRE-00050513$$jORCID:0000-0003-2371-9723$$uOxford U.
002655508 700__ $$aHays, Jonathan Michael$$iINSPIRE-00005408$$jORCID:0000-0003-1554-5401$$uQueen Mary, U. of London
002655508 700__ $$aHayward, Helen$$iINSPIRE-00142771$$jORCID:0000-0002-0972-3411$$uLiverpool U.
002655508 700__ $$aHaywood, Stephen$$iINSPIRE-00089254$$jORCID:0000-0003-2074-013X$$uRutherford
002655508 700__ $$aHeath, Matthew Peter$$iINSPIRE-00578168$$jORCID:0000-0003-2945-8448$$uEdinburgh U.
002655508 700__ $$aHedberg, Vincent$$iINSPIRE-00215527$$jORCID:0000-0002-4596-3965$$uLund U.
002655508 700__ $$aHeelan, Louise$$iINSPIRE-00215539$$jORCID:0000-0002-4879-0131$$uTexas U., Arlington
002655508 700__ $$aHeer, Sebastian$$iINSPIRE-00551895$$jORCID:0000-0002-1618-5973$$uBonn U.
002655508 700__ $$aHeidegger, Kim Katrin$$iINSPIRE-00224321$$jORCID:0000-0003-3113-0484$$uFreiburg U.
002655508 700__ $$aHeilman, Jesse$$iINSPIRE-00291600$$jORCID:0000-0001-6792-2294$$uCarleton U.
002655508 700__ $$aHeim, Sarah$$iINSPIRE-00215540$$jORCID:0000-0002-2639-6571$$uDESY
002655508 700__ $$aHeim, Timon Frank-thomas$$iINSPIRE-00356268$$jORCID:0000-0002-7669-5318$$uLBL, Berkeley
002655508 700__ $$aHeinemann, Beate$$iINSPIRE-00089482$$jORCID:0000-0002-1673-7926$$uDESY$$uFreiburg U.
002655508 700__ $$aHeinrich, Jochen Jens$$iINSPIRE-00441872$$jORCID:0000-0002-0253-0924$$uMunich U.
002655508 700__ $$aHeinrich, Lukas$$iINSPIRE-00356271$$jORCID:0000-0002-4048-7584$$uNew York U.
002655508 700__ $$aHeinz, Christian$$iINSPIRE-00439219$$uGiessen U.
002655508 700__ $$aHejbal, Jiri$$iINSPIRE-00339101$$uPrague, Inst. Phys.
002655508 700__ $$aHelary, Louis$$iINSPIRE-00215564$$jORCID:0000-0001-7891-8354$$uCERN
002655508 700__ $$aHeld, Alexander$$iINSPIRE-00536620$$jORCID:0000-0002-8924-5885$$uBritish Columbia U.
002655508 700__ $$aHellesund, Simen$$iINSPIRE-00576474$$jORCID:0000-0002-4424-4643$$uOslo U.
002655508 700__ $$aHellman, Sten$$iINSPIRE-00089640$$jORCID:0000-0002-5415-1600$$uStockholm U.$$uStockholm U., OKC
002655508 700__ $$aHelsens, Clement$$iINSPIRE-00215588$$jORCID:0000-0002-9243-7554$$uCERN
002655508 700__ $$aHenderson, Robert$$iINSPIRE-00037338$$uLancaster U.
002655508 700__ $$aHeng, Yang$$iINSPIRE-00334432$$uWisconsin U., Madison
002655508 700__ $$aHenkelmann, Steffen$$iINSPIRE-00407415$$jORCID:0000-0001-5431-5428$$uBritish Columbia U.
002655508 700__ $$aHenriques Correia, Ana Maria$$iINSPIRE-00305891$$uCERN
002655508 700__ $$aHerbert, Geoffrey Henry$$iINSPIRE-00337055$$uHumboldt U., Berlin
002655508 700__ $$aHerde, Hannah$$iINSPIRE-00524702$$jORCID:0000-0001-8926-6734$$uBrandeis U.
002655508 700__ $$aHerget, Verena$$iINSPIRE-00524714$$jORCID:0000-0001-5126-2666$$uWurzburg U.
002655508 700__ $$aHernandez Jimenez, Yesenia$$iINSPIRE-00215618$$uWitwatersrand U.
002655508 700__ $$aHerr, Holger$$iINSPIRE-00549805$$uMainz U.
002655508 700__ $$aHerrmann, Maximilian Georg$$iINSPIRE-00640487$$uMunich U.
002655508 700__ $$aHerten, Gregor$$iINSPIRE-00089942$$jORCID:0000-0001-7661-5122$$uFreiburg U.
002655508 700__ $$aHertenberger, Ralf$$iINSPIRE-00215631$$uMunich U.
002655508 700__ $$aHervas, Luis$$iINSPIRE-00215643$$uCERN
002655508 700__ $$aHerwig, Theodor Christian$$iINSPIRE-00535667$$jORCID:0000-0002-4280-6382$$uPennsylvania U.
002655508 700__ $$aHesketh, Gavin Grant$$iINSPIRE-00054306$$jORCID:0000-0003-4537-1385$$uUniversity Coll. London
002655508 700__ $$aHessey, Nigel$$iINSPIRE-00090012$$jORCID:0000-0002-6698-9937$$uTRIUMF
002655508 700__ $$aHetherly, Jeffrey Wayne$$iINSPIRE-00392821$$uSouthern Methodist U.
002655508 700__ $$aHigashino, Satoshi$$iINSPIRE-00536635$$uKEK, Tsukuba
002655508 700__ $$aHigon-Rodriguez, Emilio$$iINSPIRE-00215655$$jORCID:0000-0002-3094-2520$$uValencia U., IFIC
002655508 700__ $$aHildebrand, Kevin$$iINSPIRE-00549818$$uChicago U., EFI
002655508 700__ $$aHill, Ewan$$iINSPIRE-00345031$$jORCID:0000-0002-1725-7414$$uVictoria U.
002655508 700__ $$aHill, John$$iINSPIRE-00090279$$jORCID:0000-0002-8650-2807$$uCambridge U.
002655508 700__ $$aHill, Kurt Keys$$iINSPIRE-00580945$$jORCID:0000-0002-0119-0366$$uBrookhaven
002655508 700__ $$aHiller, Karl Heinz$$iINSPIRE-00185199$$uDESY
002655508 700__ $$aHillier, Stephen$$iINSPIRE-00090318$$jORCID:0000-0002-7599-6469$$uBirmingham U.
002655508 700__ $$aHils, Maximilian$$iINSPIRE-00534610$$jORCID:0000-0002-8616-5898$$uDresden, Tech. U.
002655508 700__ $$aHinchliffe, Ian$$iINSPIRE-00161746$$jORCID:0000-0002-5529-2173$$uLBL, Berkeley
002655508 700__ $$aHirose, Minoru$$iINSPIRE-00215710$$jORCID:0000-0003-4988-9149$$uOsaka U.
002655508 700__ $$aHirschbuehl, Dominic$$iINSPIRE-00041134$$jORCID:0000-0002-7998-8925$$uWuppertal U.
002655508 700__ $$aHiti, Bojan$$iINSPIRE-00541780$$jORCID:0000-0002-8668-6933$$uStefan Inst., Ljubljana
002655508 700__ $$aHladik, Ondrej$$iINSPIRE-00512847$$uPrague, Inst. Phys.
002655508 700__ $$aHlaluku, Dingane Reward$$iINSPIRE-00572370$$jORCID:0000-0001-6534-9121$$uWitwatersrand U.
002655508 700__ $$aHoad, Xanthe$$iINSPIRE-00441925$$jORCID:0000-0002-8334-8541$$uEdinburgh U.
002655508 700__ $$aHobbs, John$$iINSPIRE-00090491$$uSUNY, Stony Brook
002655508 700__ $$aHod, Noam$$iINSPIRE-00215734$$jORCID:0000-0001-5241-0544$$uTRIUMF
002655508 700__ $$aHodgkinson, Mark$$iINSPIRE-00030600$$jORCID:0000-0002-1040-1241$$uSheffield U.
002655508 700__ $$aHoecker, Andreas$$iINSPIRE-00090516$$jORCID:0000-0002-6596-9395$$uCERN
002655508 700__ $$aHoeferkamp, Martin$$iINSPIRE-00021230$$uNew Mexico U.
002655508 700__ $$aHoenig, Friedrich$$iINSPIRE-00376466$$uMunich U.
002655508 700__ $$aHohn, David$$iINSPIRE-00392879$$jORCID:0000-0002-5317-1247$$uBonn U.
002655508 700__ $$aHohov, Dmytro$$iINSPIRE-00574409$$uOrsay, LAL
002655508 700__ $$aHolmes, Tova Ray$$iINSPIRE-00349798$$uChicago U., EFI
002655508 700__ $$aHolzbock, Michael$$iINSPIRE-00570916$$jORCID:0000-0001-8018-4185$$uMunich U.
002655508 700__ $$aHomann, Michael$$iINSPIRE-00381480$$uDortmund U.
002655508 700__ $$aHonda, Shunsuke$$iINSPIRE-00524723$$jORCID:0000-0002-0403-3729$$uTsukuba U.
002655508 700__ $$aHonda, Takuya$$iINSPIRE-00524733$$uKEK, Tsukuba
002655508 700__ $$aHong, Tae Min$$iINSPIRE-00042918$$jORCID:0000-0001-7834-328X$$uPittsburgh U.
002655508 700__ $$aHonle, Andreas$$iINSPIRE-00577471$$jORCID:0000-0001-6063-2884$$uMunich, Max Planck Inst.
002655508 700__ $$aHooberman, Benjamin Henry$$iINSPIRE-00017664$$jORCID:0000-0002-4090-6099$$uIllinois U., Urbana
002655508 700__ $$aHopkins, Walter Howard$$iINSPIRE-00009068$$jORCID:0000-0001-7814-8740$$uOregon U.
002655508 700__ $$aHorii, Yasuyuki$$iINSPIRE-00370685$$jORCID:0000-0003-0457-3052$$uNagoya U.
002655508 700__ $$aHorn, Philipp$$iINSPIRE-00567091$$jORCID:0000-0002-5640-0447$$uDresden, Tech. U.
002655508 700__ $$aHorton, Arthur James$$iINSPIRE-00376759$$jORCID:0000-0003-0287-3289$$uSimon Fraser U.
002655508 700__ $$aHoryn, Lesya Anna$$iINSPIRE-00576873$$jORCID:0000-0002-9512-4932$$uChicago U., EFI
002655508 700__ $$aHostachy, Jean-Yves$$iINSPIRE-00215837$$uLPSC, Grenoble
002655508 700__ $$aHostiuc, Alexandru$$iINSPIRE-00567103$$uWashington U., Seattle
002655508 700__ $$aHou, Suen$$iINSPIRE-00091198$$jORCID:0000-0001-9861-151X$$uTaiwan, Inst. Phys.
002655508 700__ $$aHoummada, Abdeslam$$iINSPIRE-00215849$$uCasablanca U.
002655508 700__ $$aHowarth, James$$iINSPIRE-00230643$$jORCID:0000-0002-0560-8985$$uManchester U.
002655508 700__ $$aHoya, Joaquin$$iINSPIRE-00517879$$jORCID:0000-0002-7562-0234$$uLa Plata U.
002655508 700__ $$aHrabovsky, Miroslav$$iINSPIRE-00334449$$jORCID:0000-0003-4223-7316$$uPalacky U.
002655508 700__ $$aHrdinka, Julia$$iINSPIRE-00547626$$uCERN
002655508 700__ $$aHristova, Ivana$$iINSPIRE-00286578$$jORCID:0000-0001-7958-1431$$uHumboldt U., Berlin
002655508 700__ $$aHrivnac, Julius$$iINSPIRE-00215850$$uOrsay, LAL
002655508 700__ $$aHrynevich, Aliaksei$$iINSPIRE-00383643$$jORCID:0000-0002-5411-114X$$uMinsk, High Energy Phys. Ctr.
002655508 700__ $$aHryn'ova, Tetiana$$iINSPIRE-00049739$$jORCID:0000-0001-5914-8614$$uAnnecy, LAPP
002655508 700__ $$aHsu, Pai-hsien Jennifer$$iINSPIRE-00036505$$jORCID:0000-0003-3895-8356$$uTaiwan, Natl. Tsing Hua U.
002655508 700__ $$aHsu, Shih-Chieh$$iINSPIRE-00041120$$uWashington U., Seattle
002655508 700__ $$aHu, Qipeng$$iINSPIRE-00386928$$jORCID:0000-0002-9705-7518$$uBrookhaven
002655508 700__ $$aHu, Shuyang$$iINSPIRE-00388803$$jORCID:0000-0003-4696-4430$$uShanghai Jiao Tong U.
002655508 700__ $$aHuang, Yanping$$iINSPIRE-00340219$$jORCID:0000-0002-5972-2855$$uBeijing, Inst. High Energy Phys.
002655508 700__ $$aHubacek, Zdenek$$iINSPIRE-00032940$$jORCID:0000-0003-3250-9066$$uPrague, Tech. U.
002655508 700__ $$aHubaut, Fabrice$$iINSPIRE-00215862$$jORCID:0000-0002-0113-2465$$uMarseille, CPPM
002655508 700__ $$aHuebner, Michael$$iINSPIRE-00578837$$jORCID:0000-0002-1162-8763$$uBonn U.
002655508 700__ $$aHuegging, Fabian$$iINSPIRE-00215874$$jORCID:0000-0002-7472-3151$$uBonn U.
002655508 700__ $$aHuffman, Todd Brian$$iINSPIRE-00215888$$jORCID:0000-0002-5332-2738$$uOxford U.
002655508 700__ $$aHughes, Emlyn$$iINSPIRE-00091540$$uNevis Labs, Columbia U.
002655508 700__ $$aHuhtinen, Mika$$iINSPIRE-00320486$$jORCID:0000-0002-1752-3583$$uCERN
002655508 700__ $$aHunter, Robert Francis$$iINSPIRE-00566486$$jORCID:0000-0002-6839-7775$$uCarleton U.
002655508 700__ $$aHuo, Peng$$iINSPIRE-00386180$$uSUNY, Stony Brook
002655508 700__ $$aHupe, Andre Marc$$iINSPIRE-00568398$$uCarleton U.
002655508 700__ $$aHuseynov, Nazim$$iINSPIRE-00215894$$uDubna, JINR$$uBaku, Inst. Phys.
002655508 700__ $$aHuston, Joey$$iINSPIRE-00091715$$uMichigan State U.
002655508 700__ $$aHuth, John$$iINSPIRE-00091758$$jORCID:0000-0002-6867-2538$$uHarvard U., Phys. Dept.
002655508 700__ $$aHyneman, Rachel$$iINSPIRE-00564990$$jORCID:0000-0002-9093-7141$$uMichigan U.
002655508 700__ $$aIacobucci, Giuseppe$$iINSPIRE-00172036$$jORCID:0000-0001-9965-5442$$uGeneva U.
002655508 700__ $$aIakovidis, Georgios$$iINSPIRE-00215906$$jORCID:0000-0002-0330-5921$$uBrookhaven
002655508 700__ $$aIbragimov, Iskander$$iINSPIRE-00215918$$jORCID:0000-0001-8847-7337$$uSiegen U.
002655508 700__ $$aIconomidou-Fayard, Lydia$$iINSPIRE-00215920$$jORCID:0000-0001-6334-6648$$uOrsay, LAL
002655508 700__ $$aIdrissi, Zineb$$iINSPIRE-00378656$$uMohammed V U., Agdal
002655508 700__ $$aIengo, Paolo$$iINSPIRE-00215943$$jORCID:0000-0002-5035-1242$$uCERN
002655508 700__ $$aIgnazzi, Rosanna$$iINSPIRE-00575001$$uBohr Inst.
002655508 700__ $$aIgonkina, Olga$$iINSPIRE-00057191$$jORCID:0000-0002-9472-0759$$uFOM, Amsterdam$$uNijmegen U.
002655508 700__ $$aIguchi, Ryunosuke$$iINSPIRE-00565002$$uTokyo U., ICEPP
002655508 700__ $$aIizawa, Tomoya$$iINSPIRE-00353645$$jORCID:0000-0001-5312-4865$$uGeneva U.
002655508 700__ $$aIkegami, Yoichi$$iINSPIRE-00215955$$uKEK, Tsukuba
002655508 700__ $$aIkeno, Masahiro$$iINSPIRE-00215967$$jORCID:0000-0003-3105-088X$$uKEK, Tsukuba
002655508 700__ $$aIliadis, Dimitrios$$iINSPIRE-00215979$$jORCID:0000-0001-6303-2761$$uAristotle U., Thessaloniki
002655508 700__ $$aIlic, Nikolina$$iINSPIRE-00236423$$uNijmegen U.
002655508 700__ $$aIltzsche Speiser, Franziska$$iINSPIRE-00544700$$uDresden, Tech. U.
002655508 700__ $$aIntrozzi, Gianluca$$iINSPIRE-00092229$$jORCID:0000-0002-1314-2580$$uINFN, Pavia$$uPavia U.
002655508 700__ $$aIodice, Mauro$$iINSPIRE-00215987$$jORCID:0000-0003-4446-8150$$uINFN, Rome3
002655508 700__ $$aIordanidou, Kalliopi$$iINSPIRE-00286590$$jORCID:0000-0002-5375-934X$$uNevis Labs, Columbia U.
002655508 700__ $$aIppolito, Valerio$$iINSPIRE-00286608$$jORCID:0000-0001-5126-1620$$uINFN, Rome$$uRome U.
002655508 700__ $$aIsacson, Max Fredrik$$iINSPIRE-00517150$$jORCID:0000-0003-1630-6664$$uUppsala U., Inst. Theor. Phys.
002655508 700__ $$aIshijima, Naoki$$iINSPIRE-00417878$$uOsaka U.
002655508 700__ $$aIshino, Masaya$$iINSPIRE-00092428$$jORCID:0000-0002-7185-1334$$uTokyo U., ICEPP
002655508 700__ $$aIshitsuka, Masaki$$iINSPIRE-00184437$$uTokyo Inst. Tech.
002655508 700__ $$aIslam, Wasikul$$iINSPIRE-00586069$$jORCID:0000-0002-5624-5934$$uOklahoma State U.
002655508 700__ $$aIssever, Cigdem$$iINSPIRE-00178101$$uOxford U.
002655508 700__ $$aIstin, Serhat$$iINSPIRE-00216012$$jORCID:0000-0001-8504-6291$$uBogazici U.$$uNear East U.
002655508 700__ $$aIto, Fumiaki$$iINSPIRE-00441977$$uTsukuba U.
002655508 700__ $$aIturbe Ponce, Julia Mariana$$iINSPIRE-00358758$$uHong Kong, Chinese U.
002655508 700__ $$aIuppa, Roberto$$iINSPIRE-00368483$$jORCID:0000-0001-5038-2762$$uTIFPA-INFN, Trento$$uTrento U.
002655508 700__ $$aIvina, Anna$$iINSPIRE-00577489$$uWeizmann Inst.
002655508 700__ $$aIwasaki, Hiroyuki$$iINSPIRE-00216040$$jORCID:0000-0002-9724-8525$$uKEK, Tsukuba
002655508 700__ $$aIzen, Joseph$$iINSPIRE-00092738$$jORCID:0000-0002-9846-5601$$uTexas U., Dallas
002655508 700__ $$aIzzo, Vincenzo$$iINSPIRE-00216053$$jORCID:0000-0002-8770-1592$$uINFN, Naples
002655508 700__ $$aJacka, Petr$$iINSPIRE-00576487$$jORCID:0000-0003-2489-9930$$uPrague, Inst. Phys.
002655508 700__ $$aJackson, Paul$$iINSPIRE-00042110$$jORCID:0000-0002-0847-402X$$uAdelaide U., Sch. Chem. Phys.
002655508 700__ $$aJacobs, Ruth Magdalena$$iINSPIRE-00540535$$jORCID:0000-0001-5446-5901$$uBonn U.
002655508 700__ $$aJain, Vivek$$iINSPIRE-00093006$$jORCID:0000-0002-0214-5292$$uSUNY, Albany
002655508 700__ $$aJakel, Gunnar$$iINSPIRE-00567813$$jORCID:0000-0001-5687-1006$$uWuppertal U.
002655508 700__ $$aJakobi, Katharina Bianca$$iINSPIRE-00381934$$uMainz U.
002655508 700__ $$aJakobs, Karl$$iINSPIRE-00093013$$jORCID:0000-0001-8885-012X$$uFreiburg U.
002655508 700__ $$aJakobsen, Sune$$iINSPIRE-00216083$$jORCID:0000-0002-6564-040X$$uInnsbruck U.
002655508 700__ $$aJakoubek, Tomas$$iINSPIRE-00236452$$jORCID:0000-0001-7038-0369$$uPrague, Inst. Phys.
002655508 700__ $$aJamin, David Olivier$$iINSPIRE-00019160$$jORCID:0000-0003-4231-3868$$uOklahoma State U.
002655508 700__ $$aJana, Dilip$$iINSPIRE-00216107$$uLouisiana Tech. U.
002655508 700__ $$aJansky, Roland$$iINSPIRE-00389298$$jORCID:0000-0003-0456-4658$$uGeneva U.
002655508 700__ $$aJanssen, Jens$$iINSPIRE-00339121$$jORCID:0000-0002-2391-3078$$uBonn U.
002655508 700__ $$aJanus, Michel$$iINSPIRE-00216144$$jORCID:0000-0003-0410-8097$$uGottingen U., II. Phys. Inst.
002655508 700__ $$aJanus, Piotr Andrzej$$iINSPIRE-00524744$$jORCID:0000-0002-0016-2881$$uAGH-UST, Cracow
002655508 700__ $$aJarlskog, Goeran$$iINSPIRE-00175123$$jORCID:0000-0002-8731-2060$$uLund U.
002655508 700__ $$aJavadov, Namig$$iINSPIRE-00358780$$uDubna, JINR$$uBaku, Inst. Phys.
002655508 700__ $$aJavurek, Tomas$$iINSPIRE-00359657$$uCERN
002655508 700__ $$aJavurkova, Martina$$iINSPIRE-00359670$$jORCID:0000-0001-8798-808X$$uFreiburg U.
002655508 700__ $$aJeanneau, Fabien$$iINSPIRE-00380308$$jORCID:0000-0002-6360-6136$$uIRFU, Saclay
002655508 700__ $$aJeanty, Laura$$iINSPIRE-00216156$$jORCID:0000-0001-6507-4623$$uLBL, Berkeley
002655508 700__ $$aJejelava, Juansher$$iINSPIRE-00396142$$uTbilisi, Inst. Phys.$$uIlia State U.
002655508 700__ $$aJelinskas, Adomas$$iINSPIRE-00537773$$jORCID:0000-0002-1933-8031$$uWarwick U.
002655508 700__ $$aJenni, Peter$$iINSPIRE-00093290$$jORCID:0000-0002-4539-4192$$uFreiburg U.$$uCERN
002655508 700__ $$aJeong, Jihyun$$iINSPIRE-00583970$$jORCID:0000-0003-3069-5416$$uDESY
002655508 700__ $$aJezequel, Stephane$$iINSPIRE-00216174$$jORCID:0000-0001-7369-6975$$uAnnecy, LAPP
002655508 700__ $$aJi, Haoshuang$$iINSPIRE-00216186$$uWisconsin U., Madison
002655508 700__ $$aJia, Jiangyong$$iINSPIRE-00241915$$jORCID:0000-0002-5725-3397$$uSUNY, Stony Brook
002655508 700__ $$aJiang, Hai$$iINSPIRE-00431393$$uIowa State U.
002655508 700__ $$aJiang, Yi$$iINSPIRE-00216201$$uHefei, CUST
002655508 700__ $$aJiang, Zihao$$iINSPIRE-00524754$$uSLAC$$uStanford U., Phys. Dept.
002655508 700__ $$aJiggins, Stephen$$iINSPIRE-00392933$$jORCID:0000-0003-2906-1977$$uFreiburg U.
002655508 700__ $$aJimenez Morales, Fabricio Andres$$iINSPIRE-00573353$$uClermont-Ferrand U.
002655508 700__ $$aJimenez Pena, Javier$$iINSPIRE-00386283$$uValencia U., IFIC
002655508 700__ $$aJin, Shan$$iINSPIRE-00216225$$jORCID:0000-0002-5076-7803$$uNanjing U.
002655508 700__ $$aJinaru, Adam$$iINSPIRE-00349814$$uBucharest, IFIN-HH
002655508 700__ $$aJinnouchi, Osamu$$iINSPIRE-00241926$$jORCID:0000-0001-5073-0974$$uTokyo Inst. Tech.
002655508 700__ $$aJivan, Harshna$$iINSPIRE-00507050$$uWitwatersrand U.
002655508 700__ $$aJohansson, Per$$iINSPIRE-00305905$$jORCID:0000-0001-5410-1315$$uSheffield U.
002655508 700__ $$aJohns, Kenneth$$iINSPIRE-00093591$$jORCID:0000-0001-9147-6052$$uArizona U.
002655508 700__ $$aJohnson, Christian$$iINSPIRE-00512851$$jORCID:0000-0002-5387-572X$$uIndiana U.
002655508 700__ $$aJohnson, William Joseph$$iINSPIRE-00424402$$uWashington U., Seattle
002655508 700__ $$aJon-And, Kerstin$$iINSPIRE-00180510$$jORCID:0000-0001-8201-7700$$uStockholm U.$$uStockholm U., OKC
002655508 700__ $$aJones, Roger$$iINSPIRE-00216280$$jORCID:0000-0002-6427-3513$$uLancaster U.
002655508 700__ $$aJones, Samuel David$$iINSPIRE-00544715$$jORCID:0000-0003-4012-5310$$uSussex U.
002655508 700__ $$aJones, Sarah$$iINSPIRE-00439605$$jORCID:0000-0001-5748-0728$$uArizona U.
002655508 700__ $$aJones, Tim$$iINSPIRE-00227120$$uLiverpool U.
002655508 700__ $$aJongmanns, Jan$$iINSPIRE-00362112$$jORCID:0000-0002-1201-5600$$uKirchhoff Inst. Phys.
002655508 700__ $$aJorge, Pedro$$iINSPIRE-00227131$$uLIP, Lisbon$$uLisbon U., CFNUL
002655508 700__ $$aJovicevic, Jelena$$iINSPIRE-00286620$$jORCID:0000-0001-5650-4556$$uTRIUMF
002655508 700__ $$aJu, Xiangyang$$iINSPIRE-00230799$$jORCID:0000-0002-9745-1638$$uLBL, Berkeley
002655508 700__ $$aJunggeburth, Johannes Josef$$iINSPIRE-00573369$$jORCID:0000-0001-7205-1171$$uMunich, Max Planck Inst.
002655508 700__ $$aJuste Rozas, Aurelio$$iINSPIRE-00094149$$jORCID:0000-0002-1558-3291$$uBarcelona, IFAE$$uICREA, Barcelona
002655508 700__ $$aKaczmarska, Anna$$iINSPIRE-00216330$$jORCID:0000-0002-8880-4120$$uCracow, INP
002655508 700__ $$aKado, Marumi$$iINSPIRE-00216354$$uOrsay, LAL
002655508 700__ $$aKagan, Harris$$iINSPIRE-00144825$$uOhio State U.
002655508 700__ $$aKagan, Michael$$iINSPIRE-00008953$$uSLAC
002655508 700__ $$aKaji, Toshiaki$$iINSPIRE-00517162$$jORCID:0000-0002-6532-7501$$uWaseda U.
002655508 700__ $$aKajomovitz, Enrique$$iINSPIRE-00216378$$jORCID:0000-0002-8464-1790$$uTechnion
002655508 700__ $$aKalderon, Charles William$$iINSPIRE-00358313$$jORCID:0000-0002-2875-853X$$uLund U.
002655508 700__ $$aKaluza, Adam$$iINSPIRE-00375925$$uMainz U.
002655508 700__ $$aKama, Sami$$iINSPIRE-00216391$$jORCID:0000-0003-4943-8612$$uSouthern Methodist U.
002655508 700__ $$aKamenshchikov, Andrey$$iINSPIRE-00374470$$uSerpukhov, IHEP
002655508 700__ $$aKanjir, Luka$$iINSPIRE-00405560$$uStefan Inst., Ljubljana
002655508 700__ $$aKano, Yuya$$iINSPIRE-00571918$$jORCID:0000-0003-1090-3820$$uTokyo U., ICEPP
002655508 700__ $$aKantserov, Vadim$$iINSPIRE-00216415$$jORCID:0000-0001-8255-416X$$uMoscow Phys. Eng. Inst.
002655508 700__ $$aKanzaki, Junichi$$iINSPIRE-00216427$$uKEK, Tsukuba
002655508 700__ $$aKaplan, Benjamin$$iINSPIRE-00216439$$uNew York U.
002655508 700__ $$aKaplan, Laser Seymour$$iINSPIRE-00407495$$jORCID:0000-0003-2984-826X$$uWisconsin U., Madison
002655508 700__ $$aKar, Deepak$$iINSPIRE-00022031$$jORCID:0000-0002-4238-9822$$uWitwatersrand U.
002655508 700__ $$aKareem, Mohammad Jawad$$iINSPIRE-00384533$$jORCID:0000-0001-8967-1705$$uYork U., Canada
002655508 700__ $$aKarentzos, Efstathios$$iINSPIRE-00409082$$jORCID:0000-0002-1037-1206$$uNatl. Tech. U., Athens
002655508 700__ $$aKarpov, Sergey$$iINSPIRE-00236647$$jORCID:0000-0002-2230-5353$$uDubna, JINR
002655508 700__ $$aKarpova, Zoya$$iINSPIRE-00236653$$jORCID:0000-0003-0254-4629$$uDubna, JINR
002655508 700__ $$aKartvelishvili, Vakhtang$$iINSPIRE-00188948$$jORCID:0000-0002-1957-3787$$uLancaster U.
002655508 700__ $$aKaryukhin, Andrey$$iINSPIRE-00216469$$jORCID:0000-0001-9087-4315$$uSerpukhov, IHEP
002655508 700__ $$aKashif, Lashkar$$iINSPIRE-00005306$$jORCID:0000-0001-9572-6784$$uWisconsin U., Madison
002655508 700__ $$aKass, Richard$$iINSPIRE-00144848$$uOhio State U.
002655508 700__ $$aKastanas, Alex$$iINSPIRE-00216472$$jORCID:0000-0001-6945-1916$$uRoyal Inst. Tech., Stockholm
002655508 700__ $$aKataoka, Yousuke$$iINSPIRE-00216508$$uTokyo U., ICEPP
002655508 700__ $$aKato, Chikuma$$iINSPIRE-00413068$$jORCID:0000-0002-0794-4325$$uTsung-Dao Lee Inst., Shanghai$$uShanghai Jiao Tong U.
002655508 700__ $$aKatzy, Judith$$iINSPIRE-00185240$$uDESY
002655508 700__ $$aKawade, Kentaro$$iINSPIRE-00419409$$jORCID:0000-0002-7874-6107$$uKobe U.
002655508 700__ $$aKawagoe, Kiyotomo$$iINSPIRE-00095283$$jORCID:0000-0001-8882-129X$$uKyushu U.
002655508 700__ $$aKawamoto, Tatsuo$$iINSPIRE-00216510$$jORCID:0000-0002-5841-5511$$uTokyo U., ICEPP
002655508 700__ $$aKawamura, Gen$$iINSPIRE-00216521$$uGottingen U., II. Phys. Inst.
002655508 700__ $$aKay, Ellis Fawn$$iINSPIRE-00536644$$jORCID:0000-0002-6304-3230$$uLiverpool U.
002655508 700__ $$aKazanin, Vassili$$iINSPIRE-00216540$$uNovosibirsk State U.$$uNovosibirsk, IYF
002655508 700__ $$aKeeler, Richard$$iINSPIRE-00095435$$jORCID:0000-0002-0510-4189$$uVictoria U.
002655508 700__ $$aKehoe, Robert$$iINSPIRE-00095456$$jORCID:0000-0002-7101-697X$$uSouthern Methodist U.
002655508 700__ $$aKeller, John Stakely$$iINSPIRE-00334458$$jORCID:0000-0001-7140-9813$$uCarleton U.
002655508 700__ $$aKellermann, Edgar$$iINSPIRE-00534637$$uLund U.
002655508 700__ $$aKempster, Jacob Julian$$iINSPIRE-00371337$$jORCID:0000-0003-4168-3373$$uBirmingham U.
002655508 700__ $$aKendrick, James Andrew$$iINSPIRE-00540546$$jORCID:0000-0001-9845-5473$$uBirmingham U.
002655508 700__ $$aKepka, Oldrich$$iINSPIRE-00026678$$uPrague, Inst. Phys.
002655508 700__ $$aKersten, Susanne$$iINSPIRE-00095720$$uWuppertal U.
002655508 700__ $$aKersevan, Borut Paul$$iINSPIRE-00216670$$jORCID:0000-0002-4529-452X$$uStefan Inst., Ljubljana
002655508 700__ $$aKeyes, Robert$$iINSPIRE-00377077$$jORCID:0000-0002-4687-5107$$uMcGill U.
002655508 700__ $$aKhader, Mazin$$iINSPIRE-00517175$$jORCID:0000-0002-0405-4212$$uIllinois U., Urbana
002655508 700__ $$aKhalil-Zada, Farkhad$$iINSPIRE-00216693$$uBaku, Inst. Phys.
002655508 700__ $$aKhanov, Alexander$$iINSPIRE-00053352$$jORCID:0000-0001-9621-422X$$uOklahoma State U.
002655508 700__ $$aKharlamov, Alexey$$iINSPIRE-00297758$$jORCID:0000-0002-1051-3833$$uNovosibirsk State U.$$uNovosibirsk, IYF
002655508 700__ $$aKharlamova, Tatyana$$iINSPIRE-00524947$$jORCID:0000-0002-0387-6804$$uNovosibirsk State U.$$uNovosibirsk, IYF
002655508 700__ $$aKhoda, Elham E$$iINSPIRE-00585194$$jORCID:0000-0001-8720-6615$$uBritish Columbia U.
002655508 700__ $$aKhodinov, Alexander$$iINSPIRE-00216729$$jORCID:0000-0003-3551-5808$$uTomsk State U.
002655508 700__ $$aKhoo, Teng Jian$$iINSPIRE-00230858$$jORCID:0000-0002-5954-3101$$uGeneva U.
002655508 700__ $$aKhramov, Evgeniy$$iINSPIRE-00305942$$jORCID:0000-0001-7400-6454$$uDubna, JINR
002655508 700__ $$aKhubua, Jemal$$iINSPIRE-00305959$$jORCID:0000-0003-2350-1249$$uTbilisi State U.
002655508 700__ $$aKido, Shogo$$iINSPIRE-00413107$$jORCID:0000-0003-0536-5386$$uKobe U.
002655508 700__ $$aKiehn, Moritz$$iINSPIRE-00569643$$jORCID:0000-0001-9608-2626$$uGeneva U.
002655508 700__ $$aKilby, Callum Robert$$iINSPIRE-00514530$$jORCID:0000-0002-1617-5572$$uRoyal Holloway, U. of London
002655508 700__ $$aKim, Young-Kee$$iINSPIRE-00096350$$jORCID:0000-0003-3286-1326$$uChicago U., EFI
002655508 700__ $$aKimura, Naoki$$iINSPIRE-00008600$$uINFN, Udine$$uUdine U.
002655508 700__ $$aKind, Oliver$$iINSPIRE-00191251$$jORCID:0000-0002-7880-9665$$uHumboldt U., Berlin
002655508 700__ $$aKing, Barry$$iINSPIRE-00039391$$uLiverpool U.
002655508 700__ $$aKirchmeier, David$$iINSPIRE-00524951$$jORCID:0000-0001-8545-5650$$uDresden, Tech. U.
002655508 700__ $$aKirk, Julie$$iINSPIRE-00216784$$jORCID:0000-0001-8096-7577$$uRutherford
002655508 700__ $$aKiryunin, Andrey$$iINSPIRE-00216808$$jORCID:0000-0001-7490-6890$$uMunich, Max Planck Inst.
002655508 700__ $$aKishimoto, Tomoe$$iINSPIRE-00236684$$uTokyo U., ICEPP
002655508 700__ $$aKisielewska, Danuta$$iINSPIRE-00172500$$jORCID:0000-0002-8787-5736$$uAGH-UST, Cracow
002655508 700__ $$aKitali, Vincent$$iINSPIRE-00547637$$jORCID:0000-0002-6171-6059$$uDESY
002655508 700__ $$aKivernyk, Oleh$$iINSPIRE-00408270$$jORCID:0000-0002-6854-2717$$uAnnecy, LAPP
002655508 700__ $$aKladiva, Eduard$$iINSPIRE-00216810$$uKosice, IEF
002655508 700__ $$aKlapdor-kleingrothaus, Thorwald$$iINSPIRE-00534640$$jORCID:0000-0003-1423-6041$$uFreiburg U.
002655508 700__ $$aKlein, Matthew Henry$$iINSPIRE-00380915$$jORCID:0000-0002-9999-2534$$uMichigan U.
002655508 700__ $$aKlein, Max$$iINSPIRE-00096790$$jORCID:0000-0002-8527-964X$$uLiverpool U.
002655508 700__ $$aKlein, Uta$$iINSPIRE-00172660$$jORCID:0000-0001-7391-5330$$uLiverpool U.
002655508 700__ $$aKleinknecht, Konrad$$iINSPIRE-00157115$$uMainz U.
002655508 700__ $$aKlimek, Pawel$$iINSPIRE-00236698$$jORCID:0000-0003-1661-6873$$uNorthern Illinois U.
002655508 700__ $$aKlimentov, Alexei$$iINSPIRE-00216840$$uBrookhaven
002655508 700__ $$aKlingenberg, Reiner$$iINSPIRE-00189090$$uDortmund U.
002655508 700__ $$aKlingl, Tobias$$iINSPIRE-00549820$$jORCID:0000-0002-5721-9834$$uBonn U.
002655508 700__ $$aKlioutchnikova, Tatiana$$iINSPIRE-00216863$$jORCID:0000-0002-9580-0363$$uCERN
002655508 700__ $$aKlitzner, Felix Fidelio$$iINSPIRE-00569432$$uMunich U.
002655508 700__ $$aKluit, Peter$$iINSPIRE-00096892$$uFOM, Amsterdam
002655508 700__ $$aKluth, Stefan$$iINSPIRE-00096918$$uMunich, Max Planck Inst.
002655508 700__ $$aKneringer, Emmerich$$iINSPIRE-00096974$$jORCID:0000-0002-6206-1912$$uInnsbruck U.
002655508 700__ $$aKnoops, Edith B F G$$iINSPIRE-00096991$$jORCID:0000-0002-0694-0103$$uMarseille, CPPM
002655508 700__ $$aKnue, Andrea$$iINSPIRE-00230947$$jORCID:0000-0002-1559-9285$$uFreiburg U.
002655508 700__ $$aKobayashi, Aine$$iINSPIRE-00403465$$uTokyo U., ICEPP
002655508 700__ $$aKobayashi, Dai$$iINSPIRE-00374480$$uKyushu U.
002655508 700__ $$aKobayashi, Tomio$$iINSPIRE-00210282$$uTokyo U., ICEPP
002655508 700__ $$aKobel, Michael$$iINSPIRE-00097070$$jORCID:0000-0002-0124-2699$$uDresden, Tech. U.
002655508 700__ $$aKocian, Martin$$iINSPIRE-00041830$$jORCID:0000-0003-4559-6058$$uSLAC
002655508 700__ $$aKodys, Peter$$iINSPIRE-00216912$$jORCID:0000-0002-8644-2349$$uCharles U.
002655508 700__ $$aKoenig, Philipp Thomas$$iINSPIRE-00583985$$jORCID:0000-0002-0497-3550$$uBonn U.
002655508 700__ $$aKoffas, Thomas$$iINSPIRE-00218105$$jORCID:0000-0001-9612-4988$$uCarleton U.
002655508 700__ $$aKoffeman, Els$$iINSPIRE-00173731$$uFOM, Amsterdam
002655508 700__ $$aKoehler, Nicolas Maximilian$$iINSPIRE-00517182$$jORCID:0000-0002-0490-9778$$uMunich, Max Planck Inst.
002655508 700__ $$aKoi, Tatsumi$$iINSPIRE-00035594$$jORCID:0000-0003-2909-148X$$uSLAC
002655508 700__ $$aKolb, Mathis$$iINSPIRE-00417839$$jORCID:0000-0002-6117-3816$$uHeidelberg U.
002655508 700__ $$aKoletsou, Iro$$iINSPIRE-00015902$$jORCID:0000-0002-8560-8917$$uAnnecy, LAPP
002655508 700__ $$aKondo, Takahiko$$iINSPIRE-00097562$$uKEK, Tsukuba
002655508 700__ $$aKondrashova, Natalia$$iINSPIRE-00345331$$uShanghai Jiao Tong U.
002655508 700__ $$aKoeneke, Karsten$$iINSPIRE-00042236$$jORCID:0000-0002-6901-9717$$uFreiburg U.
002655508 700__ $$aKoenig, Adriaan$$iINSPIRE-00097590$$jORCID:0000-0001-6702-6473$$uNijmegen U.
002655508 700__ $$aKono, Takanori$$iINSPIRE-00218319$$jORCID:0000-0003-1553-2950$$uKEK, Tsukuba
002655508 700__ $$aKonoplich, Rostislav$$iINSPIRE-00097654$$jORCID:0000-0002-6223-7017$$uNew York U.$$uManhattan Coll., Riverdale
002655508 700__ $$aKonstantinides, Vasilis$$iINSPIRE-00586690$$uUniversity Coll. London
002655508 700__ $$aKonstantinidis, Nikolaos$$iINSPIRE-00097667$$jORCID:0000-0002-4140-6360$$uUniversity Coll. London
002655508 700__ $$aKonya, Balazs$$iINSPIRE-00543670$$jORCID:0000-0002-1859-6557$$uLund U.
002655508 700__ $$aKopeliansky, Revital$$iINSPIRE-00337069$$jORCID:0000-0002-8775-1194$$uIndiana U.
002655508 700__ $$aKoperny, Stefan$$iINSPIRE-00218320$$jORCID:0000-0002-2023-5945$$uAGH-UST, Cracow
002655508 700__ $$aKorcyl, Krzysztof$$iINSPIRE-00097773$$jORCID:0000-0001-8085-4505$$uCracow, INP
002655508 700__ $$aKordas, Konstantinos$$iINSPIRE-00218332$$jORCID:0000-0003-0486-2081$$uAristotle U., Thessaloniki
002655508 700__ $$aKoren, Guy$$iINSPIRE-00643659$$uTel Aviv U.
002655508 700__ $$aKorn, Andreas$$iINSPIRE-00052183$$jORCID:0000-0002-3962-2099$$uUniversity Coll. London
002655508 700__ $$aKorolkov, Ilya$$iINSPIRE-00097847$$uBarcelona, IFAE
002655508 700__ $$aKorolkova, Elena$$iINSPIRE-00218344$$uSheffield U.
002655508 700__ $$aKorotkova, Natalia$$iINSPIRE-00551928$$uLomonosov Moscow State U.
002655508 700__ $$aKortner, Oliver$$iINSPIRE-00218368$$jORCID:0000-0003-0352-3096$$uMunich, Max Planck Inst.
002655508 700__ $$aKortner, Sandra$$iINSPIRE-00215825$$jORCID:0000-0001-8667-1814$$uMunich, Max Planck Inst.
002655508 700__ $$aKosek, Tomas$$iINSPIRE-00364770$$jORCID:0000-0003-1639-5564$$uCharles U.
002655508 700__ $$aKostyukhin, Vadim$$iINSPIRE-00218374$$jORCID:0000-0002-0490-9209$$uBonn U.
002655508 700__ $$aKotwal, Ashutosh$$iINSPIRE-00097984$$jORCID:0000-0003-3384-5053$$uDuke U.
002655508 700__ $$aKoulouris, Aimilianos$$iINSPIRE-00524960$$jORCID:0000-0003-1012-4675$$uNatl. Tech. U., Athens
002655508 700__ $$aKourkoumeli-Charalampidi, Athina$$iINSPIRE-00365526$$jORCID:0000-0002-6614-108X$$uINFN, Pavia$$uPavia U.
002655508 700__ $$aKourkoumelis, Christine$$iINSPIRE-00218386$$jORCID:0000-0003-0083-274X$$uAthens Natl. Capodistrian U.
002655508 700__ $$aKourlitis, Evangelos$$iINSPIRE-00537788$$jORCID:0000-0001-6568-2047$$uSheffield U.
002655508 700__ $$aKouskoura, Vasiliki$$iINSPIRE-00286669$$jORCID:0000-0002-8987-3208$$uBrookhaven
002655508 700__ $$aKowalewska, Anna Bozena$$iINSPIRE-00431470$$jORCID:0000-0003-2694-5080$$uCracow, INP
002655508 700__ $$aKowalewski, Robert Victor$$iINSPIRE-00098130$$jORCID:0000-0002-7314-0990$$uVictoria U.
002655508 700__ $$aKowalski, Tadeusz$$iINSPIRE-00305987$$jORCID:0000-0001-9981-6306$$uAGH-UST, Cracow
002655508 700__ $$aKozakai, Chihiro$$iINSPIRE-00452631$$jORCID:0000-0003-2853-869X$$uTokyo U., ICEPP
002655508 700__ $$aKozanecki, Witold$$iINSPIRE-00098207$$jORCID:0000-0001-6226-8385$$uIRFU, Saclay
002655508 700__ $$aKozhin, Anatoly$$iINSPIRE-00218400$$jORCID:0000-0003-4724-9017$$uSerpukhov, IHEP
002655508 700__ $$aKramarenko, Viktor$$iINSPIRE-00218423$$uLomonosov Moscow State U.
002655508 700__ $$aKramberger, Gregor$$iINSPIRE-00098259$$uStefan Inst., Ljubljana
002655508 700__ $$aKrasnopevtsev, Dimitrii$$iINSPIRE-00349845$$jORCID:0000-0002-6356-372X$$uHefei, CUST
002655508 700__ $$aKrasny, Mieczyslaw Witold$$iINSPIRE-00218435$$uParis U., VI-VII
002655508 700__ $$aKrasznahorkay, Attila$$iINSPIRE-00218447$$uCERN
002655508 700__ $$aKrauss, Dominik$$iINSPIRE-00540551$$jORCID:0000-0002-6419-7602$$uMunich, Max Planck Inst.
002655508 700__ $$aKremer, Jakub Andrzej$$iINSPIRE-00524978$$jORCID:0000-0003-4487-6365$$uAGH-UST, Cracow
002655508 700__ $$aKretzschmar, Jan$$iINSPIRE-00185292$$jORCID:0000-0002-8515-1355$$uLiverpool U.
002655508 700__ $$aKrieger, Peter$$iINSPIRE-00195228$$jORCID:0000-0001-9958-949X$$uToronto U.
002655508 700__ $$aKrizka, Karol$$iINSPIRE-00384270$$jORCID:0000-0001-6408-2648$$uLBL, Berkeley
002655508 700__ $$aKroeninger, Kevin$$iINSPIRE-00218479$$jORCID:0000-0001-9873-0228$$uDortmund U.
002655508 700__ $$aKroha, Hubert$$iINSPIRE-00218480$$jORCID:0000-0003-1808-0259$$uMunich, Max Planck Inst.
002655508 700__ $$aKroll, Jiri$$iINSPIRE-00524985$$jORCID:0000-0001-6215-3326$$uPrague, Inst. Phys.
002655508 700__ $$aKroll, Joe$$iINSPIRE-00098670$$jORCID:0000-0002-0964-6815$$uPennsylvania U.
002655508 700__ $$aKrstic, Jelena$$iINSPIRE-00218492$$jORCID:0000-0002-1710-1524$$uBelgrade U.
002655508 700__ $$aKruchonak, Uladzimir$$iINSPIRE-00218504$$uDubna, JINR
002655508 700__ $$aKrueger, Hans$$iINSPIRE-00218516$$uBonn U.
002655508 700__ $$aKrumnack, Nils$$iINSPIRE-00055045$$uIowa State U.
002655508 700__ $$aKruse, Mark$$iINSPIRE-00098798$$jORCID:0000-0001-5791-0345$$uDuke U.
002655508 700__ $$aKubota, Takashi$$iINSPIRE-00218541$$jORCID:0000-0002-1156-5571$$uMelbourne U.
002655508 700__ $$aKuday, Sinan$$iINSPIRE-00236766$$jORCID:0000-0002-0116-5494$$uIstanbul Aydin U.
002655508 700__ $$aKuechler, Jan Thomas$$iINSPIRE-00439671$$jORCID:0000-0001-9087-6230$$uWuppertal U.
002655508 700__ $$aKuehn, Susanne$$iINSPIRE-00218553$$jORCID:0000-0001-5270-0920$$uCERN
002655508 700__ $$aKugel, Andreas$$iINSPIRE-00218560$$jORCID:0000-0002-8493-6660$$uKirchhoff Inst. Phys.
002655508 700__ $$aKuger, Fabian$$iINSPIRE-00387450$$jORCID:0000-0001-9475-3916$$uWurzburg U.
002655508 700__ $$aKuhl, Thorsten$$iINSPIRE-00051546$$jORCID:0000-0002-1473-350X$$uDESY
002655508 700__ $$aKukhtin, Victor$$iINSPIRE-00218599$$uDubna, JINR
002655508 700__ $$aKukla, Romain$$iINSPIRE-00388150$$jORCID:0000-0002-1140-2465$$uMarseille, CPPM
002655508 700__ $$aKulchitsky, Yuri$$iINSPIRE-00098974$$jORCID:0000-0002-3036-5575$$uMinsk, Inst. Phys.
002655508 700__ $$aKuleshov, Sergey$$iINSPIRE-00320322$$jORCID:0000-0002-3065-326X$$uSanta Maria U., Valparaiso
002655508 700__ $$aKulinich, Yakov Petrovich$$iINSPIRE-00517193$$uIllinois U., Urbana
002655508 700__ $$aKuna, Marine$$iINSPIRE-00218612$$jORCID:0000-0002-3598-2847$$uLPSC, Grenoble
002655508 700__ $$aKunigo, Takuto$$iINSPIRE-00381656$$jORCID:0000-0001-9613-2849$$uKyoto U.
002655508 700__ $$aKupco, Alexander$$iINSPIRE-00099163$$jORCID:0000-0003-3692-1410$$uPrague, Inst. Phys.
002655508 700__ $$aKupfer, Tobias$$iINSPIRE-00548847$$uDortmund U.
002655508 700__ $$aKuprash, Oleg$$iINSPIRE-00173407$$jORCID:0000-0002-7540-0012$$uTel Aviv U.
002655508 700__ $$aKurashige, Hisaya$$iINSPIRE-00099197$$jORCID:0000-0003-3932-016X$$uKobe U.
002655508 700__ $$aKurchaninov, Leonid$$iINSPIRE-00524990$$jORCID:0000-0001-9392-3936$$uTRIUMF
002655508 700__ $$aKurochkin, Yurii$$iINSPIRE-00218636$$uMinsk, Inst. Phys.
002655508 700__ $$aKurth, Matthew Glenn$$iINSPIRE-00537264$$uBeijing, GUCAS
002655508 700__ $$aKuwertz, Emma Sian$$iINSPIRE-00286685$$jORCID:0000-0002-1921-6173$$uCERN
002655508 700__ $$aKuze, Masahiro$$iINSPIRE-00099360$$jORCID:0000-0001-8858-8440$$uTokyo Inst. Tech.
002655508 700__ $$aKvita, Jiri$$iINSPIRE-00038915$$uPalacky U.
002655508 700__ $$aKwan, Tony$$iINSPIRE-00379325$$jORCID:0000-0001-8717-4449$$uMcGill U.
002655508 700__ $$aLa Rosa, Alessandro$$iINSPIRE-00218666$$jORCID:0000-0001-6291-2142$$uMunich, Max Planck Inst.
002655508 700__ $$aLa Rosa Navarro, Jose Luis$$iINSPIRE-00379447$$uSao Paulo U.
002655508 700__ $$aLa Rotonda, Laura$$iINSPIRE-00218678$$jORCID:0000-0002-6780-5829$$uINFN, Cosenza$$uCalabria U.
002655508 700__ $$aLa Ruffa, Francesco$$iINSPIRE-00551932$$jORCID:0000-0001-6104-1189$$uINFN, Cosenza$$uCalabria U.
002655508 700__ $$aLacasta, Carlos$$iINSPIRE-00099524$$jORCID:0000-0002-2623-6252$$uValencia U., IFIC
002655508 700__ $$aLacava, Francesco$$iINSPIRE-00218690$$jORCID:0000-0003-4588-8325$$uINFN, Rome$$uRome U.
002655508 700__ $$aLacey, James$$iINSPIRE-00334483$$uDESY
002655508 700__ $$aLack, David Philip John$$iINSPIRE-00536653$$jORCID:0000-0003-4829-5824$$uManchester U.
002655508 700__ $$aLacker, Heiko$$iINSPIRE-00042702$$jORCID:0000-0002-7183-8607$$uHumboldt U., Berlin
002655508 700__ $$aLacour, Didier$$iINSPIRE-00099578$$jORCID:0000-0002-1590-194X$$uParis U., VI-VII
002655508 700__ $$aLadygin, Evgueni$$iINSPIRE-00099592$$uDubna, JINR
002655508 700__ $$aLafaye, Remi$$iINSPIRE-00218717$$jORCID:0000-0001-7848-6088$$uAnnecy, LAPP
002655508 700__ $$aLaforge, Bertrand$$iINSPIRE-00057788$$jORCID:0000-0002-4209-4194$$uParis U., VI-VII
002655508 700__ $$aLagouri, Theodota$$iINSPIRE-00218740$$jORCID:0000-0001-7509-7765$$uWitwatersrand U.
002655508 700__ $$aLai, Stanley$$iINSPIRE-00218758$$jORCID:0000-0002-9898-9253$$uGottingen U., II. Phys. Inst.
002655508 700__ $$aLammers, Sabine$$iINSPIRE-00051670$$uIndiana U.
002655508 700__ $$aLampl, Walter$$iINSPIRE-00218776$$jORCID:0000-0002-2337-0958$$uArizona U.
002655508 700__ $$aLancon, Eric$$iINSPIRE-00218788$$jORCID:0000-0002-0225-187X$$uBrookhaven
002655508 700__ $$aLandgraf, Ulrich$$iINSPIRE-00218790$$jORCID:0000-0002-8222-2066$$uFreiburg U.
002655508 700__ $$aLandon, Murrough$$iINSPIRE-00099860$$jORCID:0000-0001-6828-9769$$uQueen Mary, U. of London
002655508 700__ $$aLanfermann, Marie Christine$$iINSPIRE-00508917$$jORCID:0000-0002-2938-2757$$uGeneva U.
002655508 700__ $$aLang, Valerie Susanne$$iINSPIRE-00286700$$jORCID:0000-0001-9954-7898$$uDESY
002655508 700__ $$aLange, Joern Christian$$iINSPIRE-00397348$$jORCID:0000-0003-1307-1441$$uBarcelona, IFAE
002655508 700__ $$aLangenberg, Robert Johannes$$iINSPIRE-00551027$$jORCID:0000-0001-6595-1382$$uCERN
002655508 700__ $$aLankford, Andrew$$iINSPIRE-00100028$$jORCID:0000-0001-8057-4351$$uUC, Irvine
002655508 700__ $$aLanni, Francesco$$iINSPIRE-00100030$$jORCID:0000-0002-7197-9645$$uBrookhaven
002655508 700__ $$aLantzsch, Kerstin$$iINSPIRE-00218824$$uBonn U.
002655508 700__ $$aLanza, Agostino$$iINSPIRE-00218836$$jORCID:0000-0003-4980-6032$$uINFN, Pavia
002655508 700__ $$aLapertosa, Alessandro$$iINSPIRE-00536668$$jORCID:0000-0001-6246-6787$$uINFN, Genoa$$uGenoa U.
002655508 700__ $$aLaplace, Sandrine$$iINSPIRE-00032441$$jORCID:0000-0003-3526-6258$$uParis U., VI-VII
002655508 700__ $$aLaporte, Jean-Francois$$iINSPIRE-00218850$$jORCID:0000-0002-4815-5314$$uIRFU, Saclay
002655508 700__ $$aLari, Tommaso$$iINSPIRE-00240476$$jORCID:0000-0002-1388-869X$$uINFN, Milan
002655508 700__ $$aLasagni Manghi, Federico$$iINSPIRE-00378808$$jORCID:0000-0001-6068-4473$$uINFN, Bologna$$uBologna U.
002655508 700__ $$aLassnig, Mario$$iINSPIRE-00218873$$jORCID:0000-0002-9541-0592$$uCERN
002655508 700__ $$aLau, Tak Shun$$iINSPIRE-00569441$$uHong Kong, Chinese U.
002655508 700__ $$aLaudrain, Antoine$$iINSPIRE-00573375$$jORCID:0000-0001-6098-0555$$uOrsay, LAL
002655508 700__ $$aLavorgna, Marco$$iINSPIRE-00641146$$jORCID:0000-0002-3407-752X$$uINFN, Naples$$uNaples U.
002655508 700__ $$aLaw, Alexander Thomas$$iINSPIRE-00348140$$uUC, Santa Cruz
002655508 700__ $$aLaycock, Paul$$iINSPIRE-00037318$$jORCID:0000-0002-8572-5339$$uLiverpool U.
002655508 700__ $$aLazzaroni, Massimo$$iINSPIRE-00445566$$jORCID:0000-0002-4094-1273$$uINFN, Milan$$uMilan U.
002655508 700__ $$aLe, Brian$$iINSPIRE-00507250$$uMelbourne U.
002655508 700__ $$aLe Dortz, Olivier$$iINSPIRE-00218897$$uParis U., VI-VII
002655508 700__ $$aLe Guirriec, Emmanuel$$iINSPIRE-00218909$$jORCID:0000-0001-5227-6736$$uMarseille, CPPM
002655508 700__ $$aLe Quilleuc, Eloi Paul$$iINSPIRE-00439709$$uIRFU, Saclay
002655508 700__ $$aLeblanc, Matthew Edgar$$iINSPIRE-00397460$$jORCID:0000-0001-5977-6418$$uArizona U.
002655508 700__ $$aLeCompte, Thomas$$iINSPIRE-00100495$$jORCID:0000-0002-9450-6568$$uArgonne
002655508 700__ $$aLedroit-Guillon, Fabienne$$iINSPIRE-00200437$$jORCID:0000-0001-9398-1909$$uLPSC, Grenoble
002655508 700__ $$aLee, Claire Alexandra$$iINSPIRE-00048758$$jORCID:0000-0001-6113-0982$$uBrookhaven
002655508 700__ $$aLee, Graham Richard$$iINSPIRE-00361302$$uChile U., Catolica
002655508 700__ $$aLee JR, Lawrence$$iINSPIRE-00231146$$jORCID:0000-0002-5590-335X$$uHarvard U., Phys. Dept.
002655508 700__ $$aLee, Shih-Chang$$iINSPIRE-00100720$$jORCID:0000-0002-3353-2658$$uTaiwan, Inst. Phys.
002655508 700__ $$aLefebvre, Benoit$$iINSPIRE-00426582$$jORCID:0000-0001-8212-6624$$uMcGill U.
002655508 700__ $$aLefebvre, Michel$$iINSPIRE-00198481$$jORCID:0000-0002-5560-0586$$uVictoria U.
002655508 700__ $$aLegger, Federica$$iINSPIRE-00218990$$jORCID:0000-0003-1400-0709$$uMunich U.
002655508 700__ $$aLeggett, Charles$$iINSPIRE-00100895$$jORCID:0000-0002-9299-9020$$uLBL, Berkeley
002655508 700__ $$aLehmann, Konstantin$$iINSPIRE-00642180$$jORCID:0000-0002-8590-8231$$uSimon Fraser U.
002655508 700__ $$aLehmann, Niklaus$$iINSPIRE-00545897$$jORCID:0000-0001-5521-1655$$uWuppertal U.
002655508 700__ $$aLehmann Miotto, Giovanna$$iINSPIRE-00100928$$jORCID:0000-0001-9045-7853$$uCERN
002655508 700__ $$aLeight, William Axel$$iINSPIRE-00182253$$jORCID:0000-0002-2968-7841$$uDESY
002655508 700__ $$aLeisos, Antonios$$iINSPIRE-00236807$$jORCID:0000-0002-8126-3958$$uAristotle U., Thessaloniki$$uHellenic Open U., Patras
002655508 700__ $$aLeite, Marco Aurelio Lisboa$$iINSPIRE-00242334$$uSao Paulo U.
002655508 700__ $$aLeitner, Rupert$$iINSPIRE-00301106$$jORCID:0000-0002-2994-2187$$uCharles U.
002655508 700__ $$aLellouch, Daniel$$iINSPIRE-00101050$$jORCID:0000-0002-2330-765X$$uWeizmann Inst.
002655508 700__ $$aLemmer, Boris$$iINSPIRE-00236819$$uGottingen U., II. Phys. Inst.
002655508 700__ $$aLeney, Katharine$$iINSPIRE-00192210$$jORCID:0000-0002-1525-2695$$uUniversity Coll. London
002655508 700__ $$aLenz, Tatjana$$iINSPIRE-00219020$$jORCID:0000-0002-9560-1778$$uBonn U.
002655508 700__ $$aLenzi, Bruno$$iINSPIRE-00242346$$jORCID:0000-0002-1024-4004$$uCERN
002655508 700__ $$aLeone, Robert$$iINSPIRE-00263632$$jORCID:0000-0002-2311-3847$$uArizona U.
002655508 700__ $$aLeone, Sandra$$iINSPIRE-00101163$$jORCID:0000-0001-6222-9642$$uINFN, Pisa
002655508 700__ $$aLeonidopoulos, Christos$$iINSPIRE-00101179$$jORCID:0000-0002-7241-2114$$uEdinburgh U.
002655508 700__ $$aLerner, Giuseppe$$iINSPIRE-00442062$$jORCID:0000-0002-0976-4993$$uSussex U.
002655508 700__ $$aLeroy, Claude$$iINSPIRE-00149161$$jORCID:0000-0003-3105-7045$$uMontreal U.
002655508 700__ $$aLes, Robert$$iINSPIRE-00565690$$jORCID:0000-0002-8875-1399$$uToronto U.
002655508 700__ $$aLesage, Arthur$$iINSPIRE-00439764$$jORCID:0000-0001-6645-1005$$uIRFU, Saclay
002655508 700__ $$aLester, Christopher$$iINSPIRE-00101328$$jORCID:0000-0001-5770-4883$$uCambridge U.
002655508 700__ $$aLevchenko, Mikhail$$iINSPIRE-00358155$$jORCID:0000-0002-5495-0656$$uSt. Petersburg, INP
002655508 700__ $$aLeveque, Jessica$$iINSPIRE-00038900$$jORCID:0000-0002-0244-4743$$uAnnecy, LAPP
002655508 700__ $$aLevin, Daniel$$iINSPIRE-00101433$$uMichigan U.
002655508 700__ $$aLevinson, Lorne$$iINSPIRE-00101477$$jORCID:0000-0003-4679-0485$$uWeizmann Inst.
002655508 700__ $$aLewis, Dave$$iINSPIRE-00443670$$uQueen Mary, U. of London
002655508 700__ $$aLi, Bing$$iINSPIRE-00329518$$jORCID:0000-0002-1974-2229$$uMichigan U.
002655508 700__ $$aLi, Changqiao$$iINSPIRE-00512869$$jORCID:0000-0003-3495-7778$$uHefei, CUST$$uParis U., VI-VII
002655508 700__ $$aLi, Haifeng$$iINSPIRE-00219079$$jORCID:0000-0001-9346-6982$$uShandong U.
002655508 700__ $$aLi, Liang$$iINSPIRE-00300470$$jORCID:0000-0001-6411-6107$$uShanghai Jiao Tong U.
002655508 700__ $$aLi, Qi$$iINSPIRE-00439752$$uBeijing, GUCAS
002655508 700__ $$aLi, Quanyin$$iINSPIRE-00465217$$uHefei, CUST
002655508 700__ $$aLi, Shu$$iINSPIRE-00231230$$jORCID:0000-0001-7879-3272$$uTsung-Dao Lee Inst., Shanghai$$uShanghai Jiao Tong U.
002655508 700__ $$aLi, Xingguo$$iINSPIRE-00388243$$jORCID:0000-0001-6975-102X$$uShanghai Jiao Tong U.
002655508 700__ $$aLi, Yichen$$iINSPIRE-00364274$$uSiegen U.
002655508 700__ $$aLiang, Zhijun$$iINSPIRE-00219122$$jORCID:0000-0003-0629-2131$$uBeijing, Inst. High Energy Phys.
002655508 700__ $$aLiberti, Barbara$$iINSPIRE-00219134$$jORCID:0000-0002-6011-2851$$uINFN, Rome2
002655508 700__ $$aLiblong, Aaron$$iINSPIRE-00392999$$jORCID:0000-0003-2909-7144$$uToronto U.
002655508 700__ $$aLie, Ki$$iINSPIRE-00219158$$jORCID:0000-0002-5779-5989$$uHong Kong U. Sci. Tech.
002655508 700__ $$aLiem Arvidsson, Sebastian$$iINSPIRE-00571509$$uFOM, Amsterdam
002655508 700__ $$aLimosani, Antonio$$iINSPIRE-00219183$$jORCID:0000-0001-5675-8345$$uSydney U.
002655508 700__ $$aLin, Chiao-ying$$iINSPIRE-00452793$$jORCID:0000-0002-6350-8915$$uCambridge U.
002655508 700__ $$aLin, Kuan-yu$$iINSPIRE-00565011$$jORCID:0000-0002-2269-3632$$uMichigan State U.
002655508 700__ $$aLin, Tai-hua$$iINSPIRE-00368490$$uMainz U.
002655508 700__ $$aLinck, Rebecca Anne$$iINSPIRE-00534651$$uIndiana U.
002655508 700__ $$aLindon, Jack Henry$$iINSPIRE-00643674$$uBirmingham U.
002655508 700__ $$aLindquist, Brian Edward$$iINSPIRE-00016188$$uSUNY, Stony Brook
002655508 700__ $$aLionti, Anthony Eric$$iINSPIRE-00443766$$jORCID:0000-0002-0526-9602$$uGeneva U.
002655508 700__ $$aLipeles, Elliot$$iINSPIRE-00102076$$jORCID:0000-0001-5982-7326$$uPennsylvania U.
002655508 700__ $$aLipniacka, Anna$$iINSPIRE-00219225$$jORCID:0000-0002-8759-8564$$uBergen U.
002655508 700__ $$aLisovyi, Mykhailo$$iINSPIRE-00172687$$jORCID:0000-0002-3014-5855$$uHeidelberg U.
002655508 700__ $$aLiss, Tony$$iINSPIRE-00102136$$jORCID:0000-0002-1735-3924$$uIllinois U., Urbana$$uCity Coll., N.Y.
002655508 700__ $$aLister, Alison$$iINSPIRE-00149260$$jORCID:0000-0002-1552-3651$$uBritish Columbia U.
002655508 700__ $$aLitke, Alan$$iINSPIRE-00219237$$jORCID:0000-0003-3973-3642$$uUC, Santa Cruz
002655508 700__ $$aLittle, Jared David$$iINSPIRE-00567137$$jORCID:0000-0002-9372-0730$$uTexas U., Arlington
002655508 700__ $$aLiu, Bo$$iINSPIRE-00354242$$jORCID:0000-0003-2823-9307$$uIowa State U.
002655508 700__ $$aLiu, Bingxuan$$iINSPIRE-00354011$$jORCID:0000-0002-0721-8331$$uArgonne
002655508 700__ $$aLiu, Hongbin$$iINSPIRE-00445642$$uBrookhaven
002655508 700__ $$aLiu, Hao$$iINSPIRE-00407622$$uMichigan U.
002655508 700__ $$aLiu, Jianbei$$iINSPIRE-00219262$$jORCID:0000-0003-3259-8775$$uHefei, CUST
002655508 700__ $$aLiu, Jesse Kar Kee$$iINSPIRE-00547644$$jORCID:0000-0001-5359-4541$$uOxford U.
002655508 700__ $$aLiu, Kun$$iINSPIRE-00337073$$jORCID:0000-0001-5807-0501$$uParis U., VI-VII
002655508 700__ $$aLiu, Minghui$$iINSPIRE-00219274$$jORCID:0000-0003-0056-7296$$uHefei, CUST
002655508 700__ $$aLiu, Peilian$$iINSPIRE-00455463$$jORCID:0000-0002-9815-8898$$uLBL, Berkeley
002655508 700__ $$aLiu, Yang$$iINSPIRE-00585827$$uBeijing, Inst. High Energy Phys.
002655508 700__ $$aLiu, Yanlin$$iINSPIRE-00436733$$jORCID:0000-0001-9190-4547$$uHefei, CUST
002655508 700__ $$aLiu, Yanwen$$iINSPIRE-00034400$$jORCID:0000-0003-4448-4679$$uHefei, CUST
002655508 700__ $$aLivan, Michele$$iINSPIRE-00102290$$jORCID:0000-0002-5877-0062$$uINFN, Pavia$$uPavia U.
002655508 700__ $$aLleres, Annick$$iINSPIRE-00300681$$jORCID:0000-0003-1769-8524$$uLPSC, Grenoble
002655508 700__ $$aLlorente Merino, Javier$$iINSPIRE-00236900$$jORCID:0000-0003-0027-7969$$uBeijing, Inst. High Energy Phys.
002655508 700__ $$aLloyd, Stephen$$iINSPIRE-00102350$$jORCID:0000-0002-5073-2264$$uQueen Mary, U. of London
002655508 700__ $$aLo, Cheuk Yee$$iINSPIRE-00436780$$jORCID:0000-0001-7028-5644$$uHong Kong U.
002655508 700__ $$aLo Sterzo, Francesco$$iINSPIRE-00286726$$jORCID:0000-0002-5048-6198$$uSouthern Methodist U.
002655508 700__ $$aLobodzinska, Ewelina$$iINSPIRE-00172692$$jORCID:0000-0001-9012-3431$$uDESY
002655508 700__ $$aLoch, Peter$$iINSPIRE-00102360$$jORCID:0000-0002-2005-671X$$uArizona U.
002655508 700__ $$aLohse, Thomas$$iINSPIRE-00219316$$jORCID:0000-0002-9751-7633$$uHumboldt U., Berlin
002655508 700__ $$aLohwasser, Kristin$$iINSPIRE-00219328$$jORCID:0000-0003-1833-9160$$uSheffield U.
002655508 700__ $$aLokajicek, Milos$$iINSPIRE-00278790$$jORCID:0000-0001-8929-1243$$uPrague, Inst. Phys.
002655508 700__ $$aLong, Brian Alexander$$iINSPIRE-00371005$$uBoston U.
002655508 700__ $$aLong, Jonathan$$iINSPIRE-00349854$$jORCID:0000-0002-2115-9382$$uIllinois U., Urbana
002655508 700__ $$aLong, Robin Eamonn$$iINSPIRE-00219330$$jORCID:0000-0003-2249-645X$$uLancaster U.
002655508 700__ $$aLongo, Luigi$$iINSPIRE-00298644$$jORCID:0000-0002-2357-7043$$uINFN, Lecce$$uSalento U.
002655508 700__ $$aLooper, Kristina Anne$$iINSPIRE-00390156$$jORCID:0000-0001-9198-6001$$uOhio State U.
002655508 700__ $$aLopez Lopez, Jorge Andres$$iINSPIRE-00511724$$jORCID:0000-0002-5648-4206$$uSanta Maria U., Valparaiso
002655508 700__ $$aLopez Paz, Ivan$$iINSPIRE-00372192$$uBarcelona, IFAE
002655508 700__ $$aLopez Solis, Alvaro$$iINSPIRE-00439816$$uSheffield U.
002655508 700__ $$aLorenz, Jeanette$$iINSPIRE-00236914$$jORCID:0000-0001-6530-1873$$uMunich U.
002655508 700__ $$aLorenzo Martinez, Narei$$iINSPIRE-00236921$$jORCID:0000-0002-7857-7606$$uAnnecy, LAPP
002655508 700__ $$aLosada, Marta$$iINSPIRE-00102690$$jORCID:0000-0001-8374-5806$$uAntonio Narino U.
002655508 700__ $$aLosel, Philipp Jonathan$$iINSPIRE-00389527$$uMunich U.
002655508 700__ $$aLoesle, Alena$$iINSPIRE-00580952$$jORCID:0000-0002-6328-8561$$uFreiburg U.
002655508 700__ $$aLou, Xuanhong$$iINSPIRE-00575766$$jORCID:0000-0002-8309-5548$$uDESY
002655508 700__ $$aLou, Xinchou$$iINSPIRE-00102733$$jORCID:0000-0003-0867-2189$$uBeijing, Inst. High Energy Phys.
002655508 700__ $$aLounis, Abdenour$$iINSPIRE-00219420$$jORCID:0000-0003-4066-2087$$uOrsay, LAL
002655508 700__ $$aLove, Jeremy$$iINSPIRE-00007273$$jORCID:0000-0001-7743-3849$$uArgonne
002655508 700__ $$aLove, Peter$$iINSPIRE-00006364$$jORCID:0000-0002-7803-6674$$uLancaster U.
002655508 700__ $$aLozano Bahilo, Jose Julio$$iINSPIRE-00152017$$jORCID:0000-0003-0613-140X$$uValencia U., IFIC
002655508 700__ $$aLu, Haonan$$iINSPIRE-00436841$$uHong Kong, Chinese U.
002655508 700__ $$aLu, Miaoran$$iINSPIRE-00465231$$jORCID:0000-0001-7610-3952$$uHefei, CUST
002655508 700__ $$aLu, Nan$$iINSPIRE-00378788$$jORCID:0000-0002-2631-6770$$uMichigan U.
002655508 700__ $$aLu, Yun-Ju$$iINSPIRE-00191837$$uTaiwan, Natl. Tsing Hua U.
002655508 700__ $$aLubatti, Henry$$iINSPIRE-00102893$$uWashington U., Seattle
002655508 700__ $$aLuci, Claudio$$iINSPIRE-00102930$$jORCID:0000-0001-7464-304X$$uINFN, Rome$$uRome U.
002655508 700__ $$aLucotte, Arnaud$$iINSPIRE-00102945$$jORCID:0000-0002-5992-0640$$uLPSC, Grenoble
002655508 700__ $$aLuedtke, Christian$$iINSPIRE-00418008$$uFreiburg U.
002655508 700__ $$aLuehring, Fred$$iINSPIRE-00102988$$jORCID:0000-0001-8721-6901$$uIndiana U.
002655508 700__ $$aLuise, Ilaria$$iINSPIRE-00577491$$jORCID:0000-0001-5028-3342$$uParis U., VI-VII
002655508 700__ $$aLuminari, Lamberto$$iINSPIRE-00219493$$uINFN, Rome
002655508 700__ $$aLund-Jensen, Bengt$$iINSPIRE-00103080$$jORCID:0000-0003-3867-0336$$uRoyal Inst. Tech., Stockholm
002655508 700__ $$aLutz, Margaret Susan$$iINSPIRE-00560823$$jORCID:0000-0003-4515-0224$$uMassachusetts U., Amherst
002655508 700__ $$aLuzi, Pierre Marc$$iINSPIRE-00442158$$uParis U., VI-VII
002655508 700__ $$aLynn, David$$iINSPIRE-00219523$$uBrookhaven
002655508 700__ $$aLysak, Roman$$iINSPIRE-00040995$$jORCID:0000-0003-2990-1673$$uPrague, Inst. Phys.
002655508 700__ $$aLytken, Else$$iINSPIRE-00040983$$jORCID:0000-0002-8141-3995$$uLund U.
002655508 700__ $$aLyu, Feng$$iINSPIRE-00227256$$uBeijing, Inst. High Energy Phys.
002655508 700__ $$aLyubushkin, Vladimir$$iINSPIRE-00056876$$jORCID:0000-0003-0136-233X$$uDubna, JINR
002655508 700__ $$aMa, Hong$$iINSPIRE-00103432$$jORCID:0000-0002-8916-6220$$uBrookhaven
002655508 700__ $$aMa, LianLiang$$iINSPIRE-00219535$$uShandong U.
002655508 700__ $$aMa, Yanhui$$iINSPIRE-00445756$$uShandong U.
002655508 700__ $$aMaccarrone, Giovanni$$iINSPIRE-00219559$$jORCID:0000-0002-7234-9522$$uFrascati
002655508 700__ $$aMacchiolo, Anna$$iINSPIRE-00219560$$jORCID:0000-0003-0199-6957$$uMunich, Max Planck Inst.
002655508 700__ $$aMacdonald, Calum Michael$$iINSPIRE-00389031$$jORCID:0000-0001-7857-9188$$uSheffield U.
002655508 700__ $$aMachado Miguens, Joana$$iINSPIRE-00219584$$jORCID:0000-0003-3076-5066$$uPennsylvania U.$$uLisbon U., CFNUL
002655508 700__ $$aMadaffari, Daniele$$iINSPIRE-00358553$$jORCID:0000-0002-8987-223X$$uValencia U., IFIC
002655508 700__ $$aMadar, Romain$$iINSPIRE-00301124$$jORCID:0000-0002-6875-6408$$uClermont-Ferrand U.
002655508 700__ $$aMader, Wolfgang$$iINSPIRE-00103627$$jORCID:0000-0003-4276-1046$$uDresden, Tech. U.
002655508 700__ $$aMadsen, Alexander$$iINSPIRE-00333100$$uDESY
002655508 700__ $$aMadysa, Nico$$iINSPIRE-00567140$$jORCID:0000-0001-8375-7532$$uDresden, Tech. U.
002655508 700__ $$aMaeda, Jumpei$$iINSPIRE-00030940$$jORCID:0000-0002-9084-3305$$uKobe U.
002655508 700__ $$aMaekawa, Koki$$iINSPIRE-00639220$$uTokyo U., ICEPP
002655508 700__ $$aMaeland, Steffen$$iINSPIRE-00389670$$uBergen U.
002655508 700__ $$aMaeno, Tadashi$$iINSPIRE-00219608$$jORCID:0000-0003-0901-1817$$uBrookhaven
002655508 700__ $$aMaevskiy, Artem$$iINSPIRE-00377096$$jORCID:0000-0003-1652-8005$$uLomonosov Moscow State U.
002655508 700__ $$aMagerl, Veronika$$iINSPIRE-00560836$$jORCID:0000-0003-0693-793X$$uFreiburg U.
002655508 700__ $$aMaidantchik, Carmen$$iINSPIRE-00219677$$jORCID:0000-0002-3511-0133$$uRio de Janeiro Federal U.
002655508 700__ $$aMaier, Thomas$$iINSPIRE-00393059$$uMunich U.
002655508 700__ $$aMaio, Amelia$$iINSPIRE-00219689$$jORCID:0000-0001-9099-0009$$uLIP, Lisbon$$uLisbon U., CFNUL
002655508 700__ $$aMajersky, Oliver$$iINSPIRE-00485315$$jORCID:0000-0001-8857-5770$$uComenius U.
002655508 700__ $$aMajewski, Stephanie$$iINSPIRE-00041779$$jORCID:0000-0002-6871-3395$$uOregon U.
002655508 700__ $$aMakida, Yasuhiro$$iINSPIRE-00219690$$uKEK, Tsukuba
002655508 700__ $$aMakovec, Nikola$$iINSPIRE-00006510$$jORCID:0000-0001-5124-904X$$uOrsay, LAL
002655508 700__ $$aMalaescu, Bogdan$$iINSPIRE-00144706$$uParis U., VI-VII
002655508 700__ $$aMalecki, Pawel$$iINSPIRE-00219707$$jORCID:0000-0001-8183-0468$$uCracow, INP
002655508 700__ $$aMaleev, Victor$$iINSPIRE-00219720$$jORCID:0000-0003-1028-8602$$uSt. Petersburg, INP
002655508 700__ $$aMalek, Fairouz$$iINSPIRE-00104125$$jORCID:0000-0002-0948-5775$$uLPSC, Grenoble
002655508 700__ $$aMallik, Usha$$iINSPIRE-00104172$$jORCID:0000-0001-7934-1649$$uIowa U.
002655508 700__ $$aMalon, David$$iINSPIRE-00219732$$jORCID:0000-0002-9819-3888$$uArgonne
002655508 700__ $$aMalone, Claire$$iINSPIRE-00439828$$uCambridge U.
002655508 700__ $$aMaltezos, Stavros$$iINSPIRE-00219744$$uNatl. Tech. U., Athens
002655508 700__ $$aMalyukov, Sergei$$iINSPIRE-00219768$$uCERN
002655508 700__ $$aMamuzic, Judita$$iINSPIRE-00219793$$jORCID:0000-0002-3203-4243$$uValencia U., IFIC
002655508 700__ $$aMancini, Giada$$iINSPIRE-00389811$$jORCID:0000-0001-6158-2751$$uFrascati
002655508 700__ $$aMandic, Igor$$iINSPIRE-00219818$$jORCID:0000-0002-0131-7523$$uStefan Inst., Ljubljana
002655508 700__ $$aManeira, Jose$$iINSPIRE-00219831$$jORCID:0000-0002-3222-2738$$uLIP, Lisbon
002655508 700__ $$aManhaes de Andrade Filho, Luciano$$iINSPIRE-00236954$$jORCID:0000-0003-1792-6793$$uJuiz de Fora U.
002655508 700__ $$aManjarres Ramos, Joany Andreina$$iINSPIRE-00332115$$jORCID:0000-0003-3896-5222$$uDresden, Tech. U.
002655508 700__ $$aMankinen, Katja Hannele$$iINSPIRE-00551914$$jORCID:0000-0001-7357-9648$$uLund U.
002655508 700__ $$aMann, Alexander$$iINSPIRE-00219853$$uMunich U.
002655508 700__ $$aManousos, Athanasios$$iINSPIRE-00508922$$jORCID:0000-0003-4627-4026$$uInnsbruck U.
002655508 700__ $$aMansoulie, Bruno$$iINSPIRE-00104458$$jORCID:0000-0001-5945-5518$$uIRFU, Saclay
002655508 700__ $$aMansour, Jason Dhia$$iINSPIRE-00281038$$uBeijing, Inst. High Energy Phys.
002655508 700__ $$aMantoani, Matteo$$iINSPIRE-00384468$$uGottingen U., II. Phys. Inst.
002655508 700__ $$aManzoni, Stefano$$iINSPIRE-00436885$$jORCID:0000-0002-2488-0511$$uINFN, Milan$$uMilan U.
002655508 700__ $$aMarceca, Gino$$iINSPIRE-00443931$$jORCID:0000-0002-8850-614X$$uBuenos Aires U.
002655508 700__ $$aMarch Ruiz, Luis$$iINSPIRE-00219890$$jORCID:0000-0002-0849-2244$$uGeneva U.
002655508 700__ $$aMarchese, Luigi$$iINSPIRE-00377884$$jORCID:0000-0001-6627-8716$$uOxford U.
002655508 700__ $$aMarchiori, Giovanni$$iINSPIRE-00041986$$jORCID:0000-0003-2655-7643$$uParis U., VI-VII
002655508 700__ $$aMarcisovsky, Michal$$iINSPIRE-00021119$$jORCID:0000-0003-0860-7897$$uPrague, Inst. Phys.
002655508 700__ $$aMarin Tobon, Cesar Augusto$$iINSPIRE-00434175$$jORCID:0000-0001-7853-6620$$uCERN
002655508 700__ $$aMarjanovic, Marija$$iINSPIRE-00355110$$jORCID:0000-0002-4468-0154$$uClermont-Ferrand U.
002655508 700__ $$aMarley, Daniel Edison$$iINSPIRE-00407608$$uMichigan U.
002655508 700__ $$aMarroquim, Fernando$$iINSPIRE-00195269$$jORCID:0000-0003-2265-784X$$uRio de Janeiro Federal U.
002655508 700__ $$aMarshall, Zach$$iINSPIRE-00219927$$jORCID:0000-0003-0786-2570$$uLBL, Berkeley
002655508 700__ $$aMartensson, Ulf Fredrik Mikael$$iINSPIRE-00530554$$jORCID:0000-0002-7288-3610$$uUppsala U., Inst. Theor. Phys.
002655508 700__ $$aMarti i Garcia, Salvador$$iINSPIRE-00050327$$jORCID:0000-0002-3897-6223$$uValencia U., IFIC
002655508 700__ $$aMartin, Christopher Blake$$iINSPIRE-00374510$$jORCID:0000-0002-4345-5051$$uOhio State U.
002655508 700__ $$aMartin, Tim$$iINSPIRE-00219969$$jORCID:0000-0002-1477-1645$$uWarwick U.
002655508 700__ $$aMartin, Victoria Jane$$iINSPIRE-00105165$$jORCID:0000-0003-3053-8146$$uEdinburgh U.
002655508 700__ $$aMartin dit Latour, Bertrand$$iINSPIRE-00001472$$jORCID:0000-0003-3420-2105$$uBergen U.
002655508 700__ $$aMartinez Perez, Mario$$iINSPIRE-00105204$$jORCID:0000-0002-3135-945X$$uBarcelona, IFAE$$uICREA, Barcelona
002655508 700__ $$aMartinez Outschoorn, Verena$$iINSPIRE-00256761$$jORCID:0000-0001-7102-6388$$uMassachusetts U., Amherst
002655508 700__ $$aMartin-Haugh, Stewart$$iINSPIRE-00236968$$jORCID:0000-0001-9457-1928$$uRutherford
002655508 700__ $$aMartoiu, Victor Sorin$$iINSPIRE-00388336$$jORCID:0000-0002-4963-9441$$uBucharest, IFIN-HH
002655508 700__ $$aMartyniuk, Alex$$iINSPIRE-00219970$$jORCID:0000-0001-9080-2944$$uUniversity Coll. London
002655508 700__ $$aMarzin, Antoine$$iINSPIRE-00220006$$jORCID:0000-0003-4364-4351$$uCERN
002655508 700__ $$aMasetti, Lucia$$iINSPIRE-00220018$$jORCID:0000-0002-0038-5372$$uMainz U.
002655508 700__ $$aMashimo, Tetsuro$$iINSPIRE-00220020$$jORCID:0000-0001-5333-6016$$uTokyo U., ICEPP
002655508 700__ $$aMashinistov, Ruslan$$iINSPIRE-00220031$$jORCID:0000-0001-7925-4676$$uLebedev Inst.
002655508 700__ $$aMasik, Jiri$$iINSPIRE-00220043$$jORCID:0000-0002-6813-8423$$uManchester U.
002655508 700__ $$aMaslennikov, Alexey$$iINSPIRE-00220055$$jORCID:0000-0002-4234-3111$$uNovosibirsk State U.$$uNovosibirsk, IYF
002655508 700__ $$aMason, Lara Hannan$$iINSPIRE-00565027$$uMelbourne U.
002655508 700__ $$aMassa, Lorenzo$$iINSPIRE-00388313$$jORCID:0000-0002-3735-7762$$uINFN, Rome2$$uRome U., Tor Vergata
002655508 700__ $$aMassarotti, Paolo$$iINSPIRE-00293652$$jORCID:0000-0002-9335-9690$$uINFN, Naples$$uNaples U.
002655508 700__ $$aMastrandrea, Paolo$$iINSPIRE-00030630$$jORCID:0000-0002-9853-0194$$uAnnecy, LAPP
002655508 700__ $$aMastroberardino, Anna$$iINSPIRE-00172288$$jORCID:0000-0002-8933-9494$$uINFN, Cosenza$$uCalabria U.
002655508 700__ $$aMasubuchi, Tatsuya$$iINSPIRE-00030446$$jORCID:0000-0001-9984-8009$$uTokyo U., ICEPP
002655508 700__ $$aMaettig, Peter$$iINSPIRE-00105833$$jORCID:0000-0002-3928-590X$$uWuppertal U.
002655508 700__ $$aMaurer, Julien$$iINSPIRE-00236977$$jORCID:0000-0002-5162-3713$$uBucharest, IFIN-HH
002655508 700__ $$aMacek, Bostjan$$iINSPIRE-00219572$$uStefan Inst., Ljubljana
002655508 700__ $$aMaxfield, Stephen$$iINSPIRE-00105929$$uLiverpool U.
002655508 700__ $$aMaximov, Dmitriy$$iINSPIRE-00236989$$jORCID:0000-0001-8783-3758$$uNovosibirsk State U.$$uNovosibirsk, IYF
002655508 700__ $$aMazini, Rachid$$iINSPIRE-00220110$$jORCID:0000-0003-0954-0970$$uTaiwan, Inst. Phys.
002655508 700__ $$aMaznas, Ioannis$$iINSPIRE-00525014$$jORCID:0000-0001-8420-3742$$uAristotle U., Thessaloniki
002655508 700__ $$aMazza, Simone Michele$$iINSPIRE-00386351$$jORCID:0000-0003-3865-730X$$uUC, Santa Cruz
002655508 700__ $$aMc Fadden, Neil Christopher$$iINSPIRE-00439697$$uNew Mexico U.
002655508 700__ $$aMc Goldrick, Garrin$$iINSPIRE-00349874$$uToronto U.
002655508 700__ $$aMc Kee, Shawn Patrick$$iINSPIRE-00260714$$jORCID:0000-0002-4551-4502$$uMichigan U.
002655508 700__ $$aMcCarn, Allison$$iINSPIRE-00220122$$jORCID:0000-0003-0360-6051$$uMichigan U.
002655508 700__ $$aMcCarthy, Tom$$iINSPIRE-00220136$$jORCID:0000-0002-1182-3526$$uMunich, Max Planck Inst.
002655508 700__ $$aMcClymont, Laurie Iain$$iINSPIRE-00439886$$uUniversity Coll. London
002655508 700__ $$aMcDonald, Emily$$iINSPIRE-00507462$$jORCID:0000-0002-8092-5331$$uMelbourne U.
002655508 700__ $$aMcfayden, Joshua Angus$$iINSPIRE-00231570$$jORCID:0000-0001-9273-2564$$uCERN
002655508 700__ $$aMchedlidze, Gvantsa$$iINSPIRE-00306035$$jORCID:0000-0003-3534-4164$$uGottingen U., II. Phys. Inst.
002655508 700__ $$aMcKay, Madalyn Ann$$iINSPIRE-00575010$$uSouthern Methodist U.
002655508 700__ $$aMcLean, Kayla Dawn$$iINSPIRE-00576898$$jORCID:0000-0001-5475-2521$$uVictoria U.
002655508 700__ $$aMcMahon, Steve$$iINSPIRE-00220148$$uRutherford
002655508 700__ $$aMcnamara, Peter Charles$$iINSPIRE-00535046$$jORCID:0000-0002-0676-324X$$uMelbourne U.
002655508 700__ $$aMcnicol, Christopher John$$iINSPIRE-00561480$$uWarwick U.
002655508 700__ $$aMcPherson, Robert$$iINSPIRE-00106476$$jORCID:0000-0001-9211-7019$$uVictoria U.$$uIPP, Canada
002655508 700__ $$aMdhluli, Joyful Elma$$iINSPIRE-00571512$$jORCID:0000-0002-9745-0504$$uWitwatersrand U.
002655508 700__ $$aMeadows, Zachary Alden$$iINSPIRE-00574057$$jORCID:0000-0001-8119-0333$$uMassachusetts U., Amherst
002655508 700__ $$aMeehan, Samuel$$iINSPIRE-00298342$$jORCID:0000-0002-3613-7514$$uWashington U., Seattle
002655508 700__ $$aMegy, Theo Jean$$iINSPIRE-00548858$$jORCID:0000-0001-8569-7094$$uFreiburg U.
002655508 700__ $$aMehlhase, Sascha$$iINSPIRE-00220289$$jORCID:0000-0002-1281-2060$$uMunich U.
002655508 700__ $$aMehta, Andrew$$iINSPIRE-00300183$$jORCID:0000-0003-2619-9743$$uLiverpool U.
002655508 700__ $$aMeideck, Thomas$$iINSPIRE-00535671$$jORCID:0000-0002-3932-7495$$uLPSC, Grenoble
002655508 700__ $$aMeirose, Bernhard$$iINSPIRE-00220290$$jORCID:0000-0003-0032-7022$$uTexas U., Dallas
002655508 700__ $$aMelini, Davide$$iINSPIRE-00442240$$jORCID:0000-0002-7018-682X$$uValencia U., IFIC$$uGranada U., Theor. Phys. Astrophys.
002655508 700__ $$aMellado Garcia, Bruce Rafael$$iINSPIRE-00005240$$jORCID:0000-0003-4838-1546$$uWitwatersrand U.
002655508 700__ $$aMellenthin, Johannes Donatus$$iINSPIRE-00546166$$jORCID:0000-0002-3436-6102$$uGottingen U., II. Phys. Inst.
002655508 700__ $$aMelo, Matej$$iINSPIRE-00508306$$jORCID:0000-0003-4557-9792$$uComenius U.
002655508 700__ $$aMeloni, Federico$$iINSPIRE-00286780$$jORCID:0000-0001-7075-2214$$uDESY
002655508 700__ $$aMelzer, Alexander$$iINSPIRE-00563935$$uBonn U.
002655508 700__ $$aMenary, Stephen Burns$$iINSPIRE-00529690$$jORCID:0000-0003-1244-2802$$uManchester U.
002655508 700__ $$aMendes Gouveia, Emanuel Demetrio$$iINSPIRE-00586285$$uLIP, Lisbon
002655508 700__ $$aMeng, Lingxin$$iINSPIRE-00533043$$jORCID:0000-0002-2901-6589$$uLiverpool U.
002655508 700__ $$aMeng, Xiangting$$iINSPIRE-00535687$$jORCID:0000-0003-0399-1607$$uMichigan U.
002655508 700__ $$aMengarelli, Alberto$$iINSPIRE-00231636$$jORCID:0000-0002-1884-854X$$uINFN, Bologna$$uBologna U.
002655508 700__ $$aMenke, Sven$$iINSPIRE-00106910$$jORCID:0000-0002-8186-4032$$uMunich, Max Planck Inst.
002655508 700__ $$aMeoni, Evelin$$iINSPIRE-00220314$$uINFN, Cosenza$$uCalabria U.
002655508 700__ $$aMergelmeyer, Sebastian$$iINSPIRE-00239978$$uHumboldt U., Berlin
002655508 700__ $$aMerlassino, Claudia$$iINSPIRE-00566499$$jORCID:0000-0002-5445-5938$$uBern U., LHEP
002655508 700__ $$aMermod, Philippe$$iINSPIRE-00220326$$jORCID:0000-0001-9656-9901$$uGeneva U.
002655508 700__ $$aMerola, Leonardo$$iINSPIRE-00107018$$jORCID:0000-0002-1822-1114$$uINFN, Naples$$uNaples U.
002655508 700__ $$aMeroni, Chiara$$iINSPIRE-00107020$$jORCID:0000-0003-4779-3522$$uINFN, Milan
002655508 700__ $$aMerritt, Frank$$iINSPIRE-00107035$$uChicago U., EFI
002655508 700__ $$aMessina, Andrea$$iINSPIRE-00220338$$jORCID:0000-0003-1195-6780$$uINFN, Rome$$uRome U.
002655508 700__ $$aMetcalfe, Jessica$$iINSPIRE-00220340$$jORCID:0000-0001-5454-3017$$uArgonne
002655508 700__ $$aMete, Alaettin Serhan$$iINSPIRE-00220356$$jORCID:0000-0002-5508-530X$$uUC, Irvine
002655508 700__ $$aMeyer, Christopher$$iINSPIRE-00237016$$jORCID:0000-0003-3552-6566$$uPennsylvania U.
002655508 700__ $$aMeyer, Jochen$$iINSPIRE-00220381$$uTechnion
002655508 700__ $$aMeyer, Jean-Pierre$$iINSPIRE-00220370$$uIRFU, Saclay
002655508 700__ $$aMeyer Zu Theenhausen, Hanno$$iINSPIRE-00413137$$jORCID:0000-0002-3231-2848$$uKirchhoff Inst. Phys.
002655508 700__ $$aMiano, Fabrizio$$iINSPIRE-00452972$$jORCID:0000-0003-2767-3769$$uSussex U.
002655508 700__ $$aMiddleton, Robin$$iINSPIRE-00107429$$jORCID:0000-0002-8396-9946$$uRutherford
002655508 700__ $$aMijovic, Liza$$iINSPIRE-00220450$$jORCID:0000-0003-0162-2891$$uEdinburgh U.
002655508 700__ $$aMikenberg, Giora$$iINSPIRE-00107520$$uWeizmann Inst.
002655508 700__ $$aMikestikova, Marcela$$iINSPIRE-00220462$$jORCID:0000-0003-1277-2596$$uPrague, Inst. Phys.
002655508 700__ $$aMikuz, Marko$$iINSPIRE-00220474$$jORCID:0000-0002-4119-6156$$uStefan Inst., Ljubljana
002655508 700__ $$aMilesi, Marco$$iINSPIRE-00396260$$jORCID:0000-0002-8805-1886$$uMelbourne U.
002655508 700__ $$aMilic, Adriana$$iINSPIRE-00371740$$jORCID:0000-0002-9173-8363$$uToronto U.
002655508 700__ $$aMillar, Declan Andrew$$iINSPIRE-00444027$$jORCID:0000-0003-3713-8997$$uQueen Mary, U. of London
002655508 700__ $$aMiller, David$$iINSPIRE-00023943$$jORCID:0000-0002-9485-9435$$uChicago U., EFI
002655508 700__ $$aMilov, Alexander$$iINSPIRE-00056451$$jORCID:0000-0003-3863-3607$$uWeizmann Inst.
002655508 700__ $$aMilstead, David$$iINSPIRE-00220498$$uStockholm U.$$uStockholm U., OKC
002655508 700__ $$aMinaenko, Andrey$$iINSPIRE-00220511$$uSerpukhov, IHEP
002655508 700__ $$aMinano, Mercedes$$iINSPIRE-00220523$$jORCID:0000-0002-1291-143X$$uValencia U., IFIC
002655508 700__ $$aMinashvili, Irakli$$iINSPIRE-00306048$$jORCID:0000-0002-4688-3510$$uTbilisi State U.
002655508 700__ $$aMincer, Allen$$iINSPIRE-00107849$$jORCID:0000-0002-6307-1418$$uNew York U.
002655508 700__ $$aMindur, Bartosz$$iINSPIRE-00220535$$jORCID:0000-0002-5511-2611$$uAGH-UST, Cracow
002655508 700__ $$aMineev, Mikhail$$iINSPIRE-00220541$$uDubna, JINR
002655508 700__ $$aMinegishi, Yuji$$iINSPIRE-00525023$$uTokyo U., ICEPP
002655508 700__ $$aMing, Yao$$iINSPIRE-00220553$$uWisconsin U., Madison
002655508 700__ $$aMir, Lluisa-Maria$$iINSPIRE-00220565$$jORCID:0000-0002-4276-715X$$uBarcelona, IFAE
002655508 700__ $$aMirto, Alessandro$$iINSPIRE-00567151$$jORCID:0000-0001-7770-0361$$uINFN, Lecce$$uSalento U.
002655508 700__ $$aMistry, Khilesh Pradip$$iINSPIRE-00403633$$jORCID:0000-0001-7577-1588$$uPennsylvania U.
002655508 700__ $$aMitani, Takashi$$iINSPIRE-00342753$$uWaseda U.
002655508 700__ $$aMitrevski, Jovan$$iINSPIRE-00038843$$uMunich U.
002655508 700__ $$aMitsou, Vasiliki A$$iINSPIRE-00108110$$jORCID:0000-0002-1533-8886$$uValencia U., IFIC
002655508 700__ $$aMiucci, Antonio$$iINSPIRE-00362129$$jORCID:0000-0001-8828-843X$$uBern U., LHEP
002655508 700__ $$aMiyagawa, Paul$$iINSPIRE-00049051$$uSheffield U.
002655508 700__ $$aMizukami, Atsushi$$iINSPIRE-00525035$$jORCID:0000-0001-6672-0500$$uKEK, Tsukuba
002655508 700__ $$aMjoernmark, Jan-Ulf$$iINSPIRE-00220668$$uLund U.
002655508 700__ $$aMkrtchyan, Tigran$$iINSPIRE-00563534$$jORCID:0000-0002-5786-3136$$uYerevan Phys. Inst.
002655508 700__ $$aMlynarikova, Michaela$$iINSPIRE-00525048$$jORCID:0000-0003-2028-1930$$uCharles U.
002655508 700__ $$aMoa, Torbjoern$$iINSPIRE-00108216$$jORCID:0000-0002-7644-5984$$uStockholm U.$$uStockholm U., OKC
002655508 700__ $$aMochizuki, Kazuya$$iINSPIRE-00359682$$jORCID:0000-0002-6310-2149$$uMontreal U.
002655508 700__ $$aMogg, Philipp$$iINSPIRE-00540560$$jORCID:0000-0003-2688-234X$$uFreiburg U.
002655508 700__ $$aMohapatra, Soumya$$iINSPIRE-00231736$$jORCID:0000-0003-3006-6337$$uNevis Labs, Columbia U.
002655508 700__ $$aMolander, Simon$$iINSPIRE-00342710$$uStockholm U.$$uStockholm U., OKC
002655508 700__ $$aMoles-Valls, Regina$$iINSPIRE-00220705$$jORCID:0000-0003-1279-1965$$uBonn U.
002655508 700__ $$aMondragon, Matthew Craig$$iINSPIRE-00383685$$uMichigan State U.
002655508 700__ $$aMoenig, Klaus$$iINSPIRE-00108503$$jORCID:0000-0002-3169-7117$$uDESY
002655508 700__ $$aMonk, James$$iINSPIRE-00046573$$jORCID:0000-0001-8471-9247$$uBohr Inst.
002655508 700__ $$aMonnier, Emmanuel$$iINSPIRE-00326813$$jORCID:0000-0002-2551-5751$$uMarseille, CPPM
002655508 700__ $$aMontalbano, Alyssa$$iINSPIRE-00386528$$jORCID:0000-0002-5295-432X$$uSimon Fraser U.
002655508 700__ $$aMontejo Berlingen, Javier$$iINSPIRE-00286815$$jORCID:0000-0001-9213-904X$$uCERN
002655508 700__ $$aMonticelli, Fernando$$iINSPIRE-00220717$$jORCID:0000-0002-6974-1443$$uLa Plata U.
002655508 700__ $$aMonzani, Simone$$iINSPIRE-00231765$$jORCID:0000-0002-0479-2207$$uINFN, Milan
002655508 700__ $$aMorange, Nicolas$$iINSPIRE-00231774$$jORCID:0000-0003-0047-7215$$uOrsay, LAL
002655508 700__ $$aMoreno, Deywis$$iINSPIRE-00220759$$jORCID:0000-0001-7914-1495$$uAntonio Narino U.
002655508 700__ $$aMoreno Llacer, Maria$$iINSPIRE-00332523$$jORCID:0000-0003-1113-3645$$uCERN
002655508 700__ $$aMorettini, Paolo$$iINSPIRE-00220772$$jORCID:0000-0001-7139-7912$$uINFN, Genoa
002655508 700__ $$aMorgenstern, Marcus$$iINSPIRE-00286823$$jORCID:0000-0002-1287-1781$$uFOM, Amsterdam
002655508 700__ $$aMorgenstern, Stefanie$$iINSPIRE-00511715$$jORCID:0000-0002-7834-4781$$uDresden, Tech. U.
002655508 700__ $$aMori, Daniel$$iINSPIRE-00410854$$jORCID:0000-0002-0693-4133$$uSimon Fraser U.
002655508 700__ $$aMorii, Masahiro$$iINSPIRE-00108914$$jORCID:0000-0001-9324-057X$$uHarvard U., Phys. Dept.
002655508 700__ $$aMorinaga, Masahiro$$iINSPIRE-00381150$$uWaseda U.
002655508 700__ $$aMorisbak, Vanja$$iINSPIRE-00379515$$jORCID:0000-0001-8715-8780$$uOslo U.
002655508 700__ $$aMorley, Anthony Keith$$iINSPIRE-00201749$$jORCID:0000-0003-0373-1346$$uCERN
002655508 700__ $$aMornacchi, Giuseppe$$iINSPIRE-00220784$$jORCID:0000-0002-7866-4275$$uCERN
002655508 700__ $$aMorris, Alice Polyxeni$$iINSPIRE-00586295$$jORCID:0000-0002-2929-3869$$uUniversity Coll. London
002655508 700__ $$aMorris, John$$iINSPIRE-00220796$$uQueen Mary, U. of London
002655508 700__ $$aMorvaj, Ljiljana$$iINSPIRE-00237030$$jORCID:0000-0003-2061-2904$$uSUNY, Stony Brook
002655508 700__ $$aMoschovakos, Paraschos$$iINSPIRE-00529702$$jORCID:0000-0001-6993-9698$$uNatl. Tech. U., Athens
002655508 700__ $$aMosidze, Maia$$iINSPIRE-00306063$$uTbilisi State U.
002655508 700__ $$aMoss, Harry James$$iINSPIRE-00449187$$jORCID:0000-0001-6497-3619$$uSheffield U.
002655508 700__ $$aMoss, Josh$$iINSPIRE-00220808$$uSLAC$$uCal State, Sacramento
002655508 700__ $$aMotohashi, Kazuki$$iINSPIRE-00372213$$jORCID:0000-0001-6434-031X$$uTokyo Inst. Tech.
002655508 700__ $$aMount, Richard$$iINSPIRE-00059638$$uSLAC
002655508 700__ $$aMountricha, Eleni$$iINSPIRE-00220810$$uCERN
002655508 700__ $$aMoyse, Edward$$iINSPIRE-00220821$$jORCID:0000-0003-4449-6178$$uMassachusetts U., Amherst
002655508 700__ $$aMuanza, Steve$$iINSPIRE-00109389$$jORCID:0000-0002-1786-2075$$uMarseille, CPPM
002655508 700__ $$aMueller, Felix$$iINSPIRE-00220833$$uMunich, Max Planck Inst.
002655508 700__ $$aMueller, James$$iINSPIRE-00109443$$jORCID:0000-0001-5099-4718$$uPittsburgh U.
002655508 700__ $$aMueller, Ralph Soeren Peter$$iINSPIRE-00389964$$uMunich U.
002655508 700__ $$aMuenstermann, Daniel$$iINSPIRE-00220841$$jORCID:0000-0001-6223-2497$$uLancaster U.
002655508 700__ $$aMullier, Geoffrey Andre$$iINSPIRE-00407702$$jORCID:0000-0001-6771-0937$$uBern U., LHEP
002655508 700__ $$aMunoz Sanchez, Francisca Javiela$$iINSPIRE-00017703$$jORCID:0000-0002-6374-458X$$uManchester U.
002655508 700__ $$aMurin, Pavel$$iINSPIRE-00185470$$uKosice, IEF
002655508 700__ $$aMurray, Bill$$iINSPIRE-00109809$$jORCID:0000-0003-1710-6306$$uWarwick U.$$uRutherford
002655508 700__ $$aMurrone, Alessia$$iINSPIRE-00575770$$jORCID:0000-0001-5399-2478$$uINFN, Milan$$uMilan U.
002655508 700__ $$aMuskinja, Miha$$iINSPIRE-00452370$$jORCID:0000-0001-8442-2718$$uStefan Inst., Ljubljana
002655508 700__ $$aMwewa, Chilufya$$iINSPIRE-00571522$$uCape Town U.
002655508 700__ $$aMyagkov, Alexey$$iINSPIRE-00220926$$jORCID:0000-0003-4189-4250$$uSerpukhov, IHEP$$uMoscow, MIPT
002655508 700__ $$aMyers, John$$iINSPIRE-00572384$$jORCID:0000-0003-4126-4101$$uOregon U.
002655508 700__ $$aMyska, Miroslav$$iINSPIRE-00220932$$jORCID:0000-0003-0982-3380$$uPrague, Tech. U.
002655508 700__ $$aNachman, Benjamin Philip$$iINSPIRE-00376212$$jORCID:0000-0003-1024-0932$$uLBL, Berkeley
002655508 700__ $$aNackenhorst, Olaf$$iINSPIRE-00286840$$jORCID:0000-0002-2191-2725$$uDortmund U.
002655508 700__ $$aNagai, Koichi$$iINSPIRE-00220956$$jORCID:0000-0002-4285-0578$$uOxford U.
002655508 700__ $$aNagano, Kunihiro$$iINSPIRE-00110036$$jORCID:0000-0003-2741-0627$$uKEK, Tsukuba
002655508 700__ $$aNagasaka, Yasushi$$iINSPIRE-00220968$$jORCID:0000-0002-3669-9525$$uHiroshima Inst. Tech.
002655508 700__ $$aNagel, Martin$$iINSPIRE-00030110$$jORCID:0000-0002-2588-6691$$uFreiburg U.
002655508 700__ $$aNagy, Elemer$$iINSPIRE-00110088$$jORCID:0000-0001-5420-9537$$uMarseille, CPPM
002655508 700__ $$aNairz, Armin Michael$$iINSPIRE-00220970$$jORCID:0000-0003-3561-0880$$uCERN
002655508 700__ $$aNakahama, Yu$$iINSPIRE-00286861$$uNagoya U.
002655508 700__ $$aNakamura, Koji$$iINSPIRE-00047824$$uKEK, Tsukuba
002655508 700__ $$aNakamura, Tomoaki$$iINSPIRE-00110240$$uTokyo U., ICEPP
002655508 700__ $$aNakano, Itsuo$$iINSPIRE-00040923$$uOkayama U.
002655508 700__ $$aNanjo, Hajime$$iINSPIRE-00034540$$jORCID:0000-0003-0703-103X$$uOsaka U.
002655508 700__ $$aNapolitano, Fabrizio$$iINSPIRE-00581445$$jORCID:0000-0002-8686-5923$$uKirchhoff Inst. Phys.
002655508 700__ $$aNaranjo Garcia, Roger Felipe$$iINSPIRE-00381918$$jORCID:0000-0002-3222-6587$$uDESY
002655508 700__ $$aNarayan, Rohin$$iINSPIRE-00237051$$jORCID:0000-0002-8642-5119$$uTexas U.
002655508 700__ $$aNarrias Villar, Daniel Isaac$$iINSPIRE-00390052$$uKirchhoff Inst. Phys.
002655508 700__ $$aNaryshkin, Iouri$$iINSPIRE-00439969$$jORCID:0000-0001-6412-4801$$uSt. Petersburg, INP
002655508 700__ $$aNaumann, Thomas$$iINSPIRE-00110648$$jORCID:0000-0001-7372-8316$$uDESY
002655508 700__ $$aNavarro, Gabriela$$iINSPIRE-00221017$$jORCID:0000-0002-5108-0042$$uAntonio Narino U.
002655508 700__ $$aNayyar, Ruchika$$iINSPIRE-00301151$$uArizona U.
002655508 700__ $$aNeal, Homer$$iINSPIRE-00300519$$uMichigan U.
002655508 700__ $$aNechaeva, Polina$$iINSPIRE-00221047$$uLebedev Inst.
002655508 700__ $$aNeep, Thomas James$$iINSPIRE-00286870$$jORCID:0000-0003-0056-8651$$uIRFU, Saclay
002655508 700__ $$aNegri, Andrea$$iINSPIRE-00306082$$jORCID:0000-0002-7386-901X$$uINFN, Pavia$$uPavia U.
002655508 700__ $$aNegrini, Matteo$$iINSPIRE-00054399$$jORCID:0000-0003-0101-6963$$uINFN, Bologna
002655508 700__ $$aNektarijevic, Snezana$$iINSPIRE-00231852$$uNijmegen U.
002655508 700__ $$aNellist, Clara$$iINSPIRE-00304438$$jORCID:0000-0002-5171-8579$$uGottingen U., II. Phys. Inst.
002655508 700__ $$aNelson, Michael Edward$$iINSPIRE-00547663$$jORCID:0000-0002-0183-327X$$uOxford U.
002655508 700__ $$aNemecek, Stanislav$$iINSPIRE-00110909$$jORCID:0000-0001-8978-7150$$uPrague, Inst. Phys.
002655508 700__ $$aNemethy, Peter$$iINSPIRE-00321590$$uNew York U.
002655508 700__ $$aNessi, Marzio$$iINSPIRE-00221084$$jORCID:0000-0001-7316-0118$$uCERN$$uGeneva U.
002655508 700__ $$aNeubauer, Mark$$iINSPIRE-00110982$$jORCID:0000-0001-8434-9274$$uIllinois U., Urbana
002655508 700__ $$aNeumann, Manuel$$iINSPIRE-00288618$$uWuppertal U.
002655508 700__ $$aNewman, Paul$$iINSPIRE-00111158$$jORCID:0000-0002-6252-266X$$uBirmingham U.
002655508 700__ $$aNg, Tsz Yu$$iINSPIRE-00536671$$jORCID:0000-0002-7870-8522$$uHong Kong U. Sci. Tech.
002655508 700__ $$aNg, Yan Wing$$iINSPIRE-00548864$$uHumboldt U., Berlin
002655508 700__ $$aNguyen, Hoang Dai Nghia$$iINSPIRE-00575780$$jORCID:0000-0002-4326-9283$$uMarseille, CPPM
002655508 700__ $$aNguyen Manh, Tuan$$iINSPIRE-00417989$$jORCID:0000-0001-8585-9284$$uMontreal U.
002655508 700__ $$aNibigira, Emery$$iINSPIRE-00578858$$jORCID:0000-0001-5821-291X$$uClermont-Ferrand U.
002655508 700__ $$aNickerson, Richard$$iINSPIRE-00221121$$uOxford U.
002655508 700__ $$aNicolaidou, Rosy$$iINSPIRE-00216944$$uIRFU, Saclay
002655508 700__ $$aNielsen, Jason$$iINSPIRE-00111400$$jORCID:0000-0002-9175-4419$$uUC, Santa Cruz
002655508 700__ $$aNikiforou, Nikiforos$$iINSPIRE-00237074$$jORCID:0000-0003-1267-7740$$uTexas U.
002655508 700__ $$aNikolaenko, Vladimir$$iINSPIRE-00231894$$jORCID:0000-0001-6545-1820$$uSerpukhov, IHEP$$uMoscow, MIPT
002655508 700__ $$aNikolic-Audit, Irena$$iINSPIRE-00306103$$uParis U., VI-VII
002655508 700__ $$aNikolopoulos, Konstantinos$$iINSPIRE-00221145$$jORCID:0000-0002-3048-489X$$uBirmingham U.
002655508 700__ $$aNilsson, Paul$$iINSPIRE-00221150$$jORCID:0000-0002-6848-7463$$uBrookhaven
002655508 700__ $$aNinomiya, Yoichi$$iINSPIRE-00231907$$uKEK, Tsukuba
002655508 700__ $$aNisati, Aleandro$$iINSPIRE-00221160$$jORCID:0000-0002-5080-2293$$uINFN, Rome
002655508 700__ $$aNishu, Nishu$$iINSPIRE-00311000$$uShanghai Jiao Tong U.
002655508 700__ $$aNisius, Richard$$iINSPIRE-00111714$$jORCID:0000-0003-2257-0074$$uMunich, Max Planck Inst.
002655508 700__ $$aNitsche, Isabel$$iINSPIRE-00548871$$uDortmund U.
002655508 700__ $$aNitta, Tatsumi$$iINSPIRE-00551944$$uWaseda U.
002655508 700__ $$aNobe, Takuya$$iINSPIRE-00286888$$jORCID:0000-0002-5809-325X$$uTokyo U., ICEPP
002655508 700__ $$aNoguchi, Yohei$$iINSPIRE-00534663$$uKyoto U.
002655508 700__ $$aNomachi, Masaharu$$iINSPIRE-00111877$$uOsaka U.
002655508 700__ $$aNomidis, Ioannis$$iINSPIRE-00221178$$jORCID:0000-0002-7406-1100$$uParis U., VI-VII
002655508 700__ $$aNomura, Marcelo Ayumu$$iINSPIRE-00535055$$uBrookhaven
002655508 700__ $$aNooney, Tamsin$$iINSPIRE-00389111$$uQueen Mary, U. of London
002655508 700__ $$aNordberg, Markus$$iINSPIRE-00111954$$uCERN
002655508 700__ $$aBIN NORJOHARUDDEEN, Nurfikri$$iINSPIRE-00442949$$jORCID:0000-0002-8818-7476$$uOxford U.
002655508 700__ $$aNovak, Tadej$$iINSPIRE-00576909$$jORCID:0000-0002-3053-0913$$uStefan Inst., Ljubljana
002655508 700__ $$aNovgorodova, Olga$$iINSPIRE-00285705$$jORCID:0000-0001-6536-0179$$uDresden, Tech. U.
002655508 700__ $$aNovotny, Radek$$iINSPIRE-00571923$$uPrague, Tech. U.
002655508 700__ $$aNozka, Libor$$iINSPIRE-00152530$$uPalacky U.
002655508 700__ $$aNtekas, Konstantinos$$iINSPIRE-00349891$$jORCID:0000-0001-9252-6509$$uUC, Irvine
002655508 700__ $$aNurse, Emily$$iINSPIRE-00052439$$uUniversity Coll. London
002655508 700__ $$aNuti, Francesco$$iINSPIRE-00346170$$jORCID:0000-0003-3491-7637$$uMelbourne U.
002655508 700__ $$aOakham, Gerald$$iINSPIRE-00112393$$jORCID:0000-0003-2866-1049$$uCarleton U.$$uTRIUMF
002655508 700__ $$aOberlack, Horst$$iINSPIRE-00112415$$uMunich, Max Planck Inst.
002655508 700__ $$aObermann, Theresa$$iINSPIRE-00362697$$uBonn U.
002655508 700__ $$aOcariz, Jose$$iINSPIRE-00112459$$jORCID:0000-0003-2262-0780$$uParis U., VI-VII
002655508 700__ $$aOchi, Atsuhiko$$iINSPIRE-00112469$$uKobe U.
002655508 700__ $$aAbreu Juliao Ochoa De Castro, Maria Ines$$iINSPIRE-00335577$$jORCID:0000-0001-6156-1790$$uNevis Labs, Columbia U.
002655508 700__ $$aOchoa, Jean-pierre$$iINSPIRE-00404468$$jORCID:0000-0001-7376-5555$$uChile U., Catolica
002655508 700__ $$aO'Connor, Kelsey$$iINSPIRE-00534674$$jORCID:0000-0002-4036-5317$$uBrandeis U.
002655508 700__ $$aOda, Susumu$$iINSPIRE-00036017$$jORCID:0000-0001-5836-768X$$uKyushu U.
002655508 700__ $$aOdaka, Shigeru$$iINSPIRE-00221251$$jORCID:0000-0002-1227-1401$$uKEK, Tsukuba
002655508 700__ $$aOerdek, Serhat$$iINSPIRE-00639230$$jORCID:0000-0001-8763-0096$$uGottingen U., II. Phys. Inst.
002655508 700__ $$aOh, Alexander$$iINSPIRE-00320498$$jORCID:0000-0001-9025-0422$$uManchester U.
002655508 700__ $$aOh, Seog$$iINSPIRE-00112667$$jORCID:0000-0002-1679-7427$$uDuke U.
002655508 700__ $$aOhm, Christian$$iINSPIRE-00221275$$jORCID:0000-0002-8015-7512$$uRoyal Inst. Tech., Stockholm
002655508 700__ $$aOide, Hideyuki$$iINSPIRE-00379657$$jORCID:0000-0002-2173-3233$$uINFN, Genoa$$uGenoa U.
002655508 700__ $$aOjeda, Martina Laura$$iINSPIRE-00641151$$jORCID:0000-0002-3834-7830$$uToronto U.
002655508 700__ $$aOkawa, Hideki$$iINSPIRE-00221308$$jORCID:0000-0002-2548-6567$$uTsukuba U.
002655508 700__ $$aOkazaki, Yuta$$iINSPIRE-00579683$$jORCID:0000-0003-2677-5827$$uKyoto U.
002655508 700__ $$aOkumura, Yasuyuki$$iINSPIRE-00221310$$jORCID:0000-0002-7613-5572$$uTokyo U., ICEPP
002655508 700__ $$aOkuyama, Toyonobu$$iINSPIRE-00226798$$uKEK, Tsukuba
002655508 700__ $$aOlariu, Albert$$iINSPIRE-00237105$$uBucharest, IFIN-HH
002655508 700__ $$aOleiro Seabra, Luis Filipe$$iINSPIRE-00514541$$uLIP, Lisbon
002655508 700__ $$aOlivares Pino, Sebastian Andres$$iINSPIRE-00286912$$uChile U., Catolica
002655508 700__ $$aOliveira Damazio, Denis$$iINSPIRE-00221335$$uBrookhaven
002655508 700__ $$aOliver, Jason Lea$$iINSPIRE-00567172$$uAdelaide U., Sch. Chem. Phys.
002655508 700__ $$aOlsson, Mats Joakim Robert$$iINSPIRE-00536686$$jORCID:0000-0003-4154-8139$$uChicago U., EFI
002655508 700__ $$aOlszewski, Andrzej$$iINSPIRE-00256380$$jORCID:0000-0003-3368-5475$$uCracow, INP
002655508 700__ $$aOlszowska, Jolanta$$iINSPIRE-00221360$$jORCID:0000-0003-0520-9500$$uCracow, INP
002655508 700__ $$aO'Neil, Dugan$$iINSPIRE-00112324$$jORCID:0000-0003-0325-472X$$uSimon Fraser U.
002655508 700__ $$aOnofre, Antonio$$iINSPIRE-00221372$$jORCID:0000-0003-3471-2703$$uLIP, Lisbon$$uMinho U.
002655508 700__ $$aOnogi, Kouta$$iINSPIRE-00415586$$jORCID:0000-0002-4956-2093$$uNagoya U.
002655508 700__ $$aOnyisi, Peter$$iINSPIRE-00057397$$jORCID:0000-0003-4201-7997$$uTexas U.
002655508 700__ $$aOppen, Henrik$$iINSPIRE-00551958$$uOslo U.
002655508 700__ $$aOreglia, Mark$$iINSPIRE-00113317$$jORCID:0000-0001-6203-2209$$uChicago U., EFI
002655508 700__ $$aOren, Yona$$iINSPIRE-00221389$$uTel Aviv U.
002655508 700__ $$aOrestano, Domizia$$iINSPIRE-00113321$$jORCID:0000-0001-5103-5527$$uINFN, Rome3$$uRome III U.
002655508 700__ $$aOrgill, Emily Claire$$iINSPIRE-00551961$$jORCID:0000-0001-5093-3050$$uManchester U.
002655508 700__ $$aOrlando, Nicola$$iINSPIRE-00286920$$jORCID:0000-0003-0616-245X$$uHong Kong U.
002655508 700__ $$aO'Rourke, Abigail Alexandra$$iINSPIRE-00431615$$jORCID:0000-0002-7700-3782$$uDESY
002655508 700__ $$aOrr, Robert$$iINSPIRE-00113411$$jORCID:0000-0002-8690-9746$$uToronto U.
002655508 700__ $$aOsculati, Bianca$$iINSPIRE-00221407$$jORCID:0000-0002-7246-060X$$uINFN, Genoa$$uGenoa U.
002655508 700__ $$aO'Shea, Val$$iINSPIRE-00112370$$jORCID:0000-0001-7183-1205$$uGlasgow U.
002655508 700__ $$aOspanov, Rustem$$iINSPIRE-00029272$$jORCID:0000-0001-5091-9216$$uHefei, CUST
002655508 700__ $$aOtero y Garzon, Gustavo$$iINSPIRE-00046137$$jORCID:0000-0003-4803-5280$$uBuenos Aires U.
002655508 700__ $$aOtono, Hidetoshi$$iINSPIRE-00348488$$uKyushu U.
002655508 700__ $$aOuchrif, Mohamed$$iINSPIRE-00232012$$jORCID:0000-0002-2954-1420$$uOujda U.
002655508 700__ $$aOuld-Saada, Farid$$iINSPIRE-00221439$$jORCID:0000-0002-9404-835X$$uOslo U.
002655508 700__ $$aOuraou, Ahmimed$$iINSPIRE-00221444$$jORCID:0000-0001-6818-5994$$uIRFU, Saclay
002655508 700__ $$aOuyang, Qun$$iINSPIRE-00221456$$jORCID:0000-0002-8186-0082$$uBeijing, Inst. High Energy Phys.
002655508 700__ $$aOwen, Mark$$iINSPIRE-00007985$$jORCID:0000-0001-6820-0488$$uGlasgow U.
002655508 700__ $$aOwen, Rhys Edward$$iINSPIRE-00390165$$jORCID:0000-0002-2684-1399$$uBirmingham U.
002655508 700__ $$aOzcan, Veysi Erkcan$$iINSPIRE-00221480$$jORCID:0000-0003-4643-6347$$uBogazici U.
002655508 700__ $$aOzturk, Nurcan$$iINSPIRE-00026861$$jORCID:0000-0003-1125-6784$$uTexas U., Arlington
002655508 700__ $$aPacalt, Josef$$iINSPIRE-00547674$$uPalacky U.
002655508 700__ $$aPacey, Holly Ann$$iINSPIRE-00583997$$jORCID:0000-0002-2325-6792$$uCambridge U.
002655508 700__ $$aPachal, Katherine$$iINSPIRE-00337371$$jORCID:0000-0002-8332-243X$$uSimon Fraser U.
002655508 700__ $$aPacheco Pages, Andres$$iINSPIRE-00221495$$jORCID:0000-0001-8210-1734$$uBarcelona, IFAE
002655508 700__ $$aPacheco Rodriguez, Laura$$iINSPIRE-00511732$$uIRFU, Saclay
002655508 700__ $$aPadilla Aranda, Cristobal$$iINSPIRE-00306128$$jORCID:0000-0001-7951-0166$$uBarcelona, IFAE
002655508 700__ $$aPagan Griso, Simone$$iINSPIRE-00022647$$jORCID:0000-0003-0999-5019$$uLBL, Berkeley
002655508 700__ $$aPaganini, Michela$$iINSPIRE-00452535$$jORCID:0000-0003-4102-8002$$uYale U.
002655508 700__ $$aPalacino, Gabriel$$iINSPIRE-00237152$$uIndiana U.
002655508 700__ $$aPalazzo, Serena$$iINSPIRE-00511747$$uINFN, Cosenza$$uCalabria U.
002655508 700__ $$aPalestini, Sandro$$iINSPIRE-00221549$$jORCID:0000-0002-4110-096X$$uCERN
002655508 700__ $$aPalka, Marek$$iINSPIRE-00371751$$jORCID:0000-0002-7185-3540$$uJagiellonian U.
002655508 700__ $$aPallin, Dominique$$iINSPIRE-00221552$$jORCID:0000-0003-3751-9300$$uClermont-Ferrand U.
002655508 700__ $$aPanagoulias, Ilias$$iINSPIRE-00185557$$uNatl. Tech. U., Athens
002655508 700__ $$aPandini, Carlo Enrico$$iINSPIRE-00388516$$jORCID:0000-0003-3838-1307$$uCERN
002655508 700__ $$aPanduro Vazquez, Jose Guillermo$$iINSPIRE-00042480$$jORCID:0000-0003-2605-8940$$uRoyal Holloway, U. of London
002655508 700__ $$aPani, Priscilla$$iINSPIRE-00291943$$jORCID:0000-0003-2149-3791$$uCERN
002655508 700__ $$aPanizzo, Giancarlo$$iINSPIRE-00584000$$jORCID:0000-0002-0352-4833$$uINFN, Udine$$uUdine U.
002655508 700__ $$aPaolozzi, Lorenzo$$iINSPIRE-00349900$$uGeneva U.
002655508 700__ $$aPapadopoulou, Theodora$$iINSPIRE-00185572$$uNatl. Tech. U., Athens
002655508 700__ $$aPapageorgiou, Konstantinos$$iINSPIRE-00114455$$uAthens Natl. Capodistrian U.$$uAegean U., Chios
002655508 700__ $$aParamonov, Alexander$$iINSPIRE-00040880$$jORCID:0000-0002-6492-3061$$uArgonne
002655508 700__ $$aParedes Hernandez, Daniela$$iINSPIRE-00286969$$uHong Kong U.
002655508 700__ $$aParedes Saenz, Santiago Rafael$$iINSPIRE-00579695$$jORCID:0000-0001-8487-9603$$uOxford U.
002655508 700__ $$aParida, Bibhuti$$iINSPIRE-00206935$$jORCID:0000-0001-9367-8061$$uShanghai Jiao Tong U.
002655508 700__ $$aParker, Adam Jackson$$iINSPIRE-00511754$$jORCID:0000-0001-9410-3075$$uLancaster U.
002655508 700__ $$aParker, Kerry Ann$$iINSPIRE-00371766$$jORCID:0000-0003-0952-2043$$uDESY
002655508 700__ $$aParker, Andy$$iINSPIRE-00114726$$jORCID:0000-0001-9798-8411$$uCambridge U.
002655508 700__ $$aParodi, Fabrizio$$iINSPIRE-00339598$$jORCID:0000-0002-7160-4720$$uINFN, Genoa$$uGenoa U.
002655508 700__ $$aParsons, John$$iINSPIRE-00114789$$uNevis Labs, Columbia U.
002655508 700__ $$aParzefall, Ulrich$$iINSPIRE-00114827$$jORCID:0000-0002-4858-6560$$uFreiburg U.
002655508 700__ $$aPascuzzi, Vincent$$iINSPIRE-00423665$$jORCID:0000-0003-3167-8773$$uToronto U.
002655508 700__ $$aPasner, Jacob Martin$$iINSPIRE-00540573$$jORCID:0000-0003-3870-708X$$uUC, Santa Cruz
002655508 700__ $$aPasqualucci, Enrico$$iINSPIRE-00221595$$jORCID:0000-0001-8160-2545$$uINFN, Rome
002655508 700__ $$aPassaggio, Stefano$$iINSPIRE-00114912$$jORCID:0000-0001-9200-5738$$uINFN, Genoa
002655508 700__ $$aPastore, Francesca$$iINSPIRE-00221618$$jORCID:0000-0001-5962-7826$$uRoyal Holloway, U. of London
002655508 700__ $$aPasuwan, Patrawan$$iINSPIRE-00580293$$jORCID:0000-0003-2987-2964$$uStockholm U.$$uStockholm U., OKC
002655508 700__ $$aPataraia, Sophio$$iINSPIRE-00221648$$jORCID:0000-0002-3802-8100$$uMainz U.
002655508 700__ $$aPater, Joleen$$iINSPIRE-00221668$$uManchester U.
002655508 700__ $$aPathak, Atanu$$iINSPIRE-00574416$$uWisconsin U., Madison$$uLouisville U.
002655508 700__ $$aPauly, Thilo$$iINSPIRE-00221680$$uCERN
002655508 700__ $$aPearson, Benjamin$$iINSPIRE-00368502$$jORCID:0000-0003-3071-3143$$uMunich, Max Planck Inst.
002655508 700__ $$aPedersen, Maiken$$iINSPIRE-00298350$$uOslo U.
002655508 700__ $$aPedraza Diaz, Lucia$$iINSPIRE-00584017$$jORCID:0000-0003-3924-8276$$uNijmegen U.
002655508 700__ $$aCosta Batalha Pedro, Rute$$iINSPIRE-00357018$$jORCID:0000-0002-7139-9587$$uLIP, Lisbon$$uLisbon U., CFNUL
002655508 700__ $$aPeleganchuk, Sergey$$iINSPIRE-00221714$$jORCID:0000-0003-0907-7592$$uNovosibirsk State U.$$uNovosibirsk, IYF
002655508 700__ $$aPenc, Ondrej$$iINSPIRE-00408388$$jORCID:0000-0002-5433-3981$$uPrague, Inst. Phys.
002655508 700__ $$aPeng, Cong$$iINSPIRE-00407696$$jORCID:0000-0001-5769-9236$$uBeijing, GUCAS
002655508 700__ $$aPeng, Haiping$$iINSPIRE-00217635$$uHefei, CUST
002655508 700__ $$aSotto-Maior Peralva, Bernardo$$iINSPIRE-00517880$$jORCID:0000-0003-1664-5658$$uJuiz de Fora U.
002655508 700__ $$aPerego, Marta Maria$$iINSPIRE-00444101$$jORCID:0000-0002-9875-0904$$uIRFU, Saclay
002655508 700__ $$aPereira Peixoto, Ana Paula$$iINSPIRE-00576910$$jORCID:0000-0003-3424-7338$$uLIP, Lisbon
002655508 700__ $$aPerepelitsa, Dennis$$iINSPIRE-00342739$$jORCID:0000-0001-8732-6908$$uBrookhaven
002655508 700__ $$aPeri, Francesco$$iINSPIRE-00548883$$jORCID:0000-0002-7539-2534$$uHumboldt U., Berlin
002655508 700__ $$aPerini, Laura$$iINSPIRE-00221789$$jORCID:0000-0003-3715-0523$$uINFN, Milan$$uMilan U.
002655508 700__ $$aPernegger, Heinz$$iINSPIRE-00115755$$jORCID:0000-0001-6418-8784$$uCERN
002655508 700__ $$aPerrella, Sabrina$$iINSPIRE-00377109$$jORCID:0000-0003-4955-5130$$uINFN, Naples$$uNaples U.
002655508 700__ $$aPeshekhonov, Vladimir$$iINSPIRE-00221820$$uDubna, JINR
002655508 700__ $$aPeters, Krisztian$$iINSPIRE-00055152$$jORCID:0000-0002-7654-1677$$uDESY
002655508 700__ $$aPeters, Reinhild$$iINSPIRE-00008252$$jORCID:0000-0003-1702-7544$$uManchester U.
002655508 700__ $$aPetersen, Brian$$iINSPIRE-00115959$$jORCID:0000-0002-7380-6123$$uCERN
002655508 700__ $$aPetersen, Troels$$iINSPIRE-00221831$$jORCID:0000-0003-0221-3037$$uBohr Inst.
002655508 700__ $$aPetit, Elisabeth$$iINSPIRE-00221840$$jORCID:0000-0002-3059-735X$$uLPSC, Grenoble
002655508 700__ $$aPetridis, Andreas$$iINSPIRE-00232124$$jORCID:0000-0002-9716-1243$$uAdelaide U., Sch. Chem. Phys.
002655508 700__ $$aPetridou, Chariclia$$iINSPIRE-00116033$$jORCID:0000-0001-5957-6133$$uAristotle U., Thessaloniki
002655508 700__ $$aPetroff, Pierre$$iINSPIRE-00116049$$uOrsay, LAL
002655508 700__ $$aPetrov, Mariyan$$iINSPIRE-00443150$$uOxford U.
002655508 700__ $$aPetrucci, Fabrizio$$iINSPIRE-00221875$$jORCID:0000-0002-5278-2206$$uINFN, Rome3$$uRome III U.
002655508 700__ $$aPettee, Mariel Nelson$$iINSPIRE-00584029$$jORCID:0000-0001-9208-3218$$uYale U.
002655508 700__ $$aPettersson, Nora Emilia$$iINSPIRE-00360876$$jORCID:0000-0001-7451-3544$$uMassachusetts U., Amherst
002655508 700__ $$aPeyaud, Alan$$iINSPIRE-00380396$$jORCID:0000-0001-8933-8689$$uIRFU, Saclay
002655508 700__ $$aPezoa, Raquel$$iINSPIRE-00221890$$jORCID:0000-0003-3344-791X$$uSanta Maria U., Valparaiso
002655508 700__ $$aPham, Thu$$iINSPIRE-00573381$$jORCID:0000-0002-8859-1313$$uMelbourne U.
002655508 700__ $$aPhillips, Forrest Hays$$iINSPIRE-00525050$$jORCID:0000-0001-5928-6785$$uMichigan State U.
002655508 700__ $$aPhillips, Peter William$$iINSPIRE-00116199$$jORCID:0000-0003-3651-4081$$uRutherford
002655508 700__ $$aPiacquadio, Giacinto$$iINSPIRE-00221917$$jORCID:0000-0002-4531-2900$$uSUNY, Stony Brook
002655508 700__ $$aPianori, Elisabetta$$iINSPIRE-00009958$$jORCID:0000-0001-9233-5892$$uLBL, Berkeley
002655508 700__ $$aPicazio, Attilio$$iINSPIRE-00286993$$jORCID:0000-0001-5070-4717$$uMassachusetts U., Amherst
002655508 700__ $$aPickering, Mark Andrew$$iINSPIRE-00378953$$uOxford U.
002655508 700__ $$aPickles, Rebecca Hayley$$iINSPIRE-00537796$$uManchester U.
002655508 700__ $$aPiegaia, Ricardo$$iINSPIRE-00152829$$jORCID:0000-0001-7850-8005$$uBuenos Aires U.
002655508 700__ $$aPilcher, James$$iINSPIRE-00116477$$jORCID:0000-0003-2417-2176$$uChicago U., EFI
002655508 700__ $$aPilkington, Andrew$$iINSPIRE-00221938$$jORCID:0000-0001-8007-0778$$uManchester U.
002655508 700__ $$aPinamonti, Michele$$iINSPIRE-00221947$$jORCID:0000-0002-5282-5050$$uINFN, Rome2$$uRome U., Tor Vergata
002655508 700__ $$aPinfold, James$$iINSPIRE-00116512$$jORCID:0000-0002-2397-4196$$uAlberta U.
002655508 700__ $$aPitt, Michael$$iINSPIRE-00354261$$jORCID:0000-0003-2461-5985$$uWeizmann Inst.
002655508 700__ $$aPleier, Marc-Andre$$iINSPIRE-00046720$$jORCID:0000-0002-9461-3494$$uBrookhaven
002655508 700__ $$aPleskot, Vojtech$$iINSPIRE-00335597$$jORCID:0000-0001-5435-497X$$uCharles U.
002655508 700__ $$aPlotnikova, Elena$$iINSPIRE-00237193$$uDubna, JINR
002655508 700__ $$aPluth, Daniel$$iINSPIRE-00365906$$uIowa State U.
002655508 700__ $$aPodberezko, Pavel$$iINSPIRE-00537273$$jORCID:0000-0002-1142-3215$$uNovosibirsk State U.$$uNovosibirsk, IYF
002655508 700__ $$aPoettgen, Ruth$$iINSPIRE-00335606$$jORCID:0000-0002-3304-0987$$uLund U.
002655508 700__ $$aPoggi, Riccardo$$iINSPIRE-00560338$$uGeneva U.
002655508 700__ $$aPoggioli, Luc$$iINSPIRE-00221996$$uOrsay, LAL
002655508 700__ $$aPogrebnyak, Ivan$$iINSPIRE-00563948$$uMichigan State U.
002655508 700__ $$aPohl, David-leon$$iINSPIRE-00288837$$uBonn U.
002655508 700__ $$aPokharel, Ishan$$iINSPIRE-00567820$$jORCID:0000-0002-7915-0161$$uGottingen U., II. Phys. Inst.
002655508 700__ $$aPolesello, Giacomo$$iINSPIRE-00117049$$jORCID:0000-0001-8636-0186$$uINFN, Pavia
002655508 700__ $$aPoley, Anne-luise$$iINSPIRE-00407830$$jORCID:0000-0002-4063-0408$$uLBL, Berkeley
002655508 700__ $$aPolicicchio, Antonio$$iINSPIRE-00020903$$jORCID:0000-0002-1290-220X$$uINFN, Rome$$uRome U.
002655508 700__ $$aPolifka, Richard$$iINSPIRE-00185642$$uCERN
002655508 700__ $$aPolini, Alessandro$$iINSPIRE-00172064$$jORCID:0000-0002-4986-6628$$uINFN, Bologna
002655508 700__ $$aPollard, Christopher Samuel$$iINSPIRE-00345073$$jORCID:0000-0002-3690-3960$$uDESY
002655508 700__ $$aPolychronakos, Venetios$$iINSPIRE-00177114$$jORCID:0000-0002-4051-0828$$uBrookhaven
002655508 700__ $$aPonomarenko, Daniil$$iINSPIRE-00537808$$uMoscow Phys. Eng. Inst.
002655508 700__ $$aPontecorvo, Ludovico$$iINSPIRE-00222031$$jORCID:0000-0003-2284-3765$$uCERN
002655508 700__ $$aPopeneciu, Gabriel Alexandru$$iINSPIRE-00226844$$jORCID:0000-0001-9783-7736$$uINCDTIM, Cluj Napoca
002655508 700__ $$aPortillo Quintero, Dilia Maria$$iINSPIRE-00567387$$jORCID:0000-0002-7042-4058$$uParis U., VI-VII
002655508 700__ $$aPospisil, Stanislav$$iINSPIRE-00222085$$jORCID:0000-0001-5424-9096$$uPrague, Tech. U.
002655508 700__ $$aPotamianos, Karolos Jozef$$iINSPIRE-00019188$$jORCID:0000-0001-7839-9785$$uDESY
002655508 700__ $$aPotrap, Igor$$iINSPIRE-00222100$$jORCID:0000-0002-0375-6909$$uDubna, JINR
002655508 700__ $$aPotter, Christina$$iINSPIRE-00222115$$jORCID:0000-0002-9815-5208$$uCambridge U.
002655508 700__ $$aPotti, Harish$$iINSPIRE-00542110$$jORCID:0000-0002-0800-9902$$uTexas U.
002655508 700__ $$aPoulsen, Trine$$iINSPIRE-00534683$$jORCID:0000-0001-7207-6029$$uLund U.
002655508 700__ $$aPoveda, Joaquin$$iINSPIRE-00222132$$jORCID:0000-0001-8144-1964$$uCERN
002655508 700__ $$aPowell, Thomas Dennis$$iINSPIRE-00579707$$uSheffield U.
002655508 700__ $$aPozo Astigarraga, Mikel Eukeni$$iINSPIRE-00390254$$uCERN
002655508 700__ $$aPralavorio, Pascal$$iINSPIRE-00117512$$jORCID:0000-0002-2452-6715$$uMarseille, CPPM
002655508 700__ $$aPrell, Soeren$$iINSPIRE-00117610$$jORCID:0000-0002-0195-8005$$uIowa State U.
002655508 700__ $$aPrice, Darren$$iINSPIRE-00027472$$jORCID:0000-0003-2750-9977$$uManchester U.
002655508 700__ $$aPrimavera, Margherita$$iINSPIRE-00117740$$jORCID:0000-0002-6866-3818$$uINFN, Lecce
002655508 700__ $$aPrince, Sebastien$$iINSPIRE-00359694$$jORCID:0000-0001-9947-3892$$uMcGill U.
002655508 700__ $$aProklova, Nadezda$$iINSPIRE-00537815$$jORCID:0000-0002-5237-0201$$uMoscow Phys. Eng. Inst.
002655508 700__ $$aProkofiev, Kirill$$iINSPIRE-00002760$$jORCID:0000-0002-2177-6401$$uHong Kong U. Sci. Tech.
002655508 700__ $$aProkoshin, Fedor$$iINSPIRE-00030407$$jORCID:0000-0001-6389-5399$$uSanta Maria U., Valparaiso
002655508 700__ $$aProtopopescu, Serban$$iINSPIRE-00117905$$uBrookhaven
002655508 700__ $$aProudfoot, James$$iINSPIRE-00117915$$jORCID:0000-0003-1032-9945$$uArgonne
002655508 700__ $$aPrzybycien, Mariusz$$iINSPIRE-00117955$$jORCID:0000-0002-9235-2649$$uAGH-UST, Cracow
002655508 700__ $$aPuri, Akshat$$iINSPIRE-00515564$$jORCID:0000-0001-7843-1482$$uIllinois U., Urbana
002655508 700__ $$aPuzo, Patrick$$iINSPIRE-00222199$$uOrsay, LAL
002655508 700__ $$aQian, Jianming$$iINSPIRE-00118167$$jORCID:0000-0003-4813-8167$$uMichigan U.
002655508 700__ $$aQin, Yang$$iINSPIRE-00367059$$jORCID:0000-0002-6960-502X$$uManchester U.
002655508 700__ $$aQuadt, Arnulf$$iINSPIRE-00118216$$jORCID:0000-0002-0098-384X$$uGottingen U., II. Phys. Inst.
002655508 700__ $$aQueitsch-maitland, Michaela$$iINSPIRE-00367060$$jORCID:0000-0003-4643-515X$$uDESY
002655508 700__ $$aQureshi, Anum$$iINSPIRE-00340282$$uAdelaide U., Sch. Chem. Phys.
002655508 700__ $$aRados, Petar Kevin$$iINSPIRE-00362130$$uMelbourne U.
002655508 700__ $$aRagusa, Francesco$$iINSPIRE-00194492$$jORCID:0000-0002-4064-0489$$uINFN, Milan$$uMilan U.
002655508 700__ $$aRahal, Ghita$$iINSPIRE-00301248$$jORCID:0000-0001-5410-6562$$uCC, Villeurbanne
002655508 700__ $$aRaine, John Andrew$$iINSPIRE-00452694$$jORCID:0000-0002-5987-4648$$uGeneva U.
002655508 700__ $$aRajagopalan, Srinivasan$$iINSPIRE-00222308$$jORCID:0000-0001-6543-1520$$uBrookhaven
002655508 700__ $$aRamirez Morales, Andres$$iINSPIRE-00551980$$uQueen Mary, U. of London
002655508 700__ $$aRashid, Tasneem$$iINSPIRE-00541089$$jORCID:0000-0001-9245-2677$$uOrsay, LAL
002655508 700__ $$aRaspopov, Sergii$$iINSPIRE-00540585$$jORCID:0000-0002-8406-4583$$uAnnecy, LAPP
002655508 700__ $$aRatti, Maria Giulia$$iINSPIRE-00443282$$jORCID:0000-0003-1777-7855$$uINFN, Milan$$uMilan U.
002655508 700__ $$aRauch, Daniel Mauricio$$iINSPIRE-00525066$$jORCID:0000-0002-8527-7695$$uDESY
002655508 700__ $$aRauscher, Felix$$iINSPIRE-00222332$$uMunich U.
002655508 700__ $$aRave, Stefan$$iINSPIRE-00386585$$jORCID:0000-0002-0050-8053$$uMainz U.
002655508 700__ $$aRavina, Baptiste$$iINSPIRE-00577511$$jORCID:0000-0002-1622-6640$$uSheffield U.
002655508 700__ $$aRavinovich, Ilia$$iINSPIRE-00119200$$jORCID:0000-0001-9348-4363$$uWeizmann Inst.
002655508 700__ $$aRawling, Jacob Henry$$iINSPIRE-00540597$$jORCID:0000-0002-0520-9060$$uManchester U.
002655508 700__ $$aRaymond, Michel$$iINSPIRE-00222353$$uCERN
002655508 700__ $$aRead, Alexander Lincoln$$iINSPIRE-00119327$$jORCID:0000-0002-5751-6636$$uOslo U.
002655508 700__ $$aReadioff, Nathan Peter$$iINSPIRE-00368514$$jORCID:0000-0002-3427-0688$$uLPSC, Grenoble
002655508 700__ $$aReale, Marilea$$iINSPIRE-00445873$$jORCID:0000-0002-5478-6059$$uINFN, Lecce$$uSalento U.
002655508 700__ $$aRebuzzi, Daniela$$iINSPIRE-00222361$$jORCID:0000-0003-4461-3880$$uINFN, Pavia$$uPavia U.
002655508 700__ $$aRedelbach, Andreas$$iINSPIRE-00222375$$jORCID:0000-0002-8102-9686$$uWurzburg U.
002655508 700__ $$aRedlinger, George$$iINSPIRE-00119430$$jORCID:0000-0002-6437-9991$$uBrookhaven
002655508 700__ $$aReece, Ryan$$iINSPIRE-00016749$$uUC, Santa Cruz
002655508 700__ $$aReed, Robert$$iINSPIRE-00508435$$jORCID:0000-0003-4108-0548$$uWitwatersrand U.
002655508 700__ $$aReeves, Kendall$$iINSPIRE-00142245$$jORCID:0000-0003-3504-4882$$uTexas U., Dallas
002655508 700__ $$aRehnisch, Laura$$iINSPIRE-00354285$$jORCID:0000-0003-4382-8118$$uHumboldt U., Berlin
002655508 700__ $$aReichert, Joseph$$iINSPIRE-00423182$$jORCID:0000-0003-2110-8021$$uPennsylvania U.
002655508 700__ $$aReiss, Andreas$$iINSPIRE-00390339$$uMainz U.
002655508 700__ $$aRembser, Christoph$$iINSPIRE-00222420$$uCERN
002655508 700__ $$aRen, Huan$$iINSPIRE-00360700$$jORCID:0000-0003-4502-421X$$uBeijing, GUCAS
002655508 700__ $$aRescigno, Marco$$iINSPIRE-00119727$$jORCID:0000-0001-6507-2046$$uINFN, Rome
002655508 700__ $$aResconi, Silvia$$iINSPIRE-00222441$$jORCID:0000-0003-2313-4020$$uINFN, Milan
002655508 700__ $$aResseguie, Elodie Deborah$$iINSPIRE-00540608$$jORCID:0000-0002-7739-6176$$uPennsylvania U.
002655508 700__ $$aRettie, Sebastien$$iINSPIRE-00436230$$jORCID:0000-0002-7092-3893$$uBritish Columbia U.
002655508 700__ $$aReynolds, Elliot$$iINSPIRE-00537820$$jORCID:0000-0002-1506-5750$$uBirmingham U.
002655508 700__ $$aRezanova, Olga$$iINSPIRE-00235827$$jORCID:0000-0001-7141-0304$$uNovosibirsk State U.$$uNovosibirsk, IYF
002655508 700__ $$aReznicek, Pavel$$iINSPIRE-00222462$$jORCID:0000-0003-4017-9829$$uCharles U.
002655508 700__ $$aRicci, Ester$$iINSPIRE-00640500$$uTIFPA-INFN, Trento$$uTrento U.
002655508 700__ $$aRichter, Robert$$iINSPIRE-00120026$$uMunich, Max Planck Inst.
002655508 700__ $$aRichter, Stefan$$iINSPIRE-00393156$$jORCID:0000-0001-6613-4448$$uUniversity Coll. London
002655508 700__ $$aRichter-Was, Elzbieta$$iINSPIRE-00222485$$uJagiellonian U.
002655508 700__ $$aRicken, Oliver$$iINSPIRE-00394440$$jORCID:0000-0001-5107-7276$$uBonn U.
002655508 700__ $$aRidel, Melissa$$iINSPIRE-00052999$$jORCID:0000-0002-2601-7420$$uParis U., VI-VII
002655508 700__ $$aRieck, Patrick$$iINSPIRE-00333614$$jORCID:0000-0003-0290-0566$$uMunich, Max Planck Inst.
002655508 700__ $$aRiegel, Christian Johann$$iINSPIRE-00390368$$jORCID:0000-0002-3512-4420$$uWuppertal U.
002655508 700__ $$aRifki, Othmane$$iINSPIRE-00421293$$jORCID:0000-0002-9169-0793$$uDESY
002655508 700__ $$aRijssenbeek, Michael$$iINSPIRE-00120164$$uSUNY, Stony Brook
002655508 700__ $$aRimoldi, Adele$$iINSPIRE-00120224$$jORCID:0000-0003-3590-7908$$uINFN, Pavia$$uPavia U.
002655508 700__ $$aRimoldi, Marco$$iINSPIRE-00511766$$jORCID:0000-0003-1165-7940$$uBern U., LHEP
002655508 700__ $$aRinaldi, Lorenzo$$iINSPIRE-00222509$$jORCID:0000-0001-9608-9940$$uINFN, Bologna
002655508 700__ $$aRipellino, Giulia$$iINSPIRE-00549838$$jORCID:0000-0002-4053-5144$$uRoyal Inst. Tech., Stockholm
002655508 700__ $$aRistic, Branislav$$iINSPIRE-00442335$$jORCID:0000-0002-8610-1130$$uLancaster U.
002655508 700__ $$aRitsch, Elmar$$iINSPIRE-00334537$$uCERN
002655508 700__ $$aRiu, Imma$$iINSPIRE-00120419$$jORCID:0000-0002-3742-4582$$uBarcelona, IFAE
002655508 700__ $$aRivera Vergara, Juan Cristobal$$iINSPIRE-00577521$$uChile U., Catolica
002655508 700__ $$aRizatdinova, Flera$$iINSPIRE-00048668$$jORCID:0000-0002-2041-6236$$uOklahoma State U.
002655508 700__ $$aRizvi, Eram$$iINSPIRE-00120467$$jORCID:0000-0001-9834-2671$$uQueen Mary, U. of London
002655508 700__ $$aRizzi, Chiara$$iINSPIRE-00403072$$jORCID:0000-0001-6120-2325$$uBarcelona, IFAE
002655508 700__ $$aRoberts, Rhys Thomas$$iINSPIRE-00534698$$jORCID:0000-0002-0712-5215$$uManchester U.
002655508 700__ $$aRobertson, Steven$$iINSPIRE-00120586$$jORCID:0000-0003-4096-8393$$uMcGill U.$$uIPP, Canada
002655508 700__ $$aRobinson, Dave$$iINSPIRE-00222525$$jORCID:0000-0001-6169-4868$$uCambridge U.
002655508 700__ $$aRobinson, James$$iINSPIRE-00222565$$jORCID:0000-0002-2856-9413$$uDESY
002655508 700__ $$aRobson, Aidan$$iINSPIRE-00052951$$jORCID:0000-0002-1659-8284$$uGlasgow U.
002655508 700__ $$aRocco, Elena$$iINSPIRE-00385689$$jORCID:0000-0003-4468-9762$$uMainz U.
002655508 700__ $$aRoda, Chiara$$iINSPIRE-00222584$$jORCID:0000-0002-3020-4114$$uINFN, Pisa$$uPisa U.
002655508 700__ $$aRodina, Yulia$$iINSPIRE-00439858$$jORCID:0000-0003-1310-8697$$uMarseille, CPPM
002655508 700__ $$aRodriguez Bosca, Sergi$$iINSPIRE-00544722$$jORCID:0000-0002-4571-2509$$uValencia U., IFIC
002655508 700__ $$aRodriguez Perez, Andrea$$iINSPIRE-00436939$$jORCID:0000-0003-4759-9551$$uBarcelona, IFAE
002655508 700__ $$aRodriguez Rodriguez, Daniel$$iINSPIRE-00442425$$uValencia U., IFIC
002655508 700__ $$aRodriguez Vera, Ana Maria$$iINSPIRE-00548892$$jORCID:0000-0002-9609-3306$$uYork U., Canada
002655508 700__ $$aRoe, Shaun$$iINSPIRE-00222620$$uCERN
002655508 700__ $$aRogan, Christopher Sean$$iINSPIRE-00008339$$jORCID:0000-0002-4166-4503$$uHarvard U., Phys. Dept.
002655508 700__ $$aRohne, Ole$$iINSPIRE-00120872$$uOslo U.
002655508 700__ $$aRoehrig, Rainer$$iINSPIRE-00525374$$jORCID:0000-0001-5914-9270$$uMunich, Max Planck Inst.
002655508 700__ $$aRoland, Christophe Pol A$$iINSPIRE-00571930$$jORCID:0000-0003-2084-369X$$uIndiana U.
002655508 700__ $$aRoloff, Jennifer Kathryn$$iINSPIRE-00283411$$jORCID:0000-0001-6479-3079$$uHarvard U., Phys. Dept.
002655508 700__ $$aRomaniouk, Anatoli$$iINSPIRE-00222643$$uMoscow Phys. Eng. Inst.
002655508 700__ $$aRomano, Marino$$iINSPIRE-00237277$$jORCID:0000-0002-6609-7250$$uINFN, Bologna$$uBologna U.
002655508 700__ $$aRompotis, Nikolaos$$iINSPIRE-00311758$$jORCID:0000-0003-2577-1875$$uLiverpool U.
002655508 700__ $$aRonzani, Manfredi$$iINSPIRE-00265551$$uNew York U.
002655508 700__ $$aRoos, Lydia$$iINSPIRE-00121125$$jORCID:0000-0001-7151-9983$$uParis U., VI-VII
002655508 700__ $$aRosati, Stefano$$iINSPIRE-00226874$$jORCID:0000-0003-0838-5980$$uINFN, Rome
002655508 700__ $$aRosbach, Kilian$$iINSPIRE-00237292$$jORCID:0000-0002-4241-2949$$uFreiburg U.
002655508 700__ $$aRose, Peyton$$iINSPIRE-00376762$$uUC, Santa Cruz
002655508 700__ $$aRosien, Nils-arne$$iINSPIRE-00451917$$jORCID:0000-0001-6176-7975$$uGottingen U., II. Phys. Inst.
002655508 700__ $$aRossi, Edoardo$$iINSPIRE-00568840$$uDESY
002655508 700__ $$aRossi, Elvira$$iINSPIRE-00232312$$jORCID:0000-0001-9476-9854$$uINFN, Naples$$uNaples U.
002655508 700__ $$aRossi, Leonardo Paolo$$iINSPIRE-00222731$$jORCID:0000-0003-3104-7971$$uINFN, Genoa
002655508 700__ $$aRossini, Lorenzo$$iINSPIRE-00575796$$uINFN, Milan$$uMilan U.
002655508 700__ $$aRosten, Jonatan Hans$$iINSPIRE-00396349$$jORCID:0000-0001-5636-6050$$uCambridge U.
002655508 700__ $$aRosten, Rachel$$iINSPIRE-00345760$$uBarcelona, IFAE
002655508 700__ $$aRotaru, Marina$$iINSPIRE-00185709$$jORCID:0000-0003-4088-6275$$uBucharest, IFIN-HH
002655508 700__ $$aRothberg, Joseph$$iINSPIRE-00147103$$jORCID:0000-0001-7240-3747$$uWashington U., Seattle
002655508 700__ $$aRousseau, David$$iINSPIRE-00121457$$jORCID:0000-0001-7613-8063$$uOrsay, LAL
002655508 700__ $$aRoy, Debarati$$iINSPIRE-00332061$$jORCID:0000-0001-9858-1357$$uWitwatersrand U.
002655508 700__ $$aRozanov, Alexander$$iINSPIRE-00121556$$jORCID:0000-0003-0504-1453$$uMarseille, CPPM
002655508 700__ $$aRozen, Yoram$$iINSPIRE-00222740$$jORCID:0000-0001-6969-0634$$uTechnion
002655508 700__ $$aRuan, Xifeng$$iINSPIRE-00227177$$jORCID:0000-0001-5621-6677$$uWitwatersrand U.
002655508 700__ $$aRubbo, Francesco$$iINSPIRE-00263547$$jORCID:0000-0001-5170-3652$$uSLAC
002655508 700__ $$aRuehr, Frederik$$iINSPIRE-00222786$$jORCID:0000-0003-4452-620X$$uFreiburg U.
002655508 700__ $$aRuiz-Martinez, Aranzazu$$iINSPIRE-00222798$$jORCID:0000-0002-5742-2541$$uValencia U., IFIC
002655508 700__ $$aRurikova, Zuzana$$iINSPIRE-00217990$$jORCID:0000-0003-3051-9607$$uFreiburg U.
002655508 700__ $$aRusakovich, Nikolai$$iINSPIRE-00301212$$uDubna, JINR
002655508 700__ $$aRussell, Heather Lynn$$iINSPIRE-00381301$$jORCID:0000-0003-4181-0678$$uMcGill U.
002655508 700__ $$aRutherfoord, John$$iINSPIRE-00122016$$jORCID:0000-0002-4682-0667$$uArizona U.
002655508 700__ $$aRuttinger, Elias Michael$$iINSPIRE-00569467$$uDESY$$uSheffield U.
002655508 700__ $$aRyabov, Yury$$iINSPIRE-00306193$$uSt. Petersburg, INP
002655508 700__ $$aRybar, Martin$$iINSPIRE-00287074$$uIllinois U., Urbana
002655508 700__ $$aRybkin, Grigori$$iINSPIRE-00222835$$jORCID:0000-0001-5519-7267$$uOrsay, LAL
002655508 700__ $$aRyu, Soo$$iINSPIRE-00370160$$uArgonne
002655508 700__ $$aRyzhov, Andrey$$iINSPIRE-00414625$$uSerpukhov, IHEP
002655508 700__ $$aRzehorz, Gerhard Ferdinand$$iINSPIRE-00396985$$jORCID:0000-0002-3372-9565$$uGottingen U., II. Phys. Inst.
002655508 700__ $$aSabatini, Paolo$$iINSPIRE-00579719$$jORCID:0000-0003-0159-697X$$uGottingen U., II. Phys. Inst.
002655508 700__ $$aSabato, Gabriele$$iINSPIRE-00375930$$uFOM, Amsterdam
002655508 700__ $$aSacerdoti, Sabrina$$iINSPIRE-00339152$$jORCID:0000-0002-9003-5463$$uOrsay, LAL
002655508 700__ $$aSadrozinski, Hartmut$$iINSPIRE-00122290$$jORCID:0000-0003-0019-5410$$uUC, Santa Cruz
002655508 700__ $$aSadykov, Renat$$iINSPIRE-00222866$$uDubna, JINR
002655508 700__ $$aSafai Tehrani, Francesco$$iINSPIRE-00041870$$jORCID:0000-0001-7796-0120$$uINFN, Rome
002655508 700__ $$aSaha, Puja$$iINSPIRE-00418043$$uNorthern Illinois U.
002655508 700__ $$aSahinsoy, Merve$$iINSPIRE-00394595$$jORCID:0000-0002-7400-7286$$uKirchhoff Inst. Phys.
002655508 700__ $$aSahu, Arunika$$iINSPIRE-00575807$$jORCID:0000-0002-7064-0447$$uWuppertal U.
002655508 700__ $$aSaimpert, Matthias$$iINSPIRE-00387311$$jORCID:0000-0002-3765-1320$$uDESY
002655508 700__ $$aSaito, Masahiko$$iINSPIRE-00550991$$jORCID:0000-0001-5564-0935$$uTokyo U., ICEPP
002655508 700__ $$aSaito, Tomoyuki$$iINSPIRE-00399900$$jORCID:0000-0003-2567-6392$$uTokyo U., ICEPP
002655508 700__ $$aSakamoto, Hiroshi$$iINSPIRE-00122550$$jORCID:0000-0001-6819-2238$$uTokyo U., ICEPP
002655508 700__ $$aSakharov, Alexander$$iINSPIRE-00320810$$uNew York U.$$uManhattan Coll., Riverdale
002655508 700__ $$aSalamani, Dalila$$iINSPIRE-00577538$$uGeneva U.
002655508 700__ $$aSalamanna, Giuseppe$$iINSPIRE-00040818$$jORCID:0000-0002-0861-0052$$uINFN, Rome3$$uRome III U.
002655508 700__ $$aSalazar Loyola, Javier Esteban$$iINSPIRE-00393200$$uSanta Maria U., Valparaiso
002655508 700__ $$aSalek, David$$iINSPIRE-00185720$$uFOM, Amsterdam
002655508 700__ $$aSales De Bruin, Pedro Henrique$$iINSPIRE-00354071$$jORCID:0000-0003-0231-7872$$uUppsala U., Inst. Theor. Phys.
002655508 700__ $$aSalihagic, Denis$$iINSPIRE-00122755$$uMunich, Max Planck Inst.
002655508 700__ $$aSalnikov, Andrei$$iINSPIRE-00122791$$jORCID:0000-0002-3623-0161$$uSLAC
002655508 700__ $$aSalt, José$$iINSPIRE-00222878$$jORCID:0000-0003-4181-2788$$uValencia U., IFIC
002655508 700__ $$aSalvatore, Daniela$$iINSPIRE-00222890$$jORCID:0000-0002-8564-2373$$uINFN, Cosenza$$uCalabria U.
002655508 700__ $$aSalvatore, Pasquale Fabrizio$$iINSPIRE-00042310$$jORCID:0000-0002-3709-1554$$uSussex U.
002655508 700__ $$aSalvucci, Antonio$$iINSPIRE-00222904$$jORCID:0000-0003-4876-2613$$uHong Kong, Chinese U.$$uHong Kong U.$$uHong Kong U. Sci. Tech.
002655508 700__ $$aSalzburger, Andreas$$iINSPIRE-00222917$$jORCID:0000-0001-6004-3510$$uCERN
002655508 700__ $$aSamarati, Jerome$$iINSPIRE-00651703$$uCERN
002655508 700__ $$aSammel, Dirk$$iINSPIRE-00394771$$jORCID:0000-0003-4484-1410$$uFreiburg U.
002655508 700__ $$aSampsonidis, Dimitrios$$iINSPIRE-00222923$$uAristotle U., Thessaloniki
002655508 700__ $$aSampsonidou, Despoina$$iINSPIRE-00531687$$uAristotle U., Thessaloniki
002655508 700__ $$aSánchez, Javier$$iINSPIRE-00224147$$jORCID:0000-0001-9913-310X$$uValencia U., IFIC
002655508 700__ $$aSanchez Pineda, Arturo Rodolfo$$iINSPIRE-00237353$$jORCID:0000-0001-8241-7835$$uINFN, Udine$$uUdine U.
002655508 700__ $$aSandaker, Heidi$$iINSPIRE-00222934$$uOslo U.
002655508 700__ $$aSander, Christian Oliver$$iINSPIRE-00315812$$jORCID:0000-0003-2576-259X$$uDESY
002655508 700__ $$aSandhoff, Marisa$$iINSPIRE-00008264$$uWuppertal U.
002655508 700__ $$aSandoval Usme, Carlos$$iINSPIRE-00237372$$jORCID:0000-0003-1038-723X$$uAntonio Narino U.
002655508 700__ $$aSankey, Dave$$iINSPIRE-00123095$$jORCID:0000-0003-0955-4213$$uRutherford
002655508 700__ $$aSannino, Mario$$iINSPIRE-00123116$$jORCID:0000-0001-7700-8383$$uINFN, Genoa$$uGenoa U.
002655508 700__ $$aSano, Yuta$$iINSPIRE-00549843$$jORCID:0000-0001-7152-1872$$uNagoya U.
002655508 700__ $$aSansoni, Andrea$$iINSPIRE-00222964$$jORCID:0000-0002-9166-099X$$uFrascati
002655508 700__ $$aSantoni, Claudio$$iINSPIRE-00161887$$uClermont-Ferrand U.
002655508 700__ $$aSantos, Helena$$iINSPIRE-00232412$$jORCID:0000-0003-1710-9291$$uLIP, Lisbon
002655508 700__ $$aSantoyo Castillo, Itzebelt$$iINSPIRE-00291958$$uSussex U.
002655508 700__ $$aSantra, Arka$$iINSPIRE-00356248$$jORCID:0000-0003-4644-2579$$uValencia U., IFIC
002655508 700__ $$aSapronov, Andrey$$iINSPIRE-00011775$$uDubna, JINR
002655508 700__ $$aSaraiva, Joao$$iINSPIRE-00306227$$jORCID:0000-0002-7006-0864$$uLIP, Lisbon$$uLisbon U., CFNUL
002655508 700__ $$aSasaki, Osamu$$iINSPIRE-00123320$$jORCID:0000-0002-2910-3906$$uKEK, Tsukuba
002655508 700__ $$aSato, Koji$$iINSPIRE-00048967$$jORCID:0000-0001-8988-4065$$uTsukuba U.
002655508 700__ $$aSauvan, Emmanuel$$iINSPIRE-00185747$$jORCID:0000-0003-1921-2647$$uAnnecy, LAPP
002655508 700__ $$aSavard, Pierre$$iINSPIRE-00123492$$jORCID:0000-0001-5606-0107$$uToronto U.$$uTRIUMF
002655508 700__ $$aSavic, Natascha$$iINSPIRE-00517212$$uMunich, Max Planck Inst.
002655508 700__ $$aSawada, Ryu$$iINSPIRE-00572706$$jORCID:0000-0002-2226-9874$$uTokyo U., ICEPP
002655508 700__ $$aSawyer, Craig$$iINSPIRE-00337679$$jORCID:0000-0002-2027-1428$$uRutherford
002655508 700__ $$aSawyer, Lee$$iINSPIRE-00123608$$jORCID:0000-0001-8295-0605$$uLouisiana Tech. U.
002655508 700__ $$aSbarra, Carla$$iINSPIRE-00223003$$jORCID:0000-0002-8236-5251$$uINFN, Bologna
002655508 700__ $$aSbrizzi, Antonio$$iINSPIRE-00223019$$jORCID:0000-0002-1934-3041$$uBologna U.
002655508 700__ $$aScanlon, Timothy Paul$$iINSPIRE-00038709$$jORCID:0000-0002-2746-525X$$uUniversity Coll. London
002655508 700__ $$aSchaarschmidt, Jana$$iINSPIRE-00223142$$jORCID:0000-0002-0433-6439$$uWashington U., Seattle
002655508 700__ $$aSchacht, Peter$$iINSPIRE-00223156$$jORCID:0000-0002-7215-7977$$uMunich, Max Planck Inst.
002655508 700__ $$aSchachtner, Balthasar Maria$$iINSPIRE-00470481$$jORCID:0000-0002-8712-3948$$uMunich U.
002655508 700__ $$aSchaefer, Douglas$$iINSPIRE-00332120$$jORCID:0000-0002-8637-6134$$uChicago U., EFI
002655508 700__ $$aSchaefer, Leigh$$iINSPIRE-00442510$$jORCID:0000-0003-1355-5032$$uPennsylvania U.
002655508 700__ $$aSchaeffer, Jan$$iINSPIRE-00354291$$jORCID:0000-0003-2271-5739$$uMainz U.
002655508 700__ $$aSchaepe, Steffen$$iINSPIRE-00237394$$jORCID:0000-0002-6270-2214$$uCERN
002655508 700__ $$aSchaefer, Uli$$iINSPIRE-00146919$$jORCID:0000-0003-4489-9145$$uMainz U.
002655508 700__ $$aSchaffer, Arthur$$iINSPIRE-00223168$$jORCID:0000-0002-2586-7554$$uOrsay, LAL
002655508 700__ $$aSchaile, Dorothee$$iINSPIRE-00300542$$jORCID:0000-0001-7822-9663$$uMunich U.
002655508 700__ $$aSchamberger, R Dean$$iINSPIRE-00123848$$jORCID:0000-0003-1218-425X$$uSUNY, Stony Brook
002655508 700__ $$aScharmberg, Nicolas$$iINSPIRE-00585835$$jORCID:0000-0001-5180-3645$$uManchester U.
002655508 700__ $$aSchegelsky, Valery$$iINSPIRE-00223190$$jORCID:0000-0003-1870-1967$$uSt. Petersburg, INP
002655508 700__ $$aScheirich, Daniel$$iINSPIRE-00223208$$jORCID:0000-0001-6012-7191$$uCharles U.
002655508 700__ $$aSchenck, Ferdinand$$iINSPIRE-00571551$$jORCID:0000-0001-8279-4753$$uHumboldt U., Berlin
002655508 700__ $$aSchernau, Michael$$iINSPIRE-00123929$$jORCID:0000-0002-0859-4312$$uUC, Irvine
002655508 700__ $$aSchiavi, Carlo$$iINSPIRE-00223222$$jORCID:0000-0003-0957-4994$$uINFN, Genoa$$uGenoa U.
002655508 700__ $$aSchier, Sheena$$iINSPIRE-00507500$$jORCID:0000-0002-0310-7124$$uUC, Santa Cruz
002655508 700__ $$aSchildgen, Lara Katharina$$iINSPIRE-00548913$$jORCID:0000-0002-6834-9538$$uBonn U.
002655508 700__ $$aSchillaci, Zachary Michael$$iINSPIRE-00571564$$jORCID:0000-0002-6978-5323$$uBrandeis U.
002655508 700__ $$aSchioppa, Enrico Junior$$iINSPIRE-00572395$$jORCID:0000-0002-1369-9944$$uCERN
002655508 700__ $$aSchioppa, Marco$$iINSPIRE-00172296$$jORCID:0000-0003-0628-0579$$uINFN, Cosenza$$uCalabria U.
002655508 700__ $$aSchleicher, Katharina$$iINSPIRE-00572717$$jORCID:0000-0002-2917-7032$$uFreiburg U.
002655508 700__ $$aSchlenker, Stefan$$iINSPIRE-00223244$$jORCID:0000-0001-5239-3609$$uCERN
002655508 700__ $$aSchmidt-Sommerfeld, Korbinian Ralf$$iINSPIRE-00470659$$jORCID:0000-0003-4763-1822$$uMunich, Max Planck Inst.
002655508 700__ $$aSchmieden, Kristof$$iINSPIRE-00260738$$jORCID:0000-0003-1978-4928$$uCERN
002655508 700__ $$aSchmitt, Christian$$iINSPIRE-00058231$$jORCID:0000-0003-1471-690X$$uMainz U.
002655508 700__ $$aSchmitt, Stefan$$iINSPIRE-00124271$$jORCID:0000-0001-8387-1853$$uDESY
002655508 700__ $$aSchmitz, Simon$$iINSPIRE-00424511$$uMainz U.
002655508 700__ $$aSchmoeckel, Julian Constantin$$iINSPIRE-00643177$$jORCID:0000-0002-4847-5326$$uDESY
002655508 700__ $$aSchnoor, Ulrike$$iINSPIRE-00287141$$jORCID:0000-0002-2237-384X$$uFreiburg U.
002655508 700__ $$aSchoeffel, Laurent$$iINSPIRE-00185759$$jORCID:0000-0002-8081-2353$$uIRFU, Saclay
002655508 700__ $$aSchoening, Andre$$iINSPIRE-00185763$$jORCID:0000-0002-4499-7215$$uHeidelberg U.
002655508 700__ $$aSchopf, Elisabeth$$iINSPIRE-00396420$$jORCID:0000-0002-9340-2214$$uBonn U.
002655508 700__ $$aSchott, Matthias$$iINSPIRE-00223276$$jORCID:0000-0002-4235-7265$$uMainz U.
002655508 700__ $$aSchouwenberg, Jeroen$$iINSPIRE-00518610$$jORCID:0000-0002-8738-9519$$uNijmegen U.
002655508 700__ $$aSchovancova, Jaroslava$$iINSPIRE-00153378$$jORCID:0000-0003-0016-5246$$uCERN
002655508 700__ $$aSchramm, Steven$$iINSPIRE-00356617$$jORCID:0000-0001-9031-6751$$uGeneva U.
002655508 700__ $$aSchulte, Alexandra$$iINSPIRE-00452850$$jORCID:0000-0001-6692-2698$$uMainz U.
002655508 700__ $$aSchultz-Coulon, Hans-Christian$$iINSPIRE-00124529$$jORCID:0000-0002-0860-7240$$uKirchhoff Inst. Phys.
002655508 700__ $$aSchumacher, Markus$$iINSPIRE-00223322$$jORCID:0000-0002-1733-8388$$uFreiburg U.
002655508 700__ $$aSchumm, Bruce$$iINSPIRE-00124566$$jORCID:0000-0002-5394-0317$$uUC, Santa Cruz
002655508 700__ $$aSchune, Philippe$$iINSPIRE-00124581$$uIRFU, Saclay
002655508 700__ $$aSchwartzman, Ariel$$iINSPIRE-00053381$$jORCID:0000-0002-6680-8366$$uSLAC
002655508 700__ $$aSchwarz, Thomas Andrew$$iINSPIRE-00025352$$uMichigan U.
002655508 700__ $$aSchweiger, Hansdieter$$iINSPIRE-00362154$$uManchester U.
002655508 700__ $$aSchwemling, Philippe$$iINSPIRE-00124725$$jORCID:0000-0003-0989-5675$$uIRFU, Saclay
002655508 700__ $$aSchwienhorst, Reinhard$$iINSPIRE-00050408$$jORCID:0000-0001-6348-5410$$uMichigan State U.
002655508 700__ $$aSciandra, Andrea$$iINSPIRE-00537833$$jORCID:0000-0001-7163-501X$$uBonn U.
002655508 700__ $$aSciolla, Gabriella$$iINSPIRE-00124804$$jORCID:0000-0002-8482-1775$$uBrandeis U.
002655508 700__ $$aScornajenghi, Matteo$$iINSPIRE-00551992$$jORCID:0000-0001-5967-8471$$uINFN, Cosenza$$uCalabria U.
002655508 700__ $$aScuri, Fabrizio$$iINSPIRE-00124895$$jORCID:0000-0001-9569-3089$$uINFN, Pisa
002655508 700__ $$aScutti, Federico$$iINSPIRE-00339167$$uMelbourne U.
002655508 700__ $$aScyboz, Ludovic Michel$$iINSPIRE-00571572$$jORCID:0000-0001-8453-7937$$uMunich, Max Planck Inst.
002655508 700__ $$aSearcy, Jacob$$iINSPIRE-00223354$$uMichigan U.
002655508 700__ $$aSebastiani, Cristiano David$$iINSPIRE-00581451$$jORCID:0000-0003-1073-035X$$uINFN, Rome$$uRome U.
002655508 700__ $$aSeema, Pienpen$$iINSPIRE-00380584$$uBonn U.
002655508 700__ $$aSeidel, Sally$$iINSPIRE-00125002$$jORCID:0000-0002-1181-3061$$uNew Mexico U.
002655508 700__ $$aSeiden, Abraham$$iINSPIRE-00125018$$jORCID:0000-0003-4311-8597$$uUC, Santa Cruz
002655508 700__ $$aSeiss, Todd$$iINSPIRE-00584595$$jORCID:0000-0003-0810-240X$$uChicago U., EFI
002655508 700__ $$aSeixas, Jose$$iINSPIRE-00306265$$jORCID:0000-0001-5148-7363$$uRio de Janeiro Federal U.
002655508 700__ $$aSekhniaidze, Givi$$iINSPIRE-00223392$$jORCID:0000-0002-4116-5309$$uINFN, Naples
002655508 700__ $$aSekhon, Karishma$$iINSPIRE-00405663$$jORCID:0000-0001-7677-8394$$uMichigan U.
002655508 700__ $$aSekula, Stephen Jacob$$iINSPIRE-00052448$$jORCID:0000-0002-3199-4699$$uSouthern Methodist U.
002655508 700__ $$aSemprini-Cesari, Nicola$$iINSPIRE-00223442$$jORCID:0000-0002-3946-377X$$uINFN, Bologna$$uBologna U.
002655508 700__ $$aSen, Sourav$$iINSPIRE-00426825$$uDuke U.
002655508 700__ $$aSenkin, Sergey$$iINSPIRE-00002909$$jORCID:0000-0001-5848-005X$$uClermont-Ferrand U.
002655508 700__ $$aSerfon, Cedric$$iINSPIRE-00223458$$jORCID:0000-0001-7658-4901$$uOslo U.
002655508 700__ $$aSerin, Laurent$$iINSPIRE-00223468$$jORCID:0000-0003-3238-5382$$uOrsay, LAL
002655508 700__ $$aSerkin, Leonid$$iINSPIRE-00246780$$jORCID:0000-0003-4749-5250$$uINFN, Udine$$uICTP, Trieste
002655508 700__ $$aSessa, Marco$$iINSPIRE-00404546$$jORCID:0000-0002-1402-7525$$uINFN, Rome3$$uRome III U.
002655508 700__ $$aSeverini, Horst$$iINSPIRE-00125370$$jORCID:0000-0003-3316-846X$$uOklahoma U.
002655508 700__ $$aSforza, Federico$$iINSPIRE-00011580$$jORCID:0000-0002-4065-7352$$uTufts U.
002655508 700__ $$aSfyrla, Anna$$iINSPIRE-00030383$$jORCID:0000-0002-3003-9905$$uGeneva U.
002655508 700__ $$aShabalina, Elizaveta$$iINSPIRE-00038690$$jORCID:0000-0003-4849-556X$$uGottingen U., II. Phys. Inst.
002655508 700__ $$aShahinian, Jeffrey David$$iINSPIRE-00562258$$jORCID:0000-0002-1325-3432$$uUC, Santa Cruz
002655508 700__ $$aShaikh, Nabila Wahab$$iINSPIRE-00440772$$jORCID:0000-0001-9358-3505$$uStockholm U.$$uStockholm U., OKC
002655508 700__ $$aShan, Lianyou$$iINSPIRE-00223489$$jORCID:0000-0001-9134-5925$$uBeijing, Inst. High Energy Phys.
002655508 700__ $$aShang, Ruo-yu$$iINSPIRE-00367695$$jORCID:0000-0002-9856-989X$$uIllinois U., Urbana
002655508 700__ $$aShank, James$$iINSPIRE-00125560$$jORCID:0000-0002-9979-2356$$uBoston U.
002655508 700__ $$aShapiro, Marjorie$$iINSPIRE-00125625$$jORCID:0000-0001-8540-9654$$uLBL, Berkeley
002655508 700__ $$aSharma, Abhishek$$iINSPIRE-00571586$$jORCID:0000-0003-2250-4181$$uAdelaide U., Sch. Chem. Phys.
002655508 700__ $$aSharma, Abhishek$$iINSPIRE-00401935$$jORCID:0000-0002-5211-7177$$uOxford U.
002655508 700__ $$aShatalov, Pavel$$iINSPIRE-00223506$$jORCID:0000-0001-7530-4162$$uMoscow, ITEP
002655508 700__ $$aShaw, Kate$$iINSPIRE-00223518$$jORCID:0000-0001-9182-0634$$uSussex U.
002655508 700__ $$aShaw, Savanna Marie$$iINSPIRE-00347635$$jORCID:0000-0002-8958-7826$$uManchester U.
002655508 700__ $$aShcherbakova, Anna$$iINSPIRE-00386441$$jORCID:0000-0002-5690-0521$$uSt. Petersburg, INP
002655508 700__ $$aShen, Yu-Ting$$iINSPIRE-00529728$$uOklahoma U.
002655508 700__ $$aSherafati, Nima$$iINSPIRE-00548920$$jORCID:0000-0002-8080-1048$$uCarleton U.
002655508 700__ $$aSherman, Alexander David$$iINSPIRE-00542422$$uBoston U.
002655508 700__ $$aSherwood, Peter$$iINSPIRE-00223529$$jORCID:0000-0002-6621-4111$$uUniversity Coll. London
002655508 700__ $$aShi, Liaoshan$$iINSPIRE-00367077$$jORCID:0000-0001-9532-5075$$uTaiwan, Inst. Phys.$$uZhongshan U.
002655508 700__ $$aShimizu, Shima$$iINSPIRE-00173951$$jORCID:0000-0001-8279-442X$$uKEK, Tsukuba
002655508 700__ $$aShimmin, Chase Owen$$iINSPIRE-00364288$$jORCID:0000-0002-2228-2251$$uYale U.
002655508 700__ $$aShimojima, Makoto$$iINSPIRE-00050740$$jORCID:0000-0002-8738-1664$$uNagasaki Inst. Appl. Sci.
002655508 700__ $$aShipsey, Ian Peter Joseph$$iINSPIRE-00319805$$uOxford U.
002655508 700__ $$aShirabe, Shohei$$iINSPIRE-00529735$$jORCID:0000-0002-3191-0061$$uKyushu U.
002655508 700__ $$aShiyakova, Mariya$$iINSPIRE-00237482$$uDubna, JINR
002655508 700__ $$aShlomi, Jonathan$$iINSPIRE-00541100$$jORCID:0000-0002-2628-3470$$uWeizmann Inst.
002655508 700__ $$aShmeleva, Alevtina$$iINSPIRE-00223548$$uLebedev Inst.
002655508 700__ $$aShoaleh Saadi, Diane$$iINSPIRE-00382063$$uMontreal U.
002655508 700__ $$aShochet, Mel$$iINSPIRE-00126064$$jORCID:0000-0002-3017-826X$$uChicago U., EFI
002655508 700__ $$aShojaii, Seyed Ruhollah$$iINSPIRE-00380893$$jORCID:0000-0002-9449-0412$$uMelbourne U.
002655508 700__ $$aShope, David Richard$$iINSPIRE-00529749$$uOklahoma U.
002655508 700__ $$aShrestha, Suyog$$iINSPIRE-00237498$$jORCID:0000-0001-7249-7456$$uOhio State U.
002655508 700__ $$aShulga, Evgeny$$iINSPIRE-00287239$$jORCID:0000-0001-5099-7644$$uMoscow Phys. Eng. Inst.
002655508 700__ $$aSicho, Petr$$iINSPIRE-00223560$$uPrague, Inst. Phys.
002655508 700__ $$aSickles, Anne Marie$$iINSPIRE-00043440$$jORCID:0000-0002-3246-0330$$uIllinois U., Urbana
002655508 700__ $$aSidebo, Per Edvin$$iINSPIRE-00407780$$jORCID:0000-0002-0299-8236$$uRoyal Inst. Tech., Stockholm
002655508 700__ $$aSideras Haddad, Elias$$iINSPIRE-00508575$$jORCID:0000-0002-3206-395X$$uWitwatersrand U.
002655508 700__ $$aSidiropoulou, Ourania$$iINSPIRE-00377116$$jORCID:0000-0002-1285-1350$$uCERN
002655508 700__ $$aSidoti, Antonio$$iINSPIRE-00040767$$jORCID:0000-0002-3277-1999$$uINFN, Bologna$$uBologna U.
002655508 700__ $$aSiegert, Frank$$iINSPIRE-00004088$$jORCID:0000-0002-2893-6412$$uDresden, Tech. U.
002655508 700__ $$aSijacki, Djordje$$iINSPIRE-00126317$$uBelgrade U.
002655508 700__ $$aSilva, Jose Manuel$$iINSPIRE-00227185$$uLIP, Lisbon
002655508 700__ $$aSilva, Manuel Jr$$iINSPIRE-00549189$$jORCID:0000-0001-6940-8184$$uWisconsin U., Madison
002655508 700__ $$aSilva Oliveira, Marcos Vinicius$$iINSPIRE-00390428$$jORCID:0000-0003-2285-478X$$uJuiz de Fora U.
002655508 700__ $$aSilverstein, Samuel$$iINSPIRE-00223592$$jORCID:0000-0001-7734-7617$$uStockholm U.
002655508 700__ $$aSimic, Ljiljana$$iINSPIRE-00223604$$jORCID:0000-0001-7196-7655$$uDubna, JINR
002655508 700__ $$aSimion, Stefan$$iINSPIRE-00223610$$uOrsay, LAL
002655508 700__ $$aSimioni, Eduard$$iINSPIRE-00226165$$jORCID:0000-0002-8929-6236$$uMainz U.
002655508 700__ $$aSimon, Manuel$$iINSPIRE-00396523$$jORCID:0000-0002-0471-4305$$uMainz U.
002655508 700__ $$aSimoniello, Rosa$$iINSPIRE-00287242$$jORCID:0000-0003-2042-6394$$uMainz U.
002655508 700__ $$aSinervo, Pekka$$iINSPIRE-00126695$$jORCID:0000-0002-5128-2373$$uToronto U.
002655508 700__ $$aSinev, Nikolai$$iINSPIRE-00042060$$jORCID:0000-0003-3015-3879$$uOregon U.
002655508 700__ $$aSioli, Maximiliano$$iINSPIRE-00126783$$jORCID:0000-0002-0912-9121$$uINFN, Bologna$$uBologna U.
002655508 700__ $$aSiragusa, Giovanni$$iINSPIRE-00020730$$jORCID:0000-0003-3612-0410$$uWurzburg U.
002655508 700__ $$aSiral, Ismet$$iINSPIRE-00529755$$jORCID:0000-0003-4554-1831$$uMichigan U.
002655508 700__ $$aSivoklokov, Serguei$$iINSPIRE-00223641$$jORCID:0000-0003-0868-8164$$uLomonosov Moscow State U.
002655508 700__ $$aSjoelin, Joergen$$iINSPIRE-00180522$$jORCID:0000-0002-5285-8995$$uStockholm U.$$uStockholm U., OKC
002655508 700__ $$aSkubic, Patrick$$iINSPIRE-00127003$$jORCID:0000-0001-6342-9283$$uOklahoma U.
002655508 700__ $$aSlater, Mark$$iINSPIRE-00223675$$uBirmingham U.
002655508 700__ $$aSlavicek, Tomas$$iINSPIRE-00223682$$jORCID:0000-0001-8054-7345$$uPrague, Tech. U.
002655508 700__ $$aSlawinska, Magdalena$$iINSPIRE-00379172$$jORCID:0000-0002-9386-9092$$uCracow, INP
002655508 700__ $$aSliwa, Krzysztof$$iINSPIRE-00127092$$jORCID:0000-0002-1201-4771$$uTufts U.
002655508 700__ $$aSlovak, Radim$$iINSPIRE-00443411$$jORCID:0000-0002-9829-2237$$uCharles U.
002655508 700__ $$aSmakhtin, Vladimir$$iINSPIRE-00223693$$uWeizmann Inst.
002655508 700__ $$aSmart, Ben$$iINSPIRE-00237541$$jORCID:0000-0002-7192-4097$$uAnnecy, LAPP
002655508 700__ $$aSmiesko, Juraj$$iINSPIRE-00507669$$uComenius U.
002655508 700__ $$aSmirnov, Nikita$$iINSPIRE-00537849$$jORCID:0000-0003-3638-4838$$uMoscow Phys. Eng. Inst.
002655508 700__ $$aSmirnov, Sergei$$iINSPIRE-00184110$$jORCID:0000-0002-6778-073X$$uMoscow Phys. Eng. Inst.
002655508 700__ $$aSmirnov, Yury$$iINSPIRE-00287508$$jORCID:0000-0002-2891-0781$$uMoscow Phys. Eng. Inst.
002655508 700__ $$aSmirnova, Lidia$$iINSPIRE-00223701$$jORCID:0000-0002-0447-2975$$uLomonosov Moscow State U.
002655508 700__ $$aSmirnova, Oxana$$iINSPIRE-00223710$$jORCID:0000-0003-2517-531X$$uLund U.
002655508 700__ $$aSmith, Joshua Wyatt$$iINSPIRE-00529764$$jORCID:0000-0003-1819-4985$$uGottingen U., II. Phys. Inst.
002655508 700__ $$aSmith, Matthew$$iINSPIRE-00382246$$uNevis Labs, Columbia U.
002655508 700__ $$aSmizanska, Maria$$iINSPIRE-00127348$$jORCID:0000-0002-3777-4734$$uLancaster U.
002655508 700__ $$aSmolek, Karel$$iINSPIRE-00223725$$jORCID:0000-0002-5996-7000$$uPrague, Tech. U.
002655508 700__ $$aSmykiewicz, Andrzej$$iINSPIRE-00571596$$uCracow, INP
002655508 700__ $$aSnesarev, Andrei$$iINSPIRE-00223739$$jORCID:0000-0002-9067-8362$$uLebedev Inst.
002655508 700__ $$aSnyder, Ian Michael$$iINSPIRE-00529778$$jORCID:0000-0001-7775-7915$$uOregon U.
002655508 700__ $$aSnyder, Scott$$iINSPIRE-00300553$$jORCID:0000-0001-8610-8423$$uBrookhaven
002655508 700__ $$aSobie, Randall$$iINSPIRE-00127469$$uVictoria U.$$uIPP, Canada
002655508 700__ $$aSoffa, Aaron Michael$$iINSPIRE-00572721$$uUC, Irvine
002655508 700__ $$aSoffer, Abner$$iINSPIRE-00127510$$jORCID:0000-0002-0749-2146$$uTel Aviv U.
002655508 700__ $$aSogaard, Andreas$$iINSPIRE-00547687$$jORCID:0000-0002-0823-056X$$uEdinburgh U.
002655508 700__ $$aSu, Daxian$$iINSPIRE-00227270$$uTaiwan, Inst. Phys.
002655508 700__ $$aSokhrannyi, Grygorii$$iINSPIRE-00418133$$uStefan Inst., Ljubljana
002655508 700__ $$aSolans, Carlos$$iINSPIRE-00306293$$jORCID:0000-0002-0518-4086$$uCERN
002655508 700__ $$aSolar, Michael$$iINSPIRE-00223750$$uPrague, Tech. U.
002655508 700__ $$aSoldatov, Evgeny$$iINSPIRE-00237550$$jORCID:0000-0003-0694-3272$$uMoscow Phys. Eng. Inst.
002655508 700__ $$aSoldevila- Serrano, Urmila$$iINSPIRE-00232570$$jORCID:0000-0002-7674-7878$$uValencia U., IFIC
002655508 700__ $$aSolodkov, Alexander$$iINSPIRE-00127668$$jORCID:0000-0002-2737-8674$$uSerpukhov, IHEP
002655508 700__ $$aSoloshenko, Alexei$$iINSPIRE-00368534$$jORCID:0000-0001-9946-8188$$uDubna, JINR
002655508 700__ $$aSolovyanov, Oleg$$iINSPIRE-00223789$$jORCID:0000-0002-2598-5657$$uSerpukhov, IHEP
002655508 700__ $$aSolovyev, Victor$$iINSPIRE-00287277$$jORCID:0000-0002-9402-6329$$uSt. Petersburg, INP
002655508 700__ $$aSommer, Philip$$iINSPIRE-00364294$$jORCID:0000-0003-1703-7304$$uSheffield U.
002655508 700__ $$aSon, Hyungsuk$$iINSPIRE-00247667$$jORCID:0000-0003-2225-9024$$uTufts U.
002655508 700__ $$aSong, Weimin$$iINSPIRE-00408810$$jORCID:0000-0003-1376-2293$$uRutherford
002655508 700__ $$aSong, Wen Yi$$iINSPIRE-00584032$$uYork U., Canada
002655508 700__ $$aSopczak, Andre$$iINSPIRE-00127812$$jORCID:0000-0001-6981-0544$$uPrague, Tech. U.
002655508 700__ $$aSopkova, Filomena$$iINSPIRE-00573398$$uKosice, IEF
002655508 700__ $$aSosa Corral, David Eduardo$$iINSPIRE-00365541$$uHeidelberg U.
002655508 700__ $$aSotiropoulou, Calliope Louisa$$iINSPIRE-00380743$$jORCID:0000-0001-9851-1658$$uINFN, Pisa$$uPisa U.
002655508 700__ $$aSottocornola, Simone$$iINSPIRE-00568855$$uINFN, Pavia$$uPavia U.
002655508 700__ $$aSoualah, Rachik$$iINSPIRE-00237567$$jORCID:0000-0003-0124-3410$$uINFN, Udine$$uUdine U.$$uKUSTAR, Sharjah
002655508 700__ $$aSoukharev, Andrey$$iINSPIRE-00223813$$jORCID:0000-0002-2210-0913$$uNovosibirsk State U.$$uNovosibirsk, IYF
002655508 700__ $$aSouth, David$$iINSPIRE-00185821$$uDESY
002655508 700__ $$aSowden, Benjamin Charles$$iINSPIRE-00403960$$jORCID:0000-0002-6316-2870$$uRoyal Holloway, U. of London
002655508 700__ $$aSpagnolo, Stefania$$iINSPIRE-00146499$$jORCID:0000-0001-7482-6348$$uINFN, Lecce$$uSalento U.
002655508 700__ $$aSpalla, Margherita$$iINSPIRE-00393248$$jORCID:0000-0001-5813-1693$$uMunich, Max Planck Inst.
002655508 700__ $$aSpangenberg, Martin$$iINSPIRE-00396616$$uWarwick U.
002655508 700__ $$aSpano, Francesco$$iINSPIRE-00051714$$jORCID:0000-0002-6551-1878$$uRoyal Holloway, U. of London
002655508 700__ $$aSperlich, Dennis$$iINSPIRE-00407979$$jORCID:0000-0003-4454-6999$$uHumboldt U., Berlin
002655508 700__ $$aSpettel, Fabian$$iINSPIRE-00366625$$uMunich, Max Planck Inst.
002655508 700__ $$aSpieker, Thomas Malte$$iINSPIRE-00535066$$jORCID:0000-0002-9408-895X$$uKirchhoff Inst. Phys.
002655508 700__ $$aSpighi, Roberto$$iINSPIRE-00223820$$jORCID:0000-0001-8301-8588$$uINFN, Bologna
002655508 700__ $$aSpigo, Giancarlo$$iINSPIRE-00223836$$uCERN
002655508 700__ $$aSpiller, Laurence Anthony$$iINSPIRE-00413161$$jORCID:0000-0002-5650-7586$$uMelbourne U.
002655508 700__ $$aSpiteri, Dwayne Patrick$$iINSPIRE-00639250$$jORCID:0000-0002-9226-2539$$uGlasgow U.
002655508 700__ $$aSpousta, Martin$$iINSPIRE-00223860$$jORCID:0000-0001-5644-9526$$uCharles U.
002655508 700__ $$aStabile, Alberto$$iINSPIRE-00380950$$jORCID:0000-0002-6868-8329$$uINFN, Milan$$uMilan U.
002655508 700__ $$aStamen, Rainer$$iINSPIRE-00223881$$jORCID:0000-0001-7282-949X$$uKirchhoff Inst. Phys.
002655508 700__ $$aStamm, Soren$$iINSPIRE-00374679$$uHumboldt U., Berlin
002655508 700__ $$aStanecka, Ewa$$iINSPIRE-00223897$$jORCID:0000-0003-2546-0516$$uCracow, INP
002655508 700__ $$aStanek, Robert$$iINSPIRE-00128391$$uArgonne
002655508 700__ $$aStanescu, Cristian$$iINSPIRE-00128407$$uINFN, Rome3
002655508 700__ $$aStanislaus, Beojan$$iINSPIRE-00580305$$jORCID:0000-0001-9007-7658$$uOxford U.
002655508 700__ $$aStanitzki, Marcel Michael$$iINSPIRE-00006638$$uDESY
002655508 700__ $$aStapf, Birgit Sylvia$$iINSPIRE-00548935$$jORCID:0000-0001-5374-6402$$uFOM, Amsterdam
002655508 700__ $$aStapnes, Steinar$$iINSPIRE-00223901$$uOslo U.
002655508 700__ $$aStarchenko, Evgeny$$iINSPIRE-00223911$$jORCID:0000-0002-8495-0630$$uSerpukhov, IHEP
002655508 700__ $$aStark, Giordon Holtsberg$$iINSPIRE-00434905$$jORCID:0000-0001-6616-3433$$uChicago U., EFI
002655508 700__ $$aStark, Jan$$iINSPIRE-00050567$$jORCID:0000-0002-1217-672X$$uLPSC, Grenoble
002655508 700__ $$aStark, Simon Holm$$iINSPIRE-00399764$$jORCID:0000-0002-7480-7611$$uBohr Inst.
002655508 700__ $$aStaroba, Pavel$$iINSPIRE-00223923$$jORCID:0000-0001-6009-6321$$uPrague, Inst. Phys.
002655508 700__ $$aStarovoitov, Pavel$$iINSPIRE-00223937$$jORCID:0000-0003-1990-0992$$uKirchhoff Inst. Phys.
002655508 700__ $$aStaerz, Steffen$$iINSPIRE-00364781$$jORCID:0000-0002-2908-3909$$uCERN
002655508 700__ $$aStaszewski, Rafal$$iINSPIRE-00237571$$jORCID:0000-0001-7708-9259$$uCracow, INP
002655508 700__ $$aStegler, Martin$$iINSPIRE-00548940$$uDESY
002655508 700__ $$aSteinberg, Peter$$iINSPIRE-00256449$$jORCID:0000-0002-5349-8370$$uBrookhaven
002655508 700__ $$aStelzer, Bernd$$iINSPIRE-00040738$$jORCID:0000-0003-4091-1784$$uSimon Fraser U.
002655508 700__ $$aStelzer, Harald Joerg$$iINSPIRE-00027247$$jORCID:0000-0003-0690-8573$$uCERN
002655508 700__ $$aStelzer-Chilton, Oliver$$iINSPIRE-00040726$$jORCID:0000-0002-0791-9728$$uTRIUMF
002655508 700__ $$aStenzel, Hasko$$iINSPIRE-00128831$$jORCID:0000-0002-4185-6484$$uGiessen U.
002655508 700__ $$aStevenson, Thomas James$$iINSPIRE-00533054$$jORCID:0000-0003-2399-8945$$uQueen Mary, U. of London
002655508 700__ $$aStewart, Graeme$$iINSPIRE-00226135$$jORCID:0000-0003-0182-7088$$uCERN
002655508 700__ $$aStockton, Mark$$iINSPIRE-00223972$$uOregon U.
002655508 700__ $$aStoicea, Gabriel$$iINSPIRE-00185869$$jORCID:0000-0002-7511-4614$$uBucharest, IFIN-HH
002655508 700__ $$aStolte, Philipp$$iINSPIRE-00362178$$jORCID:0000-0002-8828-3564$$uGottingen U., II. Phys. Inst.
002655508 700__ $$aStonjek, Stefan$$iINSPIRE-00027833$$jORCID:0000-0001-7582-6227$$uMunich, Max Planck Inst.
002655508 700__ $$aStraessner, Arno$$iINSPIRE-00129196$$jORCID:0000-0003-2460-6659$$uDresden, Tech. U.
002655508 700__ $$aStrandberg, Jonas$$iINSPIRE-00038640$$jORCID:0000-0002-8913-0981$$uRoyal Inst. Tech., Stockholm
002655508 700__ $$aStrandberg, Sara Kristina$$iINSPIRE-00024662$$jORCID:0000-0001-7253-7497$$uStockholm U.$$uStockholm U., OKC
002655508 700__ $$aStrauss, Michael$$iINSPIRE-00129297$$jORCID:0000-0002-0465-5472$$uOklahoma U.
002655508 700__ $$aStrizenec, Pavol$$iINSPIRE-00129337$$jORCID:0000-0003-0958-7656$$uKosice, IEF
002655508 700__ $$aStroehmer, Raimund$$iINSPIRE-00129353$$jORCID:0000-0002-0062-2438$$uWurzburg U.
002655508 700__ $$aStrom, David$$iINSPIRE-00129396$$jORCID:0000-0002-8302-386X$$uOregon U.
002655508 700__ $$aStroynowski, Ryszard$$iINSPIRE-00129434$$jORCID:0000-0002-7863-3778$$uSouthern Methodist U.
002655508 700__ $$aStruebig, Antonia$$iINSPIRE-00371025$$jORCID:0000-0002-2382-6951$$uEdinburgh U.
002655508 700__ $$aStucci, Stefania Antonia$$iINSPIRE-00353969$$jORCID:0000-0002-1639-4484$$uBrookhaven
002655508 700__ $$aStugu, Bjarne$$iINSPIRE-00129469$$jORCID:0000-0002-1728-9272$$uBergen U.
002655508 700__ $$aStupak, John$$iINSPIRE-00232658$$jORCID:0000-0001-9610-0783$$uOklahoma U.
002655508 700__ $$aStyles, Nicholas Adam$$iINSPIRE-00049529$$jORCID:0000-0001-6976-9457$$uDESY
002655508 700__ $$aSu, Dong$$iINSPIRE-00224038$$jORCID:0000-0001-6980-0215$$uSLAC
002655508 700__ $$aSu, Jun$$iINSPIRE-00354087$$uPittsburgh U.
002655508 700__ $$aSuchek, Stanislav$$iINSPIRE-00366364$$jORCID:0000-0002-8066-0409$$uKirchhoff Inst. Phys.
002655508 700__ $$aSugaya, Yorihito$$iINSPIRE-00224054$$uOsaka U.
002655508 700__ $$aSuk, Michal$$iINSPIRE-00224089$$uPrague, Tech. U.
002655508 700__ $$aSulin, Vladimir$$iINSPIRE-00224090$$jORCID:0000-0003-3943-2495$$uLebedev Inst.
002655508 700__ $$aSultan, Dms$$iINSPIRE-00548956$$jORCID:0000-0003-2925-279X$$uGeneva U.
002655508 700__ $$aSultanov, Saleh$$iINSPIRE-00009070$$uTOBB ETU, Ankara
002655508 700__ $$aSumida, Toshi$$iINSPIRE-00129684$$jORCID:0000-0002-2685-6187$$uKyoto U.
002655508 700__ $$aSun, Siyuan$$iINSPIRE-00375257$$jORCID:0000-0001-8802-7184$$uMichigan U.
002655508 700__ $$aSun, Xiaohu$$iINSPIRE-00226957$$jORCID:0000-0003-4409-4574$$uAlberta U.
002655508 700__ $$aSuruliz, Kerim$$iINSPIRE-00224106$$jORCID:0000-0002-1976-3716$$uSussex U.
002655508 700__ $$aSuster, Carl$$iINSPIRE-00511778$$jORCID:0000-0001-7021-9380$$uSydney U.
002655508 700__ $$aSutton, Mark$$iINSPIRE-00129913$$uSussex U.
002655508 700__ $$aSuzuki, Shota$$iINSPIRE-00394929$$jORCID:0000-0001-6906-4465$$uKEK, Tsukuba
002655508 700__ $$aSvatos, Michal$$iINSPIRE-00237645$$jORCID:0000-0002-7199-3383$$uPrague, Inst. Phys.
002655508 700__ $$aSwiatlowski, Maximilian J$$iINSPIRE-00333637$$jORCID:0000-0001-7287-0468$$uChicago U., EFI
002655508 700__ $$aSwift, Stewart Patrick$$iINSPIRE-00529784$$uSUNY, Albany
002655508 700__ $$aSydorenko, Alexander$$iINSPIRE-00572731$$uMainz U.
002655508 700__ $$aSykora, Ivan$$iINSPIRE-00224134$$jORCID:0000-0003-3447-5621$$uComenius U.
002655508 700__ $$aSykora, Tomas$$iINSPIRE-00185883$$jORCID:0000-0001-9585-7215$$uCharles U.
002655508 700__ $$aTa, Duc Bao$$iINSPIRE-00224156$$jORCID:0000-0002-0918-9175$$uMainz U.
002655508 700__ $$aTackmann, Kerstin$$iINSPIRE-00024648$$jORCID:0000-0003-3917-3761$$uDESY$$uHamburg U.
002655508 700__ $$aKinghorn-taenzer, Joseph Peter$$iINSPIRE-00354235$$uTel Aviv U.
002655508 700__ $$aTaffard, Anyes$$iINSPIRE-00054866$$jORCID:0000-0002-5800-4798$$uUC, Irvine
002655508 700__ $$aTafirout, Reda$$iINSPIRE-00224168$$uTRIUMF
002655508 700__ $$aTahirovic, Elvedin$$iINSPIRE-00400833$$jORCID:0000-0001-8538-918X$$uQueen Mary, U. of London
002655508 700__ $$aTaiblum, Nimrod$$iINSPIRE-00232703$$uTel Aviv U.
002655508 700__ $$aTakai, Helio$$iINSPIRE-99155656$$jORCID:0000-0001-9253-8307$$uBrookhaven
002655508 700__ $$aTakashima, Ryuichi$$iINSPIRE-00130375$$uKyoto U. of Education
002655508 700__ $$aTakasugi, Eric Hayato$$iINSPIRE-00288539$$uMunich, Max Planck Inst.
002655508 700__ $$aTakeda, Kosuke$$iINSPIRE-00567831$$jORCID:0000-0002-2611-8563$$uKobe U.
002655508 700__ $$aTakeshita, Tohru$$iINSPIRE-00224192$$uShinshu U.
002655508 700__ $$aTakubo, Yosuke$$iINSPIRE-00237659$$uKEK, Tsukuba
002655508 700__ $$aTalby, Mossadek$$iINSPIRE-00224200$$jORCID:0000-0001-9985-6033$$uMarseille, CPPM
002655508 700__ $$aTalyshev, Alexey$$iINSPIRE-00224212$$uNovosibirsk State U.$$uNovosibirsk, IYF
002655508 700__ $$aTanaka, Junichi$$iINSPIRE-00224238$$jORCID:0000-0001-9994-5802$$uTokyo U., ICEPP
002655508 700__ $$aTanaka, Masahiro$$iINSPIRE-00514556$$uTokyo Inst. Tech.
002655508 700__ $$aTanaka, Reisaburo$$iINSPIRE-00130555$$uOrsay, LAL
002655508 700__ $$aTannenwald, Benjamin Bordy$$iINSPIRE-00375951$$jORCID:0000-0002-5570-8095$$uOhio State U.
002655508 700__ $$aTapia Araya, Sebastian$$iINSPIRE-00424626$$jORCID:0000-0002-3659-7270$$uSanta Maria U., Valparaiso
002655508 700__ $$aTapprogge, Stefan$$iINSPIRE-00141544$$jORCID:0000-0003-1251-3332$$uMainz U.
002655508 700__ $$aTarek Abouelfadl Mohamed, Ahmed$$iINSPIRE-00574959$$uParis U., VI-VII
002655508 700__ $$aTarem, Shlomit$$iINSPIRE-00130701$$jORCID:0000-0002-9296-7272$$uTechnion
002655508 700__ $$aTarna, Grigore$$iINSPIRE-00575817$$jORCID:0000-0002-5060-2208$$uBucharest, IFIN-HH$$uMarseille, CPPM
002655508 700__ $$aTartarelli, Giuseppe Francesco$$iINSPIRE-00130743$$jORCID:0000-0002-4244-502X$$uINFN, Milan
002655508 700__ $$aTas, Petr$$iINSPIRE-00306326$$jORCID:0000-0001-5785-7548$$uCharles U.
002655508 700__ $$aTasevsky, Marek$$iINSPIRE-00224260$$jORCID:0000-0002-1535-9732$$uPrague, Inst. Phys.
002655508 700__ $$aTashiro, Takuya$$iINSPIRE-00340474$$uKyoto U.
002655508 700__ $$aTassi, Enrico$$iINSPIRE-00172313$$jORCID:0000-0002-3335-6500$$uINFN, Cosenza$$uCalabria U.
002655508 700__ $$aTavares Delgado, Ademar$$iINSPIRE-00342767$$uLIP, Lisbon$$uLisbon U., CFNUL
002655508 700__ $$aTayalati, Yahya$$iINSPIRE-00295930$$uMohammed V U., Agdal
002655508 700__ $$aTaylor, Aaron$$iINSPIRE-00388427$$uNew Mexico U.
002655508 700__ $$aTaylor, Alan James$$iINSPIRE-00566500$$uEdinburgh U.
002655508 700__ $$aTaylor, Geoffrey$$iINSPIRE-00130854$$jORCID:0000-0002-1831-4871$$uMelbourne U.
002655508 700__ $$aTaylor, Pierre Thor Elliot$$iINSPIRE-00418209$$uMelbourne U.
002655508 700__ $$aTaylor, Wendy$$iINSPIRE-00301147$$jORCID:0000-0002-6596-9125$$uYork U., Canada
002655508 700__ $$aTee, Amy Selvi$$iINSPIRE-00580317$$uLancaster U.
002655508 700__ $$aTeixeira-Dias, Pedro$$iINSPIRE-00130949$$jORCID:0000-0001-9977-3836$$uRoyal Holloway, U. of London
002655508 700__ $$aTen Kate, Herman$$iINSPIRE-00224330$$uCERN
002655508 700__ $$aTeng, Ping-Kun$$iINSPIRE-00040709$$uTaiwan, Inst. Phys.
002655508 700__ $$aTeoh, Jia Jian$$iINSPIRE-00371033$$uFOM, Amsterdam
002655508 700__ $$aTepel, Fabian-Phillipp$$iINSPIRE-00379384$$uWuppertal U.
002655508 700__ $$aTerada, Susumu$$iINSPIRE-00224350$$uKEK, Tsukuba
002655508 700__ $$aTerashi, Koji$$iINSPIRE-00131056$$jORCID:0000-0001-6520-8070$$uTokyo U., ICEPP
002655508 700__ $$aTerron, Juan$$iINSPIRE-00145489$$jORCID:0000-0003-0132-5723$$uMadrid, Autonoma U.
002655508 700__ $$aTerzo, Stefano$$iINSPIRE-00349918$$jORCID:0000-0003-3388-3906$$uBarcelona, IFAE
002655508 700__ $$aTesta, Marianna$$iINSPIRE-00224377$$jORCID:0000-0003-1274-8967$$uFrascati
002655508 700__ $$aTeuscher, Richard$$iINSPIRE-00131201$$jORCID:0000-0002-8768-2272$$uToronto U.$$uIPP, Canada
002655508 700__ $$aThais, Savannah Jennifer$$iINSPIRE-00567186$$jORCID:0000-0001-8214-2763$$uYale U.
002655508 700__ $$aTheveneaux-Pelzer, Timothee$$iINSPIRE-00224394$$jORCID:0000-0002-9746-4172$$uDESY
002655508 700__ $$aThiele, Fabian$$iINSPIRE-00562266$$jORCID:0000-0002-6620-9734$$uBohr Inst.
002655508 700__ $$aThomas, David William$$iINSPIRE-00584607$$uRoyal Holloway, U. of London
002655508 700__ $$aThomas, Juergen$$iINSPIRE-00224412$$jORCID:0000-0001-6965-6604$$uBirmingham U.
002655508 700__ $$aThompson, Stan$$iINSPIRE-00131382$$uGlasgow U.
002655508 700__ $$aThompson, Paul$$iINSPIRE-00185894$$jORCID:0000-0002-6239-7715$$uBirmingham U.
002655508 700__ $$aThomsen, Lotte Ansgaard$$iINSPIRE-00287293$$jORCID:0000-0002-3855-5357$$uYale U.
002655508 700__ $$aThomson, Evelyn$$iINSPIRE-00300284$$jORCID:0000-0001-6031-2768$$uPennsylvania U.
002655508 700__ $$aTian, Yun$$iINSPIRE-00566519$$jORCID:0000-0002-4686-0634$$uNevis Labs, Columbia U.
002655508 700__ $$aTicse Torres, Royer Edson$$iINSPIRE-00388508$$jORCID:0000-0001-8178-5257$$uGottingen U., II. Phys. Inst.
002655508 700__ $$aTikhomirov, Vladimir$$iINSPIRE-00306337$$jORCID:0000-0002-9634-0581$$uLebedev Inst.$$uMoscow Phys. Eng. Inst.
002655508 700__ $$aTikhonov, Yury$$iINSPIRE-00198040$$jORCID:0000-0002-8023-6448$$uNovosibirsk State U.$$uNovosibirsk, IYF
002655508 700__ $$aTimoshenko, Sergey$$iINSPIRE-00183342$$uMoscow Phys. Eng. Inst.
002655508 700__ $$aTipton, Paul$$iINSPIRE-00131560$$jORCID:0000-0002-3698-3585$$uYale U.
002655508 700__ $$aTisserant, Sylvain$$iINSPIRE-00131587$$jORCID:0000-0002-0294-6727$$uMarseille, CPPM
002655508 700__ $$aTodome, Kazuki$$iINSPIRE-00410948$$jORCID:0000-0003-2445-1132$$uTokyo Inst. Tech.
002655508 700__ $$aTodorova-Nova, Sharka$$iINSPIRE-00224498$$jORCID:0000-0003-2433-231X$$uAnnecy, LAPP
002655508 700__ $$aTodt, Stefanie$$iINSPIRE-00529800$$uDresden, Tech. U.
002655508 700__ $$aTojo, Junji$$iINSPIRE-00243319$$jORCID:0000-0003-4666-3208$$uKyushu U.
002655508 700__ $$aTokar, Stanislav$$iINSPIRE-00131686$$jORCID:0000-0001-8777-0590$$uComenius U.
002655508 700__ $$aTokushuku, Katsuo$$iINSPIRE-00173305$$jORCID:0000-0002-8262-1577$$uKEK, Tsukuba
002655508 700__ $$aTolley, Emma$$iINSPIRE-00377126$$uOhio State U.
002655508 700__ $$aTomiwa, Kehinde Gbenga$$iINSPIRE-00639268$$jORCID:0000-0002-8580-9145$$uWitwatersrand U.
002655508 700__ $$aTomoto, Makoto$$iINSPIRE-00131811$$jORCID:0000-0002-4603-2070$$uNagoya U.
002655508 700__ $$aTompkins, Lauren$$iINSPIRE-00059527$$jORCID:0000-0001-8127-9653$$uSLAC$$uStanford U., Phys. Dept.
002655508 700__ $$aToms, Konstantin$$iINSPIRE-00224527$$uNew Mexico U.
002655508 700__ $$aTong, Baojia$$iINSPIRE-00436984$$jORCID:0000-0003-2430-8870$$uHarvard U., Phys. Dept.
002655508 700__ $$aTornambe, Peter$$iINSPIRE-00529818$$jORCID:0000-0003-1129-9792$$uFreiburg U.
002655508 700__ $$aTorrence, Eric$$iINSPIRE-00144881$$jORCID:0000-0003-2911-8910$$uOregon U.
002655508 700__ $$aTorres, Heberth$$iINSPIRE-00237687$$jORCID:0000-0003-0822-1206$$uDresden, Tech. U.
002655508 700__ $$aTorro Pastor, Emma$$iINSPIRE-00224567$$jORCID:0000-0002-5507-7924$$uWashington U., Seattle
002655508 700__ $$aTosciri, Cecilia$$iINSPIRE-00571611$$jORCID:0000-0001-6485-2227$$uOxford U.
002655508 700__ $$aToth, Jozsef$$iINSPIRE-00226986$$jORCID:0000-0001-9128-6080$$uMarseille, CPPM$$uBudapest, RMKI
002655508 700__ $$aTouchard, Francois$$iINSPIRE-00224579$$jORCID:0000-0002-8674-0266$$uMarseille, CPPM
002655508 700__ $$aTovey, Daniel$$iINSPIRE-00224589$$uSheffield U.
002655508 700__ $$aTreado, Colleen Jennifer$$iINSPIRE-00534702$$jORCID:0000-0002-0902-491X$$uNew York U.
002655508 700__ $$aTrefzger, Thomas$$iINSPIRE-00224598$$jORCID:0000-0002-9820-1729$$uWurzburg U.
002655508 700__ $$aTresoldi, Fabio$$iINSPIRE-00542436$$jORCID:0000-0002-3806-6895$$uSussex U.
002655508 700__ $$aTricoli, Alessandro$$iINSPIRE-00224619$$jORCID:0000-0002-8224-6105$$uBrookhaven
002655508 700__ $$aTrigger, Isabel Marian$$iINSPIRE-00132228$$jORCID:0000-0002-6127-5847$$uTRIUMF
002655508 700__ $$aTrincaz-Duvoid, Sophie$$iINSPIRE-00132232$$jORCID:0000-0001-5913-0828$$uParis U., VI-VII
002655508 700__ $$aTripiana, Martin$$iINSPIRE-00224624$$uBarcelona, IFAE
002655508 700__ $$aTrischuk, William$$iINSPIRE-00132286$$uToronto U.
002655508 700__ $$aTrocme, Benjamin$$iINSPIRE-00224658$$jORCID:0000-0001-9500-2487$$uLPSC, Grenoble
002655508 700__ $$aTrofymov, Artur$$iINSPIRE-00443508$$jORCID:0000-0001-7688-5165$$uOrsay, LAL
002655508 700__ $$aTroncon, Clara$$iINSPIRE-00132324$$jORCID:0000-0002-7997-8524$$uINFN, Milan
002655508 700__ $$aTrovatelli, Monica$$iINSPIRE-00335615$$jORCID:0000-0001-9566-6187$$uVictoria U.
002655508 700__ $$aTrovato, Fabrizio$$iINSPIRE-00580329$$jORCID:0000-0003-1041-9131$$uSussex U.
002655508 700__ $$aTruong, Loan$$iINSPIRE-00444174$$jORCID:0000-0001-8249-7150$$uJohannesburg U.
002655508 700__ $$aTrzebinski, Maciej$$iINSPIRE-00237700$$jORCID:0000-0002-5151-7101$$uCracow, INP
002655508 700__ $$aTrzupek, Adam$$iINSPIRE-00256459$$jORCID:0000-0001-6938-5867$$uCracow, INP
002655508 700__ $$aTsai, Fang-ying$$iINSPIRE-00578869$$jORCID:0000-0001-7878-6435$$uDESY
002655508 700__ $$aTseng, Jeffrey$$iINSPIRE-00224674$$jORCID:0000-0003-1731-5853$$uOxford U.
002655508 700__ $$aTsiareshka, Pavel$$iINSPIRE-00224691$$uMinsk, Inst. Phys.
002655508 700__ $$aTsirigotis, Apostolos$$iINSPIRE-00642210$$uAristotle U., Thessaloniki
002655508 700__ $$aTsirintanis, Nikolaos$$iINSPIRE-00346988$$uAthens Natl. Capodistrian U.
002655508 700__ $$aTsiskaridze, Vakhtang$$iINSPIRE-00224710$$uSUNY, Stony Brook
002655508 700__ $$aTskhadadze, Edisher$$iINSPIRE-00224724$$uTbilisi, Inst. Phys.
002655508 700__ $$aTsukerman, Ilya$$iINSPIRE-00224734$$jORCID:0000-0002-8965-6676$$uMoscow, ITEP
002655508 700__ $$aTsulaia, Vakhtang$$iINSPIRE-00224746$$jORCID:0000-0001-8157-6711$$uLBL, Berkeley
002655508 700__ $$aTsuno, Soshi$$iINSPIRE-00040679$$jORCID:0000-0002-2055-4364$$uKEK, Tsukuba
002655508 700__ $$aTsybychev, Dmitri$$iINSPIRE-00132531$$jORCID:0000-0001-8212-6894$$uSUNY, Stony Brook
002655508 700__ $$aTu, Yanjun$$iINSPIRE-00024619$$jORCID:0000-0002-5865-183X$$uHong Kong U.
002655508 700__ $$aTudorache, Alexandra$$iINSPIRE-00237716$$jORCID:0000-0001-6307-1437$$uBucharest, IFIN-HH
002655508 700__ $$aTudorache, Valentina$$iINSPIRE-00237721$$jORCID:0000-0001-5384-3843$$uBucharest, IFIN-HH
002655508 700__ $$aTulbure, Traian Tiberiu$$iINSPIRE-00517222$$uTransilvania U., Brasov
002655508 700__ $$aTuna, Alexander Naip$$iINSPIRE-00337698$$jORCID:0000-0002-7672-7754$$uHarvard U., Phys. Dept.
002655508 700__ $$aTurchikhin, Semen$$iINSPIRE-00342946$$jORCID:0000-0001-6506-3123$$uDubna, JINR
002655508 700__ $$aTurgeman, Daniel$$iINSPIRE-00437130$$uWeizmann Inst.
002655508 700__ $$aTurk Cakir, Ilkay$$iINSPIRE-00224776$$uIstanbul Aydin U.$$uGiresun U.
002655508 700__ $$aTurra, Ruggero$$iINSPIRE-00237738$$jORCID:0000-0001-8740-796X$$uINFN, Milan
002655508 700__ $$aTuts, Michael$$iINSPIRE-00132751$$jORCID:0000-0001-6131-5725$$uNevis Labs, Columbia U.
002655508 700__ $$aTzovara, Eftychia$$iINSPIRE-00577550$$uMainz U.
002655508 700__ $$aUcchielli, Giulia$$iINSPIRE-00444244$$jORCID:0000-0002-9137-4475$$uINFN, Bologna$$uBologna U.
002655508 700__ $$aUeda, Ikuo$$iINSPIRE-00224805$$jORCID:0000-0002-6833-4344$$uKEK, Tsukuba
002655508 700__ $$aUghetto, Michael$$iINSPIRE-00334596$$jORCID:0000-0002-3814-454X$$uStockholm U.$$uStockholm U., OKC
002655508 700__ $$aUkegawa, Fumihiko$$iINSPIRE-00132910$$jORCID:0000-0002-9813-7931$$uTsukuba U.
002655508 700__ $$aUnal, Guillaume$$iINSPIRE-00132979$$jORCID:0000-0001-8130-7423$$uCERN
002655508 700__ $$aUndrus, Alexander$$iINSPIRE-00132984$$jORCID:0000-0002-1384-286X$$uBrookhaven
002655508 700__ $$aUnel, Gokhan$$iINSPIRE-00132990$$jORCID:0000-0002-3274-6531$$uUC, Irvine
002655508 700__ $$aUngaro, Francesca$$iINSPIRE-00334608$$jORCID:0000-0003-2005-595X$$uMelbourne U.
002655508 700__ $$aUnno, Yoshinobu$$iINSPIRE-00133014$$jORCID:0000-0002-4170-8537$$uKEK, Tsukuba
002655508 700__ $$aUno, Kenta$$iINSPIRE-00565032$$jORCID:0000-0002-2209-8198$$uTokyo U., ICEPP
002655508 700__ $$aUrban, Jozef$$iINSPIRE-00244950$$uKosice, IEF
002655508 700__ $$aUrquijo, Phillip$$iINSPIRE-00227284$$jORCID:0000-0002-0887-7953$$uMelbourne U.
002655508 700__ $$aUrrejola, Pedro$$iINSPIRE-00226996$$uMainz U.
002655508 700__ $$aUsai, Giulio$$iINSPIRE-00224879$$uTexas U., Arlington
002655508 700__ $$aUsui, Junya$$iINSPIRE-00529820$$uKEK, Tsukuba
002655508 700__ $$aVacavant, Laurent$$iINSPIRE-00179395$$jORCID:0000-0001-8964-0327$$uMarseille, CPPM
002655508 700__ $$aVacek, Vaclav$$iINSPIRE-00227000$$uPrague, Tech. U.
002655508 700__ $$aVachon, Brigitte$$iINSPIRE-00056509$$jORCID:0000-0001-8703-6978$$uMcGill U.
002655508 700__ $$aVadla, Knut Oddvar Hoie$$iINSPIRE-00560841$$jORCID:0000-0001-6729-1584$$uOslo U.
002655508 700__ $$aVaidya, Amal$$iINSPIRE-00559317$$jORCID:0000-0003-4086-9432$$uUniversity Coll. London
002655508 700__ $$aValderanis, Chrysostomos$$iINSPIRE-00232811$$jORCID:0000-0001-9362-8451$$uMunich U.
002655508 700__ $$aValdes Santurio, Eduardo$$iINSPIRE-00441276$$jORCID:0000-0001-9931-2896$$uStockholm U.$$uStockholm U., OKC
002655508 700__ $$aValente, Marco$$iINSPIRE-00562277$$jORCID:0000-0002-0486-9569$$uGeneva U.
002655508 700__ $$aValentinetti, Sara$$iINSPIRE-00224911$$jORCID:0000-0003-2044-6539$$uINFN, Bologna$$uBologna U.
002655508 700__ $$aValero, Alberto$$iINSPIRE-00306349$$uValencia U., IFIC
002655508 700__ $$aValery, Loic$$iINSPIRE-00334610$$jORCID:0000-0002-5510-1111$$uDESY
002655508 700__ $$aVallance, Robert Adam$$iINSPIRE-00580330$$jORCID:0000-0002-6782-1941$$uBirmingham U.
002655508 700__ $$aVallier, Alexis Roger Louis$$iINSPIRE-00392294$$uAnnecy, LAPP
002655508 700__ $$aValls Ferrer, Juan Antonio$$iINSPIRE-00224946$$uValencia U., IFIC
002655508 700__ $$aVan Daalen, Tal Roelof$$iINSPIRE-00579720$$jORCID:0000-0002-2254-125X$$uBarcelona, IFAE
002655508 700__ $$avan der Graaf, Harry$$iINSPIRE-00224951$$jORCID:0000-0003-2833-8647$$uFOM, Amsterdam
002655508 700__ $$aVan Gemmeren, Peter$$iINSPIRE-00084279$$jORCID:0000-0002-7227-4006$$uArgonne
002655508 700__ $$aVan Nieuwkoop, Jacobus$$iINSPIRE-00354211$$uSimon Fraser U.
002655508 700__ $$aVan Vulpen, Ivo$$iINSPIRE-00225014$$jORCID:0000-0001-7074-5655$$uFOM, Amsterdam
002655508 700__ $$aVanadia, Marco$$iINSPIRE-00237763$$jORCID:0000-0003-2684-276X$$uINFN, Rome2$$uRome U., Tor Vergata
002655508 700__ $$aVandelli, Wainer$$iINSPIRE-00306351$$jORCID:0000-0001-6581-9410$$uCERN
002655508 700__ $$aVaniachine, Alexandre$$iINSPIRE-00133440$$uTomsk State U.
002655508 700__ $$aVankov, Peter$$iINSPIRE-00225024$$jORCID:0000-0002-7110-1728$$uFOM, Amsterdam
002655508 700__ $$aVari, Riccardo$$iINSPIRE-00225039$$jORCID:0000-0002-2814-1337$$uINFN, Rome
002655508 700__ $$aVarnes, Erich$$iINSPIRE-00133542$$jORCID:0000-0001-7820-9144$$uArizona U.
002655508 700__ $$aVarni, Carlo$$iINSPIRE-00534739$$jORCID:0000-0001-6733-4310$$uINFN, Genoa$$uGenoa U.
002655508 700__ $$aVarol, Tulin$$iINSPIRE-00287318$$jORCID:0000-0002-0697-5808$$uSouthern Methodist U.
002655508 700__ $$aVarouchas, Dimitris$$iINSPIRE-00225042$$jORCID:0000-0002-0734-4442$$uOrsay, LAL
002655508 700__ $$aVarvell, Kevin$$iINSPIRE-00225063$$jORCID:0000-0003-1017-1295$$uSydney U.
002655508 700__ $$aVasquez Arenas, Gerardo Alexis$$iINSPIRE-00529830$$jORCID:0000-0002-3285-7004$$uSanta Maria U., Valparaiso
002655508 700__ $$aVasquez, Jared Gregory$$iINSPIRE-00265075$$jORCID:0000-0001-8946-0502$$uYale U.
002655508 700__ $$aVazeille, Francois$$iINSPIRE-00225072$$jORCID:0000-0003-1631-2714$$uClermont-Ferrand U.
002655508 700__ $$aVazquez Furelos, David$$iINSPIRE-00567197$$uBarcelona, IFAE
002655508 700__ $$aVazquez Schroeder, Tamara$$iINSPIRE-00237778$$jORCID:0000-0002-9780-099X$$uMcGill U.
002655508 700__ $$aVeatch, Jason$$iINSPIRE-00354304$$jORCID:0000-0003-0855-0958$$uGottingen U., II. Phys. Inst.
002655508 700__ $$aVecchio, Valentina$$iINSPIRE-00581467$$jORCID:0000-0002-1351-6757$$uINFN, Rome3$$uRome III U.
002655508 700__ $$aVeloce, Laurelle Maria$$iINSPIRE-00406224$$uToronto U.
002655508 700__ $$aVeloso, Filipe$$iINSPIRE-00034280$$jORCID:0000-0002-5956-4244$$uLIP, Lisbon$$uCoimbra U.
002655508 700__ $$aVeneziano, Stefano$$iINSPIRE-00225080$$jORCID:0000-0002-2598-2659$$uINFN, Rome
002655508 700__ $$aVentura, Andrea$$iINSPIRE-00058029$$jORCID:0000-0002-3368-3413$$uINFN, Lecce$$uSalento U.
002655508 700__ $$aVenturi, Manuela$$iINSPIRE-00225109$$uVictoria U.
002655508 700__ $$aVenturi, Nicola$$iINSPIRE-00225111$$uCERN
002655508 700__ $$aVercesi, Valerio$$iINSPIRE-00140154$$jORCID:0000-0001-7670-4563$$uINFN, Pavia
002655508 700__ $$aVerducci, Monica$$iINSPIRE-00225123$$jORCID:0000-0001-8209-4757$$uINFN, Rome3$$uRome III U.
002655508 700__ $$aVergel Infante, Carlos Miguel$$iINSPIRE-00507820$$uIowa State U.
002655508 700__ $$aVergis, Christos$$iINSPIRE-00649349$$jORCID:0000-0002-3228-6715$$uBonn U.
002655508 700__ $$aVerkerke, Wouter$$iINSPIRE-00029133$$uFOM, Amsterdam
002655508 700__ $$aVermeulen, Ambrosius Thomas$$iINSPIRE-00548968$$jORCID:0000-0002-8884-7112$$uFOM, Amsterdam
002655508 700__ $$aVermeulen, Jos$$iINSPIRE-00140176$$jORCID:0000-0003-4378-5736$$uFOM, Amsterdam
002655508 700__ $$aVetterli, Michel$$iINSPIRE-00133870$$jORCID:0000-0002-7223-2965$$uSimon Fraser U.$$uTRIUMF
002655508 700__ $$aViaux Maira, Nicolas$$iINSPIRE-00384010$$uSanta Maria U., Valparaiso
002655508 700__ $$aVicente Barreto Pinto, Mateus$$iINSPIRE-00714258$$jORCID:0000-0002-8000-4882$$uGeneva U.
002655508 700__ $$aVichou, Irene$$iINSPIRE-00161358$$uIllinois U., Urbana
002655508 700__ $$aVickey, Trevor$$iINSPIRE-00052371$$jORCID:0000-0002-1596-2611$$uSheffield U.
002655508 700__ $$aVickey Boeriu, Oana Elena$$iINSPIRE-00237790$$jORCID:0000-0002-6497-6809$$uSheffield U.
002655508 700__ $$aViehhauser, Georg$$iINSPIRE-00225132$$jORCID:0000-0002-0237-292X$$uOxford U.
002655508 700__ $$aViel, Simon$$iINSPIRE-00232885$$jORCID:0000-0001-9554-4059$$uLBL, Berkeley
002655508 700__ $$aVigani, Luigi$$iINSPIRE-00427277$$jORCID:0000-0002-6270-9176$$uOxford U.
002655508 700__ $$aVilla, Mauro$$iINSPIRE-00225145$$jORCID:0000-0002-9181-8048$$uINFN, Bologna$$uBologna U.
002655508 700__ $$aVillaplana Perez, Miguel$$iINSPIRE-00225163$$jORCID:0000-0002-0048-4602$$uINFN, Milan$$uMilan U.
002655508 700__ $$aVilucchi, Elisabetta$$iINSPIRE-00225177$$jORCID:0000-0002-4839-6281$$uFrascati
002655508 700__ $$aVincter, Manuella$$iINSPIRE-00133971$$jORCID:0000-0002-5338-8972$$uCarleton U.
002655508 700__ $$aVinogradov, Vladimir$$iINSPIRE-00227012$$uDubna, JINR
002655508 700__ $$aVishwakarma, Akanksha$$iINSPIRE-00529840$$jORCID:0000-0001-8832-0313$$uDESY
002655508 700__ $$aVittori, Camilla$$iINSPIRE-00453010$$jORCID:0000-0001-9156-970X$$uINFN, Bologna$$uBologna U.
002655508 700__ $$aVivarelli, Iacopo$$iINSPIRE-00016420$$jORCID:0000-0003-0097-123X$$uSussex U.
002655508 700__ $$aVlachos, Sotirios$$iINSPIRE-00134107$$jORCID:0000-0002-1879-3745$$uNatl. Tech. U., Athens
002655508 700__ $$aVogel, Marcelo$$iINSPIRE-00009675$$uWuppertal U.
002655508 700__ $$aVokac, Petr$$iINSPIRE-00007099$$jORCID:0000-0002-3429-4778$$uPrague, Tech. U.
002655508 700__ $$aVolpi, Guido$$iINSPIRE-00040623$$jORCID:0000-0003-1058-8883$$uBarcelona, IFAE
002655508 700__ $$aVon Buddenbrock, Stefan Erich$$iINSPIRE-00540611$$jORCID:0000-0002-8399-9993$$uWitwatersrand U.
002655508 700__ $$aVon Toerne, Eckhard$$iINSPIRE-00058359$$uBonn U.
002655508 700__ $$aVorobel, Vit$$iINSPIRE-00188264$$jORCID:0000-0001-8757-2180$$uCharles U.
002655508 700__ $$aVorobev, Konstantin$$iINSPIRE-00364793$$uMoscow Phys. Eng. Inst.
002655508 700__ $$aVos, Marcel$$iINSPIRE-00240580$$jORCID:0000-0001-8474-5357$$uValencia U., IFIC
002655508 700__ $$aVossebeld, Joost$$iINSPIRE-00134340$$jORCID:0000-0001-8178-8503$$uLiverpool U.
002655508 700__ $$aVranjes, Nenad$$iINSPIRE-00225275$$jORCID:0000-0001-5415-5225$$uBelgrade U.
002655508 700__ $$aVranjes Milosavljevic, Marija$$iINSPIRE-00225280$$jORCID:0000-0003-4477-9733$$uBelgrade U.
002655508 700__ $$aVrba, Vaclav$$iINSPIRE-00134373$$uPrague, Tech. U.
002655508 700__ $$aVreeswijk, Marcel$$iINSPIRE-00225293$$uFOM, Amsterdam
002655508 700__ $$aSfiligoj, Tina$$iINSPIRE-00371537$$uStefan Inst., Ljubljana
002655508 700__ $$aVuillermet, Raphael$$iINSPIRE-00225322$$uCERN
002655508 700__ $$aVukotic, Ilija$$iINSPIRE-00225336$$jORCID:0000-0003-0472-3516$$uChicago U., EFI
002655508 700__ $$aZenis, Tibor$$iINSPIRE-00306374$$jORCID:0000-0001-8265-6916$$uComenius U.
002655508 700__ $$aZivkovic, Lidija$$iINSPIRE-00057284$$jORCID:0000-0003-4236-8930$$uBelgrade U.
002655508 700__ $$aWagner, Peter$$iINSPIRE-00052760$$jORCID:0000-0001-7481-2480$$uBonn U.
002655508 700__ $$aWagner, Wolfgang$$iINSPIRE-00051400$$jORCID:0000-0002-9198-5911$$uWuppertal U.
002655508 700__ $$aWagner-kuhr, Jeannine$$iINSPIRE-00003851$$jORCID:0000-0001-6306-1888$$uMunich U.
002655508 700__ $$aWahlberg, Hernan$$iINSPIRE-00153915$$jORCID:0000-0003-0616-7330$$uLa Plata U.
002655508 700__ $$aWahrmund, Sebastian$$iINSPIRE-00233070$$uDresden, Tech. U.
002655508 700__ $$aWakamiya, Kotaro$$iINSPIRE-00571628$$uKobe U.
002655508 700__ $$aWalbrecht, Verena Maria$$iINSPIRE-00584613$$uMunich, Max Planck Inst.
002655508 700__ $$aWalder, James$$iINSPIRE-00007572$$jORCID:0000-0002-9039-8758$$uLancaster U.
002655508 700__ $$aWalker, Rodney$$iINSPIRE-00225350$$jORCID:0000-0001-8535-4809$$uMunich U.
002655508 700__ $$aWalker, Stuart Derek$$iINSPIRE-00568865$$uRoyal Holloway, U. of London
002655508 700__ $$aWalkowiak, Wolfgang$$iINSPIRE-00134689$$jORCID:0000-0002-0385-3784$$uSiegen U.
002655508 700__ $$aWallangen, Veronica$$iINSPIRE-00441545$$uStockholm U.$$uStockholm U., OKC
002655508 700__ $$aWang, Ann Miao$$iINSPIRE-00573671$$jORCID:0000-0001-8972-3026$$uHarvard U., Phys. Dept.
002655508 700__ $$aWang, Chao$$iINSPIRE-00439918$$uShandong U.$$uMarseille, CPPM
002655508 700__ $$aWang, Fuquan$$iINSPIRE-00357049$$uWisconsin U., Madison
002655508 700__ $$aWang, Haichen$$iINSPIRE-00225389$$jORCID:0000-0003-3952-8139$$uLBL, Berkeley
002655508 700__ $$aWang, Hulin$$iINSPIRE-00237831$$jORCID:0000-0002-3609-5625$$uAlberta U.
002655508 700__ $$aWang, Jin$$iINSPIRE-00225390$$jORCID:0000-0002-4963-0877$$uSydney U.
002655508 700__ $$aWang, Jike$$iINSPIRE-00287547$$jORCID:0000-0001-6711-4465$$uHeidelberg U.
002655508 700__ $$aWang, Peilong$$iINSPIRE-00584049$$jORCID:0000-0002-6730-1524$$uSouthern Methodist U.
002655508 700__ $$aWang, Qing$$iINSPIRE-00507962$$uOklahoma U.
002655508 700__ $$aWang, Renjie$$iINSPIRE-00339675$$jORCID:0000-0002-5059-8456$$uParis U., VI-VII
002655508 700__ $$aWang, Rongkun$$iINSPIRE-00578185$$jORCID:0000-0001-9839-608X$$uHefei, CUST
002655508 700__ $$aWang, Rui$$iINSPIRE-00237848$$jORCID:0000-0001-8530-6487$$uArgonne
002655508 700__ $$aWang, Song-Ming$$iINSPIRE-00134900$$jORCID:0000-0002-5821-4875$$uTaiwan, Inst. Phys.
002655508 700__ $$aWang, Weitao$$iINSPIRE-00581470$$uHefei, CUST
002655508 700__ $$aWang, Wei$$iINSPIRE-00533069$$uNanjing U.$$uTaiwan, Inst. Phys.
002655508 700__ $$aWang, Wenxiao$$iINSPIRE-00449272$$jORCID:0000-0002-1444-6260$$uHefei, CUST$$uTaiwan, Inst. Phys.
002655508 700__ $$aWang, Yufeng$$iINSPIRE-00576923$$jORCID:0000-0003-2693-3442$$uHefei, CUST$$uParis U., VI-VII
002655508 700__ $$aWang, Zirui$$iINSPIRE-00537852$$jORCID:0000-0002-0928-2070$$uShanghai Jiao Tong U.
002655508 700__ $$aWanotayaroj, Chaowaroj$$iINSPIRE-00366124$$jORCID:0000-0002-8178-5705$$uDESY
002655508 700__ $$aWarburton, Andreas$$iINSPIRE-00134957$$jORCID:0000-0002-2298-7315$$uMcGill U.
002655508 700__ $$aWard, Patricia$$iINSPIRE-00034528$$jORCID:0000-0002-5162-533X$$uCambridge U.
002655508 700__ $$aWardrope, David Robert$$iINSPIRE-00305495$$jORCID:0000-0002-8208-2964$$uUniversity Coll. London
002655508 700__ $$aWashbrook, Andrew$$iINSPIRE-00287555$$uEdinburgh U.
002655508 700__ $$aWatkins, Peter$$iINSPIRE-00225418$$jORCID:0000-0002-1290-6833$$uBirmingham U.
002655508 700__ $$aWatson, Alan$$iINSPIRE-00135097$$jORCID:0000-0001-7052-7973$$uBirmingham U.
002655508 700__ $$aWatson, Miriam$$iINSPIRE-00225428$$jORCID:0000-0002-9724-2684$$uBirmingham U.
002655508 700__ $$aWatts, Gordon$$iINSPIRE-00135120$$jORCID:0000-0002-0753-7308$$uWashington U., Seattle
002655508 700__ $$aWatts, Stephen$$iINSPIRE-00003412$$jORCID:0000-0003-2392-1710$$uManchester U.
002655508 700__ $$aWaugh, Ben$$iINSPIRE-00145415$$jORCID:0000-0003-0872-8920$$uUniversity Coll. London
002655508 700__ $$aWebb, Aaron Foley$$iINSPIRE-00536691$$jORCID:0000-0002-6700-7608$$uTexas U.
002655508 700__ $$aWebb, Samuel$$iINSPIRE-00345617$$jORCID:0000-0003-4749-8814$$uMainz U.
002655508 700__ $$aWeber, Christian$$iINSPIRE-00579732$$uYale U.
002655508 700__ $$aWeber, Michele$$iINSPIRE-00135206$$jORCID:0000-0002-2770-9031$$uBern U., LHEP
002655508 700__ $$aWeber, Stephen Albert$$iINSPIRE-00529858$$jORCID:0000-0003-1710-4298$$uCarleton U.
002655508 700__ $$aWeber, Sebastian Mario$$iINSPIRE-00565709$$jORCID:0000-0002-2841-1616$$uKirchhoff Inst. Phys.
002655508 700__ $$aWeidberg, Anthony$$iINSPIRE-00148085$$jORCID:0000-0002-5158-307X$$uOxford U.
002655508 700__ $$aWeinert, Benjamin$$iINSPIRE-00359706$$uIndiana U.
002655508 700__ $$aWeingarten, Jens$$iINSPIRE-00225459$$jORCID:0000-0003-2165-871X$$uDortmund U.
002655508 700__ $$aWeirich, Marcel$$iINSPIRE-00547698$$jORCID:0000-0002-5129-872X$$uMainz U.
002655508 700__ $$aWeiser, Christian$$iINSPIRE-00225468$$jORCID:0000-0002-6456-6834$$uFreiburg U.
002655508 700__ $$aWells, Pippa$$iINSPIRE-00225479$$jORCID:0000-0003-4999-896X$$uCERN
002655508 700__ $$aWenaus, Torre$$iINSPIRE-00135450$$jORCID:0000-0002-8678-893X$$uBrookhaven
002655508 700__ $$aWengler, Thorsten$$iINSPIRE-00145320$$jORCID:0000-0002-4375-5265$$uCERN
002655508 700__ $$aWenig, Siegfried$$iINSPIRE-00145513$$jORCID:0000-0002-4770-377X$$uCERN
002655508 700__ $$aWermes, Norbert$$iINSPIRE-00135524$$jORCID:0000-0001-9971-0077$$uBonn U.
002655508 700__ $$aWerner, Michael David$$iINSPIRE-00433265$$jORCID:0000-0001-8091-749X$$uIowa State U.
002655508 700__ $$aWerner, Per$$iINSPIRE-00225665$$uCERN
002655508 700__ $$aWessels, Martin$$iINSPIRE-00217771$$jORCID:0000-0002-8192-8999$$uKirchhoff Inst. Phys.
002655508 700__ $$aWeston, Thomas Daniel$$iINSPIRE-00567203$$uBern U., LHEP
002655508 700__ $$aWhalen, Kathleen$$iINSPIRE-00225692$$jORCID:0000-0002-9383-8763$$uOregon U.
002655508 700__ $$aWhallon, Nikola Lazar$$iINSPIRE-00444316$$uWashington U., Seattle
002655508 700__ $$aWharton, Andrew Mark$$iINSPIRE-00390886$$uLancaster U.
002655508 700__ $$aWhite, Aaron$$iINSPIRE-00547705$$jORCID:0000-0003-0714-1466$$uMichigan U.
002655508 700__ $$aWhite, Andrew$$iINSPIRE-00013505$$uTexas U., Arlington
002655508 700__ $$aWhite, Martin$$iINSPIRE-00162417$$jORCID:0000-0001-5474-4580$$uAdelaide U., Sch. Chem. Phys.
002655508 700__ $$aWhite, Ryan$$iINSPIRE-00003676$$jORCID:0000-0003-3589-5900$$uSanta Maria U., Valparaiso
002655508 700__ $$aWhiteson, Daniel$$iINSPIRE-00054720$$jORCID:0000-0002-2005-3113$$uUC, Irvine
002655508 700__ $$aWhitmore, Ben William$$iINSPIRE-00565710$$jORCID:0000-0001-9130-6731$$uLancaster U.
002655508 700__ $$aWickens, Fred$$iINSPIRE-00135820$$jORCID:0000-0003-4937-6319$$uRutherford
002655508 700__ $$aWiedenmann, Werner$$iINSPIRE-00225736$$jORCID:0000-0003-3605-3633$$uWisconsin U., Madison
002655508 700__ $$aWielers, Monika$$iINSPIRE-00225743$$jORCID:0000-0001-9232-4827$$uRutherford
002655508 700__ $$aWiglesworth, Craig$$iINSPIRE-00225769$$jORCID:0000-0001-6219-8946$$uBohr Inst.
002655508 700__ $$aWiik, Liv Antje Mari$$iINSPIRE-00225778$$uFreiburg U.
002655508 700__ $$aWildauer, Andreas$$iINSPIRE-00225788$$uMunich, Max Planck Inst.
002655508 700__ $$aWilk, Fabian$$iINSPIRE-00401313$$uManchester U.
002655508 700__ $$aWilkens, Henric George$$iINSPIRE-00225806$$jORCID:0000-0002-8483-9502$$uCERN
002655508 700__ $$aWilkins, Lewis Joseph$$iINSPIRE-00639277$$jORCID:0000-0002-7092-3500$$uRoyal Holloway, U. of London
002655508 700__ $$aWilliams, Hugh$$iINSPIRE-00136066$$uPennsylvania U.
002655508 700__ $$aWilliams, Sarah$$iINSPIRE-00287350$$uCambridge U.
002655508 700__ $$aWillis, Christopher$$iINSPIRE-00358369$$uMichigan State U.
002655508 700__ $$aWillocq, Stephane$$iINSPIRE-00136116$$jORCID:0000-0002-4120-1453$$uMassachusetts U., Amherst
002655508 700__ $$aWilson, John$$iINSPIRE-00154108$$uBirmingham U.
002655508 700__ $$aWingerter-Seez, Isabelle$$iINSPIRE-00136245$$jORCID:0000-0001-9473-7836$$uAnnecy, LAPP
002655508 700__ $$aWinkels, Emma$$iINSPIRE-00542448$$jORCID:0000-0003-0156-3801$$uSussex U.
002655508 700__ $$aWinklmeier, Frank$$iINSPIRE-00042764$$jORCID:0000-0001-8290-3200$$uOregon U.
002655508 700__ $$aWinston, Oliver James$$iINSPIRE-00443634$$jORCID:0000-0001-6318-9873$$uSussex U.
002655508 700__ $$aWinter, Benedict Tobias$$iINSPIRE-00371046$$jORCID:0000-0001-9606-7688$$uBonn U.
002655508 700__ $$aWittgen, Matthias$$iINSPIRE-00041794$$uSLAC
002655508 700__ $$aWobisch, Markus$$iINSPIRE-00136413$$jORCID:0000-0002-0688-3380$$uLouisiana Tech. U.
002655508 700__ $$aWolf, Anton$$iINSPIRE-00549153$$jORCID:0000-0002-4368-9202$$uMainz U.
002655508 700__ $$aWolf, Tim Michael Heinz$$iINSPIRE-00439983$$jORCID:0000-0002-4561-0166$$uFOM, Amsterdam
002655508 700__ $$aWolff, Robert$$iINSPIRE-00533076$$jORCID:0000-0002-3758-6194$$uMarseille, CPPM
002655508 700__ $$aWolter, Marcin Wladyslaw$$iINSPIRE-00136528$$jORCID:0000-0001-9184-2921$$uCracow, INP
002655508 700__ $$aWolters, Helmut$$iINSPIRE-00225832$$jORCID:0000-0002-9588-1773$$uLIP, Lisbon$$uCoimbra U.
002655508 700__ $$aWong, Vincent Wai Sum$$iINSPIRE-00508714$$uBritish Columbia U.
002655508 700__ $$aWoods, Natasha Lee$$iINSPIRE-00567409$$jORCID:0000-0002-8993-3063$$uUC, Santa Cruz
002655508 700__ $$aWorm, Steven$$iINSPIRE-00145331$$jORCID:0000-0002-3865-4996$$uBirmingham U.
002655508 700__ $$aWosiek, Barbara$$iINSPIRE-00256470$$jORCID:0000-0003-4273-6334$$uCracow, INP
002655508 700__ $$aWozniak, Krzysztof$$iINSPIRE-00256486$$jORCID:0000-0003-1171-0887$$uCracow, INP
002655508 700__ $$aWraight, Kenneth$$iINSPIRE-00160280$$jORCID:0000-0002-3298-4900$$uGlasgow U.
002655508 700__ $$aWu, Miles$$iINSPIRE-00390966$$uChicago U., EFI
002655508 700__ $$aWu, Sau Lan$$iINSPIRE-00136809$$jORCID:0000-0001-5866-1504$$uWisconsin U., Madison
002655508 700__ $$aWu, Xin$$iINSPIRE-00306899$$jORCID:0000-0001-7655-389X$$uGeneva U.
002655508 700__ $$aWu, Yusheng$$iINSPIRE-00237882$$jORCID:0000-0002-1528-4865$$uHefei, CUST
002655508 700__ $$aWyatt, Terry Richard$$iINSPIRE-00136898$$jORCID:0000-0001-9690-2997$$uManchester U.
002655508 700__ $$aWynne, Benjamin$$iINSPIRE-00225867$$jORCID:0000-0001-9895-4475$$uEdinburgh U.
002655508 700__ $$aXella, Stefania$$iINSPIRE-00027688$$jORCID:0000-0002-0988-1655$$uBohr Inst.
002655508 700__ $$aXi, Zhaoxu$$iINSPIRE-00508949$$uMichigan U.
002655508 700__ $$aXia, Ligang$$iINSPIRE-00446504$$jORCID:0000-0003-3073-3662$$uWarwick U.
002655508 700__ $$aXu, Da$$iINSPIRE-00225894$$jORCID:0000-0001-6355-2767$$uBeijing, Inst. High Energy Phys.
002655508 700__ $$aXu, Hanlin$$iINSPIRE-00571630$$uHefei, CUST$$uMarseille, CPPM
002655508 700__ $$aXu, Lailin$$iINSPIRE-00329742$$jORCID:0000-0001-8997-3199$$uBrookhaven
002655508 700__ $$aXu, Tairan$$iINSPIRE-00465240$$jORCID:0000-0002-0215-6151$$uIRFU, Saclay
002655508 700__ $$aXu, Wenhao$$iINSPIRE-00568886$$jORCID:0000-0001-5661-1917$$uMichigan U.
002655508 700__ $$aYabsley, Bruce$$iINSPIRE-00137014$$jORCID:0000-0002-2680-0474$$uSydney U.
002655508 700__ $$aYacoob, Sahal$$iINSPIRE-00038563$$jORCID:0000-0001-6977-3456$$uCape Town U.
002655508 700__ $$aYajima, Kazuki$$iINSPIRE-00571948$$uOsaka U.
002655508 700__ $$aYallup, David Paul$$iINSPIRE-00549852$$uUniversity Coll. London
002655508 700__ $$aYamaguchi, Daiki$$iINSPIRE-00413207$$uTokyo Inst. Tech.
002655508 700__ $$aYamaguchi, Yohei$$iINSPIRE-00336655$$jORCID:0000-0002-3725-4800$$uTokyo Inst. Tech.
002655508 700__ $$aYamamoto, Akira$$iINSPIRE-00225925$$jORCID:0000-0002-5351-5169$$uKEK, Tsukuba
002655508 700__ $$aYamanaka, Takashi$$iINSPIRE-00237916$$uTokyo U., ICEPP
002655508 700__ $$aYamane, Fumiya$$iINSPIRE-00563555$$uKobe U.
002655508 700__ $$aYamatani, Masahiro$$iINSPIRE-00549868$$uTokyo U., ICEPP
002655508 700__ $$aYamazaki, Tomohiro$$iINSPIRE-00563560$$jORCID:0000-0003-0411-3590$$uTokyo U., ICEPP
002655508 700__ $$aYamazaki, Yuji$$iINSPIRE-00173319$$jORCID:0000-0003-3710-6995$$uKobe U.
002655508 700__ $$aYan, Zhen$$iINSPIRE-00225940$$jORCID:0000-0002-2483-4937$$uBoston U.
002655508 700__ $$aYang, Haijun$$iINSPIRE-00059882$$jORCID:0000-0001-7367-1380$$uShanghai Jiao Tong U.$$uTsung-Dao Lee Inst., Shanghai
002655508 700__ $$aYang, Hongtao$$iINSPIRE-00336678$$jORCID:0000-0003-3554-7113$$uLBL, Berkeley
002655508 700__ $$aYang, Siqi$$iINSPIRE-00187470$$jORCID:0000-0002-0204-984X$$uIowa U.
002655508 700__ $$aYang, Yi-lin$$iINSPIRE-00576497$$jORCID:0000-0001-8524-1855$$uTokyo U., ICEPP
002655508 700__ $$aYang, Zongchang$$iINSPIRE-00313020$$uBergen U.
002655508 700__ $$aYao, Weiming$$iINSPIRE-00137324$$jORCID:0000-0002-3335-1988$$uLBL, Berkeley
002655508 700__ $$aYap, Yee Chinn$$iINSPIRE-00441752$$jORCID:0000-0001-8939-666X$$uDESY
002655508 700__ $$aYasu, Yoshiji$$iINSPIRE-00225960$$jORCID:0000-0002-9829-2384$$uKEK, Tsukuba
002655508 700__ $$aYatsenko, Elena$$iINSPIRE-00333129$$jORCID:0000-0003-3499-3090$$uShanghai Jiao Tong U.$$uTsung-Dao Lee Inst., Shanghai
002655508 700__ $$aYe, Jingbo$$iINSPIRE-00226177$$jORCID:0000-0001-9274-707X$$uSouthern Methodist U.
002655508 700__ $$aYe, Shuwei$$iINSPIRE-00139045$$jORCID:0000-0002-7864-4282$$uBrookhaven
002655508 700__ $$aYeletskikh, Ivan$$iINSPIRE-00375274$$jORCID:0000-0003-0586-7052$$uDubna, JINR
002655508 700__ $$aYigitbasi, Efe$$iINSPIRE-00537286$$jORCID:0000-0002-9595-2623$$uBoston U.
002655508 700__ $$aYildirim, Eda$$iINSPIRE-00194534$$uMainz U.
002655508 700__ $$aYorita, Kohei$$iINSPIRE-00048979$$jORCID:0000-0003-1988-8401$$uWaseda U.
002655508 700__ $$aYoshihara, Keisuke$$iINSPIRE-00288002$$jORCID:0000-0002-3656-2326$$uPennsylvania U.
002655508 700__ $$aYoung, Christopher John$$iINSPIRE-00237930$$jORCID:0000-0001-5858-6639$$uCERN
002655508 700__ $$aYoung, Charles$$iINSPIRE-00137680$$uSLAC
002655508 700__ $$aYu, Jaehoon$$iINSPIRE-00137749$$uTexas U., Arlington
002655508 700__ $$aYu, Jie$$iINSPIRE-00226216$$jORCID:0000-0002-0398-8179$$uIowa State U.
002655508 700__ $$aYue, Xiaoguang$$iINSPIRE-00579744$$jORCID:0000-0001-6956-3205$$uKirchhoff Inst. Phys.
002655508 700__ $$aYuen, Stephanie Pui Yan$$iINSPIRE-00418328$$uBonn U.
002655508 700__ $$aZabinski, Bartlomiej$$iINSPIRE-00237959$$jORCID:0000-0001-5626-0993$$uCracow, INP
002655508 700__ $$aZacharis, George$$iINSPIRE-00529860$$jORCID:0000-0002-3156-4453$$uNatl. Tech. U., Athens
002655508 700__ $$aZaffaroni, Ettore$$iINSPIRE-00714087$$jORCID:0000-0003-1714-9218$$uGeneva U.
002655508 700__ $$aZaidan, Remi$$iINSPIRE-00226234$$jORCID:0000-0002-3710-4554$$uBarcelona, IFAE
002655508 700__ $$aZaitsev, Alexander$$iINSPIRE-00170475$$jORCID:0000-0002-4961-8368$$uSerpukhov, IHEP$$uMoscow, MIPT
002655508 700__ $$aZakareishvili, Tamar$$iINSPIRE-00641188$$uTbilisi State U.
002655508 700__ $$aZakharchuk, Nataliia$$iINSPIRE-00443845$$jORCID:0000-0002-4963-8836$$uDESY
002655508 700__ $$aZalieckas, Justas$$iINSPIRE-00379716$$uBergen U.
002655508 700__ $$aZambito, Stefano$$iINSPIRE-00337110$$jORCID:0000-0002-4499-2545$$uHarvard U., Phys. Dept.
002655508 700__ $$aZanzi, Daniele$$iINSPIRE-00288010$$jORCID:0000-0002-1222-7937$$uCERN
002655508 700__ $$aZaripovas, Donatas Ramilas$$iINSPIRE-00583063$$jORCID:0000-0001-6056-7947$$uGlasgow U.
002655508 700__ $$aZeissner, Sonja Verena$$iINSPIRE-00584533$$jORCID:0000-0002-9037-2152$$uDortmund U.
002655508 700__ $$aZeitnitz, Christian$$iINSPIRE-00138192$$jORCID:0000-0003-2280-8636$$uWuppertal U.
002655508 700__ $$aZemaityte, Gabija$$iINSPIRE-00547711$$uOxford U.
002655508 700__ $$aZeng, Jian Cong$$iINSPIRE-00439941$$uIllinois U., Urbana
002655508 700__ $$aZeng, Qi$$iINSPIRE-00387563$$uSLAC
002655508 700__ $$aZenin, Oleg$$iINSPIRE-00226303$$jORCID:0000-0002-5447-1989$$uSerpukhov, IHEP
002655508 700__ $$aZerwas, Dirk$$iINSPIRE-00140536$$jORCID:0000-0002-4198-3029$$uOrsay, LAL
002655508 700__ $$aZgubic, Miha$$iINSPIRE-00584050$$jORCID:0000-0002-5110-5959$$uOxford U.
002655508 700__ $$aZhang, Dengfeng$$iINSPIRE-00465365$$jORCID:0000-0001-7335-4983$$uShandong U.
002655508 700__ $$aZhang, Dongliang$$iINSPIRE-00237976$$uMichigan U.
002655508 700__ $$aZhang, Fangzhou$$iINSPIRE-00357056$$jORCID:0000-0003-0749-2960$$uWisconsin U., Madison
002655508 700__ $$aZhang, Guangyi$$iINSPIRE-00423270$$jORCID:0000-0002-6431-8638$$uHefei, CUST
002655508 700__ $$aZhang, Huijun$$iINSPIRE-00408038$$uNanjing U.
002655508 700__ $$aZhang, Jinlong$$iINSPIRE-00226349$$jORCID:0000-0002-9907-838X$$uArgonne
002655508 700__ $$aZhang, Lei$$iINSPIRE-00333000$$uNanjing U.
002655508 700__ $$aZhang, Liqing$$iINSPIRE-00529872$$jORCID:0000-0001-5241-6559$$uHefei, CUST
002655508 700__ $$aZhang, Matt$$iINSPIRE-00529881$$jORCID:0000-0001-8659-5727$$uIllinois U., Urbana
002655508 700__ $$aZhang, Peng$$iINSPIRE-00544989$$uNanjing U.
002655508 700__ $$aZhang, Ruiqi$$iINSPIRE-00381776$$uHefei, CUST
002655508 700__ $$aZhang, Rui$$iINSPIRE-00440984$$jORCID:0000-0002-8265-474X$$uBonn U.
002655508 700__ $$aZhang, Xueyao$$iINSPIRE-00226365$$jORCID:0000-0003-4341-1603$$uShandong U.
002655508 700__ $$aZhang, Yu$$iINSPIRE-00455492$$jORCID:0000-0002-4554-2554$$uBeijing, GUCAS
002655508 700__ $$aZhang, Zhiqing$$iINSPIRE-00138347$$jORCID:0000-0002-7853-9079$$uOrsay, LAL
002655508 700__ $$aZhao, Pingchuan$$iINSPIRE-00585846$$uDuke U.
002655508 700__ $$aZhao, Xiandong$$iINSPIRE-00379595$$uSouthern Methodist U.
002655508 700__ $$aZhao, Yongke$$iINSPIRE-00382184$$uShandong U.$$uOrsay, LAL
002655508 700__ $$aZhao, Zhengguo$$iINSPIRE-00226382$$uHefei, CUST
002655508 700__ $$aZhemchugov, Alexey$$iINSPIRE-00226395$$jORCID:0000-0002-3360-4965$$uDubna, JINR
002655508 700__ $$aZhou, Bing$$iINSPIRE-00138410$$uMichigan U.
002655508 700__ $$aZhou, Chen$$iINSPIRE-00264959$$uWisconsin U., Madison
002655508 700__ $$aZhou, Li$$iINSPIRE-00379761$$uSouthern Methodist U.
002655508 700__ $$aZhou, Maosen$$iINSPIRE-00455505$$jORCID:0000-0002-8554-9216$$uBeijing, GUCAS
002655508 700__ $$aZhou, Mingliang$$iINSPIRE-00414784$$jORCID:0000-0001-7223-8403$$uSUNY, Stony Brook
002655508 700__ $$aZhou, Ning$$iINSPIRE-00301363$$jORCID:0000-0002-1775-2511$$uShanghai Jiao Tong U.
002655508 700__ $$aZhou, You$$iINSPIRE-00515588$$uArizona U.
002655508 700__ $$aZhu, Cheng Guang$$iINSPIRE-00226420$$jORCID:0000-0001-8015-3901$$uShandong U.
002655508 700__ $$aZhu, Heling$$iINSPIRE-00581489$$uHefei, CUST
002655508 700__ $$aZhu, Hongbo$$iINSPIRE-00226430$$jORCID:0000-0001-8066-7048$$uBeijing, Inst. High Energy Phys.
002655508 700__ $$aZhu, Junjie$$iINSPIRE-00053364$$jORCID:0000-0002-5278-2855$$uMichigan U.
002655508 700__ $$aZhu, Yingchun$$iINSPIRE-00218063$$jORCID:0000-0002-7306-1053$$uHefei, CUST
002655508 700__ $$aZhuang, Xuai$$iINSPIRE-00226448$$jORCID:0000-0003-0996-3279$$uBeijing, Inst. High Energy Phys.
002655508 700__ $$aZhukov, Konstantin$$iINSPIRE-00372098$$uLebedev Inst.
002655508 700__ $$aZhulanov, Vladimir$$iINSPIRE-00366015$$uNovosibirsk State U.$$uNovosibirsk, IYF
002655508 700__ $$aZibell, Andre$$iINSPIRE-00295941$$uWurzburg U.
002655508 700__ $$aZieminska, Daria$$iINSPIRE-00138550$$jORCID:0000-0002-6311-7420$$uIndiana U.
002655508 700__ $$aZimine, Nikolai$$iINSPIRE-00342797$$jORCID:0000-0003-0277-4870$$uDubna, JINR
002655508 700__ $$aZimmermann, Stephanie$$iINSPIRE-00226472$$jORCID:0000-0002-1529-8925$$uFreiburg U.
002655508 700__ $$aZinonos, Zinonas$$iINSPIRE-00226313$$uMunich, Max Planck Inst.
002655508 700__ $$aZinser, Markus$$iINSPIRE-00388590$$uMainz U.
002655508 700__ $$aZiolkowski, Michael$$iINSPIRE-00154081$$uSiegen U.
002655508 700__ $$aZobernig, Georg$$iINSPIRE-00226497$$jORCID:0000-0001-8113-1499$$uWisconsin U., Madison
002655508 700__ $$aZoccoli, Antonio$$iINSPIRE-00138667$$jORCID:0000-0002-0993-6185$$uINFN, Bologna$$uBologna U.
002655508 700__ $$aZoch, Knut$$iINSPIRE-00583073$$jORCID:0000-0003-2138-6187$$uGottingen U., II. Phys. Inst.
002655508 700__ $$aZorbas, Theodoros Georgio$$iINSPIRE-00576502$$jORCID:0000-0003-2073-4901$$uSheffield U.
002655508 700__ $$aZou, Rui$$iINSPIRE-00535690$$jORCID:0000-0002-0542-1264$$uChicago U., EFI
002655508 700__ $$azur Nedden, Martin$$iINSPIRE-00226500$$uHumboldt U., Berlin
002655508 700__ $$aZwalinski, Lukasz$$iINSPIRE-00233300$$uCERN
002655508 710__ $$gATLAS Collaboration
002655508 710__ $$5PH-EP
002655508 773__ $$c733$$n9$$pEur. Phys. J. C$$v79$$y2019
002655508 859__ [email protected]
002655508 8564_ $$uhttps://rivet.hepforge.org/analyses/ATLAS_2019_I1718132$$yRivet analyses reference
002655508 8564_ $$81460976$$s2067817$$uhttp://cds.cern.ch/record/2655508/files/EXOT-2016-08-PAPER.pdf$$yFulltext
002655508 8564_ $$81460976$$s2938933$$uhttp://cds.cern.ch/record/2655508/files/EXOT-2016-08-PAPER.pdf?subformat=pdfa$$xpdfa
002655508 8564_ $$81461366$$s36564$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_minDeltaPhiJ1_L_isZCReejj___ST.png$$y00006 The measured generator-level differential cross-sections in the \eejj channel, where an additional selection of $\st > 600~\GeV$ has been applied, exclusively for the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461367$$s40859$$uhttp://cds.cern.ch/record/2655508/files/mumujj_jet1_pt_20181220.png$$y00005  : Caption not extracted
002655508 8564_ $$81461368$$s36446$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_DeltaEtaJJ_isZCReejj___ST.png$$y00072 The measured generator-level differential cross-sections in the \eejj channel, where an additional selection of $\st > 600~\GeV$ has been applied, exclusively for the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461369$$s31581$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_DiJetMass_isZCReejj___ST.png$$y00061 The measured generator-level differential cross-sections in the \eejj channel, where an additional selection of $\st > 600~\GeV$ has been applied, exclusively for the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461370$$s35858$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_DeltaPhiJJ_isZCReejj___ST.png$$y00095 The measured generator-level differential cross-sections in the \eejj channel, where an additional selection of $\st > 600~\GeV$ has been applied, exclusively for the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461371$$s32649$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_DiLepPt_isZCReejj__.png$$y00089 The measured generator-level differential cross-sections in the \eejj channel, exclusively for the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons.
002655508 8564_ $$81461372$$s40302$$uhttp://cds.cern.ch/record/2655508/files/enujj_met_met_20181220.png$$y00027  :
002655508 8564_ $$81461373$$s31881$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_DiJetMass_isZCRmmjj___ST.png$$y00051 The measured generator-level differential cross-sections in the \mumujj channel, where an additional selection of $\st > 600~\GeV$ has been applied. The measurements are made exclusively for the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461374$$s59647$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_St_isCRemjj___ST.png$$y00077 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass, where an additional selection of $\st > 600~\GeV$ has been applied. The measurements are made exclusively for the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461375$$s39856$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_JetPt_leading_isCRemjj___ST.png$$y00080 Examples of the measured particle-level differential cross-sections in the extreme \eejj, \mumujj and \emujj measurement regions, exclusively for the dominant process in each channel (\Zee, \Zmm and \ttbar{}, respectively). The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty on the measurement which is indicated by the error bar on each point. For the leading jet \pt\ measurement, the uncertainty in the second bin is smaller because the bin-by-bin correction factor from the alternative \ttbar{} samples agrees more closely with the nominal ones than in neighbouring bins. The variable $ min \Delta \Phi (j0,l) $ refers to the minimal difference in $\phi$ between the leading jet and a prompt lepton.
002655508 8564_ $$81461376$$s38983$$uhttp://cds.cern.ch/record/2655508/files/unreweighted_mumujj_m_jj_20181220.png$$y00014  :
002655508 8564_ $$81461377$$s46635$$uhttp://cds.cern.ch/record/2655508/files/munujj_m_LQ_T_20181220.png$$y00073 : Caption not extracted
002655508 8564_ $$81461378$$s34370$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_DiJetMass_isCRemjj__.png$$y00049 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass. The measurements are made exclusively for the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461379$$s35660$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_DeltaEtaJJ_isCRemjj__.png$$y00028 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass. The measurements are made exclusively for the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461380$$s39554$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_Ht_isZCRmmjj___ST.png$$y00058 The measured generator-level differential cross-sections in the \mumujj channel, where an additional selection of $\st > 600~\GeV$ has been applied. The measurements are made exclusively for the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461381$$s37786$$uhttp://cds.cern.ch/record/2655508/files/SRpaperisE.png$$y00104  :
002655508 8564_ $$81461382$$s33994$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_DeltaEtaJJ_isZCRmmjj__.png$$y00043 The measured generator-level differential cross-sections in the \mumujj channel, exclusively for the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461383$$s40472$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_minDeltaPhiJ0_L_isZCRmmjj___ST.png$$y00012 Examples of the measured particle-level differential cross-sections in the extreme \eejj, \mumujj and \emujj measurement regions, exclusively for the dominant process in each channel (\Zee, \Zmm and \ttbar{}, respectively). The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty on the measurement which is indicated by the error bar on each point. For the leading jet \pt\ measurement, the uncertainty in the second bin is smaller because the bin-by-bin correction factor from the alternative \ttbar{} samples agrees more closely with the nominal ones than in neighbouring bins. The variable $ min \Delta \Phi (j0,l) $ refers to the minimal difference in $\phi$ between the leading jet and a prompt lepton.
002655508 8564_ $$81461384$$s31490$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_DiJetMass_isZCRmmjj__.png$$y00078 The measured generator-level differential cross-sections in the \mumujj channel, exclusively for the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461385$$s36624$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_JetPt_leading_isZCRmmjj___ST.png$$y00068 Examples of the measured particle-level differential cross-sections in the extreme \eejj, \mumujj and \emujj measurement regions, exclusively for the dominant process in each channel (\Zee, \Zmm and \ttbar{}, respectively). The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty on the measurement which is indicated by the error bar on each point. For the leading jet \pt\ measurement, the uncertainty in the second bin is smaller because the bin-by-bin correction factor from the alternative \ttbar{} samples agrees more closely with the nominal ones than in neighbouring bins. The variable $ min \Delta \Phi (j0,l) $ refers to the minimal difference in $\phi$ between the leading jet and a prompt lepton.
002655508 8564_ $$81461386$$s36831$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_minDeltaPhiJ0_L_isCRemjj__.png$$y00037 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass. The measurements are made exclusively for the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461387$$s33639$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_DeltaEtaJJ_isZCReejj__.png$$y00100 The measured generator-level differential cross-sections in the \eejj channel, exclusively for the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons.
002655508 8564_ $$81461388$$s43378$$uhttp://cds.cern.ch/record/2655508/files/mumujj_m_LQ_min_20181220.png$$y00098  : Caption not extracted
002655508 8564_ $$81461389$$s39282$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_Ht_isCRemjj___ST.png$$y00081 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass, where an additional selection of $\st > 600~\GeV$ has been applied. The measurements are made exclusively for the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461390$$s34186$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_DeltaPhiJJ_isZCRmmjj__.png$$y00046 The measured generator-level differential cross-sections in the \mumujj channel, exclusively for the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461391$$s38570$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_Ht_isZCReejj__.png$$y00097 The measured generator-level differential cross-sections in the \eejj channel, exclusively for the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons.
002655508 8564_ $$81461392$$s40072$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_JetPt_subleading_isCRemjj___ST.png$$y00036 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass, where an additional selection of $\st > 600~\GeV$ has been applied. The measurements are made exclusively for the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461393$$s31337$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_DiJetMass_isZCReejj__.png$$y00035 The measured generator-level differential cross-sections in the \eejj channel, exclusively for the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons.
002655508 8564_ $$81461394$$s37306$$uhttp://cds.cern.ch/record/2655508/files/munujj_m_jj_ttbar_20181220.png$$y00044  : Caption not extracted
002655508 8564_ $$81461395$$s48053$$uhttp://cds.cern.ch/record/2655508/files/munujj_mt_20181220.png$$y00066  : Caption not extracted
002655508 8564_ $$81461396$$s46232$$uhttp://cds.cern.ch/record/2655508/files/munujj_met_met_TR_20181220.png$$y00092  : Caption not extracted
002655508 8564_ $$81461397$$s36398$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_JetPt_leading_isZCRmmjj__.png$$y00079 Examples of the measured particle-level differential cross-sections in the \eejj, \mumujj and \emujj measurement regions, exclusively for the dominant process in each channel (\Zee, \Zmm and \ttbar{}, respectively). The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty on the measurement which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j0,l) $ refers to the minimal difference in $\phi$ between the leading jet and a prompt lepton.
002655508 8564_ $$81461398$$s34209$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_DiLepPt_isZCRmmjj___ST.png$$y00009 The measured generator-level differential cross-sections in the \mumujj channel, where an additional selection of $\st > 600~\GeV$ has been applied. The measurements are made exclusively for the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461399$$s8850$$uhttp://cds.cern.ch/record/2655508/files/contour_low_mass_isMu_20181220.png$$y00047  : Caption not extracted
002655508 8564_ $$81461400$$s42483$$uhttp://cds.cern.ch/record/2655508/files/munujj_BDT_LQ1300_20181220.png$$y00083  : Caption not extracted
002655508 8564_ $$81461401$$s39506$$uhttp://cds.cern.ch/record/2655508/files/SRpaperisMu.png$$y00010  : Caption not extracted
002655508 8564_ $$81461402$$s40528$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_Ht_isZCReejj___ST.png$$y00019 The measured generator-level differential cross-sections in the \eejj channel, where an additional selection of $\st > 600~\GeV$ has been applied, exclusively for the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461403$$s36889$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_DiLepPt_isCRemjj__.png$$y00004 Examples of the measured particle-level differential cross-sections in the \eejj, \mumujj and \emujj measurement regions, exclusively for the dominant process in each channel (\Zee, \Zmm and \ttbar{}, respectively). The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty on the measurement which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j0,l) $ refers to the minimal difference in $\phi$ between the leading jet and a prompt lepton.
002655508 8564_ $$81461404$$s38105$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_DeltaPhiLL_isZCReejj__.png$$y00102 The measured generator-level differential cross-sections in the \eejj channel, exclusively for the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons.
002655508 8564_ $$81461405$$s34693$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_minDeltaPhiJ1_L_isCRemjj___ST.png$$y00025 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass, where an additional selection of $\st > 600~\GeV$ has been applied. The measurements are made exclusively for the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461406$$s33263$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_DiLepPt_isZCReejj___ST.png$$y00018 The measured generator-level differential cross-sections in the \eejj channel, where an additional selection of $\st > 600~\GeV$ has been applied, exclusively for the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461407$$s43252$$uhttp://cds.cern.ch/record/2655508/files/enujj_mt_ttbar_20181220.png$$y00084  :
002655508 8564_ $$81461408$$s40647$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_DeltaEtaJJ_isCRemjj___ST.png$$y00042 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass, where an additional selection of $\st > 600~\GeV$ has been applied. The measurements are made exclusively for the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461409$$s16653$$uhttp://cds.cern.ch/record/2655508/files/XSUpperLimit_isE_20181105.png$$y00070 :
002655508 8564_ $$81461410$$s39346$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_JetPt_subleading_isCRemjj__.png$$y00039 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass. The measurements are made exclusively for the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461411$$s38218$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_JetPt_subleading_isZCReejj___ST.png$$y00052 The measured generator-level differential cross-sections in the \eejj channel, where an additional selection of $\st > 600~\GeV$ has been applied, exclusively for the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461412$$s33936$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_DiJetMass_isCRemjj___ST.png$$y00090 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass, where an additional selection of $\st > 600~\GeV$ has been applied. The measurements are made exclusively for the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461413$$s46403$$uhttp://cds.cern.ch/record/2655508/files/eejj_m_LQ_min_TR_20181220.png$$y00011  :
002655508 8564_ $$81461414$$s40242$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_St_isZCReejj___ST.png$$y00065 The measured generator-level differential cross-sections in the \eejj channel, where an additional selection of $\st > 600~\GeV$ has been applied, exclusively for the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461415$$s2400440$$uhttp://cds.cern.ch/record/2655508/files/1902.00377.pdf$$yFulltext
002655508 8564_ $$81461416$$s37753$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_minDeltaPhiJ0_L_isZCReejj__.png$$y00021 Examples of the measured particle-level differential cross-sections in the \eejj, \mumujj and \emujj measurement regions, exclusively for the dominant process in each channel (\Zee, \Zmm and \ttbar{}, respectively). The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty on the measurement which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j0,l) $ refers to the minimal difference in $\phi$ between the leading jet and a prompt lepton.
002655508 8564_ $$81461417$$s46803$$uhttp://cds.cern.ch/record/2655508/files/mumujj_m_LQ_min_TR_20181220.png$$y00063  : Caption not extracted
002655508 8564_ $$81461418$$s8840$$uhttp://cds.cern.ch/record/2655508/files/contour_low_mass_isE_20181220.png$$y00101 :
002655508 8564_ $$81461419$$s37479$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_JetPt_subleading_isZCRmmjj__.png$$y00013 The measured generator-level differential cross-sections in the \mumujj channel, exclusively for the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461420$$s44980$$uhttp://cds.cern.ch/record/2655508/files/enujj_met_met_TR_20181220.png$$y00056 :
002655508 8564_ $$81461421$$s40271$$uhttp://cds.cern.ch/record/2655508/files/mumujj_m_jj_20181220.png$$y00071  : Caption not extracted
002655508 8564_ $$81461422$$s49844$$uhttp://cds.cern.ch/record/2655508/files/enujj_BDT_LQ1300_20181220.png$$y00015  :
002655508 8564_ $$81461423$$s44169$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_DeltaPhiLL_isCRemjj___ST.png$$y00076 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass, where an additional selection of $\st > 600~\GeV$ has been applied. The measurements are made exclusively for the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461424$$s40815$$uhttp://cds.cern.ch/record/2655508/files/munujj_mt_ttbar_20181220.png$$y00020  : Caption not extracted
002655508 8564_ $$81461425$$s37359$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_DiLepPt_isCRemjj___ST.png$$y00085 Examples of the measured particle-level differential cross-sections in the extreme \eejj, \mumujj and \emujj measurement regions, exclusively for the dominant process in each channel (\Zee, \Zmm and \ttbar{}, respectively). The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty on the measurement which is indicated by the error bar on each point. For the leading jet \pt\ measurement, the uncertainty in the second bin is smaller because the bin-by-bin correction factor from the alternative \ttbar{} samples agrees more closely with the nominal ones than in neighbouring bins. The variable $ min \Delta \Phi (j0,l) $ refers to the minimal difference in $\phi$ between the leading jet and a prompt lepton.
002655508 8564_ $$81461426$$s40066$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_DeltaPhiLL_isCRemjj__.png$$y00016 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass. The measurements are made exclusively for the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461427$$s36426$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_DeltaPhiJJ_isCRemjj___ST.png$$y00033 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass, where an additional selection of $\st > 600~\GeV$ has been applied. The measurements are made exclusively for the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461428$$s32742$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_DiLepPt_isZCRmmjj__.png$$y00008 The measured generator-level differential cross-sections in the \mumujj channel, exclusively for the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461429$$s37192$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_DeltaEtaJJ_isZCRmmjj___ST.png$$y00075 The measured generator-level differential cross-sections in the \mumujj channel, where an additional selection of $\st > 600~\GeV$ has been applied. The measurements are made exclusively for the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461430$$s210917$$uhttp://cds.cern.ch/record/2655508/files/feynlqpair.png$$y00006 : Caption not extracted
002655508 8564_ $$81461431$$s34773$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_DeltaPhiJJ_isZCReejj__.png$$y00045 The measured generator-level differential cross-sections in the \eejj channel, exclusively for the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons.
002655508 8564_ $$81461432$$s60839$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_St_isCRemjj__.png$$y00022 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass. The measurements are made exclusively for the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461433$$s31864$$uhttp://cds.cern.ch/record/2655508/files/contour_high_mass_isMu_20181220.png$$y00034 : Caption not extracted
002655508 8564_ $$81461434$$s39741$$uhttp://cds.cern.ch/record/2655508/files/enujj_m_jj_ttbar_20181220.png$$y00040 :
002655508 8564_ $$81461435$$s37551$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_minDeltaPhiJ0_L_isZCReejj___ST.png$$y00032 Examples of the measured particle-level differential cross-sections in the extreme \eejj, \mumujj and \emujj measurement regions, exclusively for the dominant process in each channel (\Zee, \Zmm and \ttbar{}, respectively). The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty on the measurement which is indicated by the error bar on each point. For the leading jet \pt\ measurement, the uncertainty in the second bin is smaller because the bin-by-bin correction factor from the alternative \ttbar{} samples agrees more closely with the nominal ones than in neighbouring bins. The variable $ min \Delta \Phi (j0,l) $ refers to the minimal difference in $\phi$ between the leading jet and a prompt lepton.
002655508 8564_ $$81461436$$s48931$$uhttp://cds.cern.ch/record/2655508/files/enujj_m_LQ_T_20181220.png$$y00087 :
002655508 8564_ $$81461437$$s40904$$uhttp://cds.cern.ch/record/2655508/files/mumujj_mu2_pt_TR_20181220.png$$y00093 : Caption not extracted
002655508 8564_ $$81461438$$s37898$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_Ht_isZCRmmjj__.png$$y00064 The measured generator-level differential cross-sections in the \mumujj channel, exclusively for the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461439$$s38962$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_JetPt_subleading_isZCReejj__.png$$y00105 The measured generator-level differential cross-sections in the \eejj channel, exclusively for the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons.
002655508 8564_ $$81461440$$s36972$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_St_isZCRmmjj__.png$$y00017 The measured generator-level differential cross-sections in the \mumujj channel, exclusively for the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461441$$s45069$$uhttp://cds.cern.ch/record/2655508/files/eejj_m_LQ_min_20181220.png$$y00067  :
002655508 8564_ $$81461442$$s36883$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_JetPt_leading_isZCReejj__.png$$y00030 Examples of the measured particle-level differential cross-sections in the \eejj, \mumujj and \emujj measurement regions, exclusively for the dominant process in each channel (\Zee, \Zmm and \ttbar{}, respectively). The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty on the measurement which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j0,l) $ refers to the minimal difference in $\phi$ between the leading jet and a prompt lepton.
002655508 8564_ $$81461443$$s35874$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_DeltaPhiJJ_isCRemjj__.png$$y00069 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass. The measurements are made exclusively for the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461444$$s2101$$uhttp://cds.cern.ch/record/2655508/files/feynlqsingle.png$$y00094 :
002655508 8564_ $$81461445$$s10328$$uhttp://cds.cern.ch/record/2655508/files/XSUpperLimit_step_isE_20181220.png$$y00031  :
002655508 8564_ $$81461446$$s42582$$uhttp://cds.cern.ch/record/2655508/files/eejj_m_ll_20181220.png$$y00103  :
002655508 8564_ $$81461447$$s31133$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_minDeltaPhiJ1_L_isZCRmmjj__.png$$y00057 The measured generator-level differential cross-sections in the \mumujj channel, exclusively for the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461448$$s36916$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_minDeltaPhiJ0_L_isZCRmmjj__.png$$y00074 Examples of the measured particle-level differential cross-sections in the \eejj, \mumujj and \emujj measurement regions, exclusively for the dominant process in each channel (\Zee, \Zmm and \ttbar{}, respectively). The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty on the measurement which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j0,l) $ refers to the minimal difference in $\phi$ between the leading jet and a prompt lepton.
002655508 8564_ $$81461449$$s38396$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_Ht_isCRemjj__.png$$y00050 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass. The measurements are made exclusively for the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461450$$s47364$$uhttp://cds.cern.ch/record/2655508/files/enujj_mt_20181220.png$$y00054 :
002655508 8564_ $$81461451$$s31779$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_minDeltaPhiJ1_L_isZCReejj__.png$$y00091 The measured generator-level differential cross-sections in the \eejj channel, exclusively for the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons.
002655508 8564_ $$81461452$$s37773$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_St_isZCRmmjj___ST.png$$y00059 The measured generator-level differential cross-sections in the \mumujj channel, where an additional selection of $\st > 600~\GeV$ has been applied. The measurements are made exclusively for the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461453$$s32490$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_minDeltaPhiJ1_L_isCRemjj__.png$$y00053 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass. The measurements are made exclusively for the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461454$$s40437$$uhttp://cds.cern.ch/record/2655508/files/munujj_met_met_20181220.png$$y00024 : Caption not extracted
002655508 8564_ $$81461455$$s39029$$uhttp://cds.cern.ch/record/2655508/files/eejj_BDT_LQ1300_20181220.png$$y00002  :
002655508 8564_ $$81461456$$s35115$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_minDeltaPhiJ1_L_isZCRmmjj___ST.png$$y00055 The measured generator-level differential cross-sections in the \mumujj channel, where an additional selection of $\st > 600~\GeV$ has been applied. The measurements are made exclusively for the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461457$$s36815$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_JetPt_subleading_isZCRmmjj___ST.png$$y00060 The measured generator-level differential cross-sections in the \mumujj channel, where an additional selection of $\st > 600~\GeV$ has been applied. The measurements are made exclusively for the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461458$$s40272$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_DeltaPhiLL_isZCReejj___ST.png$$y00082 The measured generator-level differential cross-sections in the \eejj channel, where an additional selection of $\st > 600~\GeV$ has been applied, exclusively for the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461459$$s39427$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_JetPt_leading_isCRemjj__.png$$y00023 Examples of the measured particle-level differential cross-sections in the \eejj, \mumujj and \emujj measurement regions, exclusively for the dominant process in each channel (\Zee, \Zmm and \ttbar{}, respectively). The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty on the measurement which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j0,l) $ refers to the minimal difference in $\phi$ between the leading jet and a prompt lepton.
002655508 8564_ $$81461460$$s44378$$uhttp://cds.cern.ch/record/2655508/files/eejj_el2_pt_TR_20181220.png$$y00099 :
002655508 8564_ $$81461461$$s15798$$uhttp://cds.cern.ch/record/2655508/files/contour_high_mass_isE_20181220.png$$y00007  :
002655508 8564_ $$81461462$$s34775$$uhttp://cds.cern.ch/record/2655508/files/mumujj_BDT_LQ1300_20181220.png$$y00026 : Caption not extracted
002655508 8564_ $$81461463$$s10339$$uhttp://cds.cern.ch/record/2655508/files/XSUpperLimit_step_isMu_20181220.png$$y00088  : Caption not extracted
002655508 8564_ $$81461464$$s41383$$uhttp://cds.cern.ch/record/2655508/files/mumujj_m_ll_20181220.png$$y00041 : Caption not extracted
002655508 8564_ $$81461465$$s32987$$uhttp://cds.cern.ch/record/2655508/files/XSUpperLimit_isMu_20181105.png$$y00096 : Caption not extracted
002655508 8564_ $$81461466$$s41792$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_minDeltaPhiJ0_L_isCRemjj___ST.png$$y00000 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass, where an additional selection of $\st > 600~\GeV$ has been applied. The measurements are made exclusively for the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461467$$s37406$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_DeltaPhiLL_isZCRmmjj__.png$$y00062 The measured generator-level differential cross-sections in the \mumujj channel, exclusively for the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461468$$s43080$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_DeltaPhiLL_isZCRmmjj___ST.png$$y00003 The measured generator-level differential cross-sections in the \mumujj channel, where an additional selection of $\st > 600~\GeV$ has been applied. The measurements are made exclusively for the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461469$$s39978$$uhttp://cds.cern.ch/record/2655508/files/unreweighted_mumujj_jet1_pt_20181220.png$$y00001 :
002655508 8564_ $$81461470$$s36404$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_DeltaPhiJJ_isZCRmmjj___ST.png$$y00048 The measured generator-level differential cross-sections in the \mumujj channel, where an additional selection of $\st > 600~\GeV$ has been applied. The measurements are made exclusively for the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81461471$$s37232$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_JetPt_leading_isZCReejj___ST.png$$y00038 Examples of the measured particle-level differential cross-sections in the extreme \eejj, \mumujj and \emujj measurement regions, exclusively for the dominant process in each channel (\Zee, \Zmm and \ttbar{}, respectively). The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty on the measurement which is indicated by the error bar on each point. For the leading jet \pt\ measurement, the uncertainty in the second bin is smaller because the bin-by-bin correction factor from the alternative \ttbar{} samples agrees more closely with the nominal ones than in neighbouring bins. The variable $ min \Delta \Phi (j0,l) $ refers to the minimal difference in $\phi$ between the leading jet and a prompt lepton.
002655508 8564_ $$81515489$$s2639918$$uhttp://cds.cern.ch/record/2655508/files/scoap3-fulltext.pdf$$yArticle from SCOAP3
002655508 8564_ $$81515736$$s43252$$uhttp://cds.cern.ch/record/2655508/files/w69_enujj_mt_ttbar_20181220.png$$y00069  :
002655508 8564_ $$81515737$$s40437$$uhttp://cds.cern.ch/record/2655508/files/w102_munujj_met_met_20181220.png$$y00102  : Caption not extracted
002655508 8564_ $$81515738$$s42483$$uhttp://cds.cern.ch/record/2655508/files/w50_munujj_BDT_LQ1300_20181220.png$$y00050  : Caption not extracted
002655508 8564_ $$81515739$$s37289$$uhttp://cds.cern.ch/record/2655508/files/w45_unfolded_data_binW_Response_minDeltaPhiJ0_L_isZCRmmjj__.png$$y00045 Examples of the measured particle-level differential cross-sections in the \eejj, \mumujj and \emujj measurement regions. The data are unfolded bin-by-bin exclusively to the dominant process in each channel (\Zee, \Zmm and \ttbar{}, respectively). The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty on the measurement which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j0,l) $ refers to the minimal difference in $\phi$ between the leading jet and a prompt lepton.
002655508 8564_ $$81515740$$s39506$$uhttp://cds.cern.ch/record/2655508/files/w53_SRpaperisMu.png$$y00053  : Caption not extracted
002655508 8564_ $$81515741$$s40647$$uhttp://cds.cern.ch/record/2655508/files/w94_unfolded_data_binW_Response_DeltaEtaJJ_isCRemjj___ST.png$$y00094 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass, where an additional selection of $\st > 600~\GeV$ has been applied. The data are unfolded bin-by-bin exclusively to the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515742$$s31675$$uhttp://cds.cern.ch/record/2655508/files/w93_unfolded_data_binW_Response_DiJetMass_isZCReejj__.png$$y00093 The measured generator-level differential cross-sections in the \eejj channel. The data are unfolded bin-by-bin exclusively to the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons.
002655508 8564_ $$81515743$$s32490$$uhttp://cds.cern.ch/record/2655508/files/w35_unfolded_data_binW_Response_minDeltaPhiJ1_L_isCRemjj__.png$$y00035 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass. The data are unfolded bin-by-bin exclusively to the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515744$$s43409$$uhttp://cds.cern.ch/record/2655508/files/w37_unfolded_data_binW_Response_DeltaPhiLL_isZCRmmjj___ST.png$$y00037 The measured generator-level differential cross-sections in the \mumujj channel, where an additional selection of $\st > 600~\GeV$ has been applied. The data are unfolded bin-by-bin exclusively to the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515745$$s16653$$uhttp://cds.cern.ch/record/2655508/files/w31_XSUpperLimit_isE_20181105.png$$y00031 :
002655508 8564_ $$81515746$$s39856$$uhttp://cds.cern.ch/record/2655508/files/w73_unfolded_data_binW_Response_JetPt_leading_isCRemjj___ST.png$$y00073 Examples of the measured particle-level differential cross-sections in the extreme \eejj, \mumujj and \emujj measurement regions. The data are unfolded bin-by-bin exclusively to the dominant process in each channel (\Zee, \Zmm and \ttbar{}, respectively). The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty on the measurement which is indicated by the error bar on each point. For the leading jet \pt\ measurement, the uncertainty in the second bin is smaller because the bin-by-bin correction factor from the alternative \ttbar{} samples agrees more closely with the nominal ones than in neighbouring bins. The variable $ min \Delta \Phi (j0,l) $ refers to the minimal difference in $\phi$ between the leading jet and a prompt lepton.
002655508 8564_ $$81515747$$s41792$$uhttp://cds.cern.ch/record/2655508/files/w39_unfolded_data_binW_Response_minDeltaPhiJ0_L_isCRemjj___ST.png$$y00039 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass, where an additional selection of $\st > 600~\GeV$ has been applied. The data are unfolded bin-by-bin exclusively to the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515748$$s161496$$uhttp://cds.cern.ch/record/2655508/files/w68_feynlqsingle.png$$y00068 :
002655508 8564_ $$81515749$$s35874$$uhttp://cds.cern.ch/record/2655508/files/w18_unfolded_data_binW_Response_DeltaPhiJJ_isCRemjj__.png$$y00018 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass. The data are unfolded bin-by-bin exclusively to the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515750$$s39529$$uhttp://cds.cern.ch/record/2655508/files/w0_unfolded_data_binW_Response_Ht_isCRemjj___ST.png$$y00000 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass, where an additional selection of $\st > 600~\GeV$ has been applied. The data are unfolded bin-by-bin exclusively to the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515751$$s46232$$uhttp://cds.cern.ch/record/2655508/files/w22_munujj_met_met_TR_20181220.png$$y00022  : Caption not extracted
002655508 8564_ $$81515752$$s39741$$uhttp://cds.cern.ch/record/2655508/files/w60_enujj_m_jj_ttbar_20181220.png$$y00060  :
002655508 8564_ $$81515753$$s44980$$uhttp://cds.cern.ch/record/2655508/files/w80_enujj_met_met_TR_20181220.png$$y00080 :
002655508 8564_ $$81515754$$s40859$$uhttp://cds.cern.ch/record/2655508/files/w49_mumujj_jet1_pt_20181220.png$$y00049  : Caption not extracted
002655508 8564_ $$81515755$$s36737$$uhttp://cds.cern.ch/record/2655508/files/w89_unfolded_data_binW_Response_JetPt_leading_isZCRmmjj__.png$$y00089 Examples of the measured particle-level differential cross-sections in the \eejj, \mumujj and \emujj measurement regions. The data are unfolded bin-by-bin exclusively to the dominant process in each channel (\Zee, \Zmm and \ttbar{}, respectively). The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty on the measurement which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j0,l) $ refers to the minimal difference in $\phi$ between the leading jet and a prompt lepton.
002655508 8564_ $$81515756$$s8840$$uhttp://cds.cern.ch/record/2655508/files/w70_contour_low_mass_isE_20181220.png$$y00070  :
002655508 8564_ $$81515757$$s210917$$uhttp://cds.cern.ch/record/2655508/files/w3_feynlqpair.png$$y00003  : Caption not extracted
002655508 8564_ $$81515758$$s36408$$uhttp://cds.cern.ch/record/2655508/files/w104_unfolded_data_binW_Response_JetPt_subleading_isZCRmmjj___ST.png$$y00104 The measured generator-level differential cross-sections in the \mumujj channel, where an additional selection of $\st > 600~\GeV$ has been applied. The data are unfolded bin-by-bin exclusively to the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515759$$s34693$$uhttp://cds.cern.ch/record/2655508/files/w54_unfolded_data_binW_Response_minDeltaPhiJ1_L_isCRemjj___ST.png$$y00054 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass, where an additional selection of $\st > 600~\GeV$ has been applied. The data are unfolded bin-by-bin exclusively to the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515760$$s34370$$uhttp://cds.cern.ch/record/2655508/files/w38_unfolded_data_binW_Response_DiJetMass_isCRemjj__.png$$y00038 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass. The data are unfolded bin-by-bin exclusively to the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515761$$s33946$$uhttp://cds.cern.ch/record/2655508/files/w17_unfolded_data_binW_Response_DiLepPt_isZCRmmjj__.png$$y00017 The measured generator-level differential cross-sections in the \mumujj channel. The data are unfolded bin-by-bin exclusively to the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515762$$s39427$$uhttp://cds.cern.ch/record/2655508/files/w27_unfolded_data_binW_Response_JetPt_leading_isCRemjj__.png$$y00027 Examples of the measured particle-level differential cross-sections in the \eejj, \mumujj and \emujj measurement regions. The data are unfolded bin-by-bin exclusively to the dominant process in each channel (\Zee, \Zmm and \ttbar{}, respectively). The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty on the measurement which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j0,l) $ refers to the minimal difference in $\phi$ between the leading jet and a prompt lepton.
002655508 8564_ $$81515763$$s36426$$uhttp://cds.cern.ch/record/2655508/files/w61_unfolded_data_binW_Response_DeltaPhiJJ_isCRemjj___ST.png$$y00061 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass, where an additional selection of $\st > 600~\GeV$ has been applied. The data are unfolded bin-by-bin exclusively to the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515764$$s45069$$uhttp://cds.cern.ch/record/2655508/files/w74_eejj_m_LQ_min_20181220.png$$y00074  :
002655508 8564_ $$81515765$$s40527$$uhttp://cds.cern.ch/record/2655508/files/w82_unfolded_data_binW_Response_DeltaPhiLL_isZCReejj___ST.png$$y00082 The measured generator-level differential cross-sections in the \eejj channel, where an additional selection of $\st > 600~\GeV$ has been applied. The data are unfolded bin-by-bin exclusively to the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515766$$s46635$$uhttp://cds.cern.ch/record/2655508/files/w7_munujj_m_LQ_T_20181220.png$$y00007 : Caption not extracted
002655508 8564_ $$81515767$$s48931$$uhttp://cds.cern.ch/record/2655508/files/w83_enujj_m_LQ_T_20181220.png$$y00083 :
002655508 8564_ $$81515768$$s37873$$uhttp://cds.cern.ch/record/2655508/files/w12_unfolded_data_binW_Response_minDeltaPhiJ0_L_isZCReejj___ST.png$$y00012 Examples of the measured particle-level differential cross-sections in the extreme \eejj, \mumujj and \emujj measurement regions. The data are unfolded bin-by-bin exclusively to the dominant process in each channel (\Zee, \Zmm and \ttbar{}, respectively). The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty on the measurement which is indicated by the error bar on each point. For the leading jet \pt\ measurement, the uncertainty in the second bin is smaller because the bin-by-bin correction factor from the alternative \ttbar{} samples agrees more closely with the nominal ones than in neighbouring bins. The variable $ min \Delta \Phi (j0,l) $ refers to the minimal difference in $\phi$ between the leading jet and a prompt lepton.
002655508 8564_ $$81515769$$s35561$$uhttp://cds.cern.ch/record/2655508/files/w62_unfolded_data_binW_Response_minDeltaPhiJ1_L_isZCRmmjj___ST.png$$y00062 The measured generator-level differential cross-sections in the \mumujj channel, where an additional selection of $\st > 600~\GeV$ has been applied. The data are unfolded bin-by-bin exclusively to the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515770$$s38922$$uhttp://cds.cern.ch/record/2655508/files/w1_unfolded_data_binW_Response_JetPt_subleading_isZCRmmjj__.png$$y00001 The measured generator-level differential cross-sections in the \mumujj channel. The data are unfolded bin-by-bin exclusively to the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515771$$s40943$$uhttp://cds.cern.ch/record/2655508/files/w72_unfolded_data_binW_Response_Ht_isZCReejj___ST.png$$y00072 The measured generator-level differential cross-sections in the \eejj channel, where an additional selection of $\st > 600~\GeV$ has been applied. The data are unfolded bin-by-bin exclusively to the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515772$$s39029$$uhttp://cds.cern.ch/record/2655508/files/w36_eejj_BDT_LQ1300_20181220.png$$y00036 :
002655508 8564_ $$81515773$$s39978$$uhttp://cds.cern.ch/record/2655508/files/w32_unreweighted_mumujj_jet1_pt_20181220.png$$y00032  :
002655508 8564_ $$81515774$$s33654$$uhttp://cds.cern.ch/record/2655508/files/w56_unfolded_data_binW_Response_DiLepPt_isZCReejj___ST.png$$y00056 The measured generator-level differential cross-sections in the \eejj channel, where an additional selection of $\st > 600~\GeV$ has been applied. The data are unfolded bin-by-bin exclusively to the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515775$$s37550$$uhttp://cds.cern.ch/record/2655508/files/w101_unfolded_data_binW_Response_DeltaEtaJJ_isZCRmmjj___ST.png$$y00101 The measured generator-level differential cross-sections in the \mumujj channel, where an additional selection of $\st > 600~\GeV$ has been applied. The data are unfolded bin-by-bin exclusively to the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515776$$s32987$$uhttp://cds.cern.ch/record/2655508/files/w75_XSUpperLimit_isMu_20181105.png$$y00075  : Caption not extracted
002655508 8564_ $$81515777$$s39838$$uhttp://cds.cern.ch/record/2655508/files/w78_unfolded_data_binW_Response_JetPt_subleading_isZCReejj__.png$$y00078 The measured generator-level differential cross-sections in the \eejj channel. The data are unfolded bin-by-bin exclusively to the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons.
002655508 8564_ $$81515778$$s39052$$uhttp://cds.cern.ch/record/2655508/files/w99_unfolded_data_binW_Response_Ht_isZCRmmjj__.png$$y00099 The measured generator-level differential cross-sections in the \mumujj channel. The data are unfolded bin-by-bin exclusively to the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515779$$s46403$$uhttp://cds.cern.ch/record/2655508/files/w59_eejj_m_LQ_min_TR_20181220.png$$y00059  :
002655508 8564_ $$81515780$$s48053$$uhttp://cds.cern.ch/record/2655508/files/w40_munujj_mt_20181220.png$$y00040  : Caption not extracted
002655508 8564_ $$81515781$$s32181$$uhttp://cds.cern.ch/record/2655508/files/w52_unfolded_data_binW_Response_DiJetMass_isZCRmmjj__.png$$y00052 The measured generator-level differential cross-sections in the \mumujj channel. The data are unfolded bin-by-bin exclusively to the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515782$$s32215$$uhttp://cds.cern.ch/record/2655508/files/w16_unfolded_data_binW_Response_DiJetMass_isZCRmmjj___ST.png$$y00016 The measured generator-level differential cross-sections in the \mumujj channel, where an additional selection of $\st > 600~\GeV$ has been applied. The data are unfolded bin-by-bin exclusively to the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515783$$s34007$$uhttp://cds.cern.ch/record/2655508/files/w25_unfolded_data_binW_Response_DeltaEtaJJ_isZCReejj__.png$$y00025 The measured generator-level differential cross-sections in the \eejj channel. The data are unfolded bin-by-bin exclusively to the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons.
002655508 8564_ $$81515784$$s49844$$uhttp://cds.cern.ch/record/2655508/files/w92_enujj_BDT_LQ1300_20181220.png$$y00092 :
002655508 8564_ $$81515785$$s38983$$uhttp://cds.cern.ch/record/2655508/files/w41_unreweighted_mumujj_m_jj_20181220.png$$y00041  :
002655508 8564_ $$81515786$$s40066$$uhttp://cds.cern.ch/record/2655508/files/w43_unfolded_data_binW_Response_DeltaPhiLL_isCRemjj__.png$$y00043 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass. The data are unfolded bin-by-bin exclusively to the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515787$$s34574$$uhttp://cds.cern.ch/record/2655508/files/w10_unfolded_data_binW_Response_DiLepPt_isZCRmmjj___ST.png$$y00010 The measured generator-level differential cross-sections in the \mumujj channel, where an additional selection of $\st > 600~\GeV$ has been applied. The data are unfolded bin-by-bin exclusively to the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515788$$s36889$$uhttp://cds.cern.ch/record/2655508/files/w4_unfolded_data_binW_Response_DiLepPt_isCRemjj__.png$$y00004 Examples of the measured particle-level differential cross-sections in the \eejj, \mumujj and \emujj measurement regions. The data are unfolded bin-by-bin exclusively to the dominant process in each channel (\Zee, \Zmm and \ttbar{}, respectively). The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty on the measurement which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j0,l) $ refers to the minimal difference in $\phi$ between the leading jet and a prompt lepton.
002655508 8564_ $$81515789$$s33660$$uhttp://cds.cern.ch/record/2655508/files/w84_unfolded_data_binW_Response_DiLepPt_isZCReejj__.png$$y00084 The measured generator-level differential cross-sections in the \eejj channel. The data are unfolded bin-by-bin exclusively to the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons.
002655508 8564_ $$81515790$$s32128$$uhttp://cds.cern.ch/record/2655508/files/w63_unfolded_data_binW_Response_minDeltaPhiJ1_L_isZCReejj__.png$$y00063 The measured generator-level differential cross-sections in the \eejj channel. The data are unfolded bin-by-bin exclusively to the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons.
002655508 8564_ $$81515791$$s43378$$uhttp://cds.cern.ch/record/2655508/files/w86_mumujj_m_LQ_min_20181220.png$$y00086 : Caption not extracted
002655508 8564_ $$81515792$$s40302$$uhttp://cds.cern.ch/record/2655508/files/w34_enujj_met_met_20181220.png$$y00034  :
002655508 8564_ $$81515793$$s40815$$uhttp://cds.cern.ch/record/2655508/files/w64_munujj_mt_ttbar_20181220.png$$y00064  : Caption not extracted
002655508 8564_ $$81515794$$s46803$$uhttp://cds.cern.ch/record/2655508/files/w85_mumujj_m_LQ_min_TR_20181220.png$$y00085  : Caption not extracted
002655508 8564_ $$81515795$$s40047$$uhttp://cds.cern.ch/record/2655508/files/w42_unfolded_data_binW_Response_JetPt_subleading_isZCReejj___ST.png$$y00042 The measured generator-level differential cross-sections in the \eejj channel, where an additional selection of $\st > 600~\GeV$ has been applied. The data are unfolded bin-by-bin exclusively to the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515796$$s34494$$uhttp://cds.cern.ch/record/2655508/files/w47_unfolded_data_binW_Response_DeltaPhiJJ_isZCRmmjj__.png$$y00047 The measured generator-level differential cross-sections in the \mumujj channel. The data are unfolded bin-by-bin exclusively to the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515797$$s31951$$uhttp://cds.cern.ch/record/2655508/files/w19_unfolded_data_binW_Response_DiJetMass_isZCReejj___ST.png$$y00019 The measured generator-level differential cross-sections in the \eejj channel, where an additional selection of $\st > 600~\GeV$ has been applied. The data are unfolded bin-by-bin exclusively to the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515798$$s33936$$uhttp://cds.cern.ch/record/2655508/files/w48_unfolded_data_binW_Response_DiJetMass_isCRemjj___ST.png$$y00048 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass, where an additional selection of $\st > 600~\GeV$ has been applied. The data are unfolded bin-by-bin exclusively to the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515799$$s31864$$uhttp://cds.cern.ch/record/2655508/files/w46_contour_high_mass_isMu_20181220.png$$y00046 : Caption not extracted
002655508 8564_ $$81515800$$s34775$$uhttp://cds.cern.ch/record/2655508/files/w11_mumujj_BDT_LQ1300_20181220.png$$y00011 : Caption not extracted
002655508 8564_ $$81515801$$s15798$$uhttp://cds.cern.ch/record/2655508/files/w88_contour_high_mass_isE_20181220.png$$y00088 :
002655508 8564_ $$81515802$$s40561$$uhttp://cds.cern.ch/record/2655508/files/w13_unfolded_data_binW_Response_St_isZCReejj___ST.png$$y00013 The measured generator-level differential cross-sections in the \eejj channel, where an additional selection of $\st > 600~\GeV$ has been applied. The data are unfolded bin-by-bin exclusively to the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515803$$s38286$$uhttp://cds.cern.ch/record/2655508/files/w77_unfolded_data_binW_Response_St_isZCRmmjj__.png$$y00077 The measured generator-level differential cross-sections in the \mumujj channel. The data are unfolded bin-by-bin exclusively to the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515804$$s40904$$uhttp://cds.cern.ch/record/2655508/files/w15_mumujj_mu2_pt_TR_20181220.png$$y00015 : Caption not extracted
002655508 8564_ $$81515805$$s10328$$uhttp://cds.cern.ch/record/2655508/files/w21_XSUpperLimit_step_isE_20181220.png$$y00021 :
002655508 8564_ $$81515806$$s31468$$uhttp://cds.cern.ch/record/2655508/files/w28_unfolded_data_binW_Response_minDeltaPhiJ1_L_isZCRmmjj__.png$$y00028 The measured generator-level differential cross-sections in the \mumujj channel. The data are unfolded bin-by-bin exclusively to the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515807$$s37634$$uhttp://cds.cern.ch/record/2655508/files/w6_unfolded_data_binW_Response_JetPt_leading_isZCReejj___ST.png$$y00006 Examples of the measured particle-level differential cross-sections in the extreme \eejj, \mumujj and \emujj measurement regions. The data are unfolded bin-by-bin exclusively to the dominant process in each channel (\Zee, \Zmm and \ttbar{}, respectively). The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty on the measurement which is indicated by the error bar on each point. For the leading jet \pt\ measurement, the uncertainty in the second bin is smaller because the bin-by-bin correction factor from the alternative \ttbar{} samples agrees more closely with the nominal ones than in neighbouring bins. The variable $ min \Delta \Phi (j0,l) $ refers to the minimal difference in $\phi$ between the leading jet and a prompt lepton.
002655508 8564_ $$81515808$$s10339$$uhttp://cds.cern.ch/record/2655508/files/w30_XSUpperLimit_step_isMu_20181220.png$$y00030 : Caption not extracted
002655508 8564_ $$81515809$$s35125$$uhttp://cds.cern.ch/record/2655508/files/w23_unfolded_data_binW_Response_DeltaPhiJJ_isZCReejj__.png$$y00023 The measured generator-level differential cross-sections in the \eejj channel. The data are unfolded bin-by-bin exclusively to the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons.
002655508 8564_ $$81515810$$s38140$$uhttp://cds.cern.ch/record/2655508/files/w24_unfolded_data_binW_Response_St_isZCRmmjj___ST.png$$y00024 The measured generator-level differential cross-sections in the \mumujj channel, where an additional selection of $\st > 600~\GeV$ has been applied. The data are unfolded bin-by-bin exclusively to the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515811$$s38891$$uhttp://cds.cern.ch/record/2655508/files/w57_unfolded_data_binW_Response_Ht_isCRemjj__.png$$y00057 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass. The data are unfolded bin-by-bin exclusively to the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515812$$s37716$$uhttp://cds.cern.ch/record/2655508/files/w8_unfolded_data_binW_Response_DeltaPhiLL_isZCRmmjj__.png$$y00008 The measured generator-level differential cross-sections in the \mumujj channel. The data are unfolded bin-by-bin exclusively to the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515813$$s34335$$uhttp://cds.cern.ch/record/2655508/files/w58_unfolded_data_binW_Response_DeltaEtaJJ_isZCRmmjj__.png$$y00058 The measured generator-level differential cross-sections in the \mumujj channel. The data are unfolded bin-by-bin exclusively to the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515814$$s42582$$uhttp://cds.cern.ch/record/2655508/files/w5_eejj_m_ll_20181220.png$$y00005 :
002655508 8564_ $$81515815$$s39105$$uhttp://cds.cern.ch/record/2655508/files/w87_unfolded_data_binW_Response_JetPt_subleading_isCRemjj__.png$$y00087 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass. The data are unfolded bin-by-bin exclusively to the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515816$$s37260$$uhttp://cds.cern.ch/record/2655508/files/w26_unfolded_data_binW_Response_JetPt_leading_isZCReejj__.png$$y00026 Examples of the measured particle-level differential cross-sections in the \eejj, \mumujj and \emujj measurement regions. The data are unfolded bin-by-bin exclusively to the dominant process in each channel (\Zee, \Zmm and \ttbar{}, respectively). The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty on the measurement which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j0,l) $ refers to the minimal difference in $\phi$ between the leading jet and a prompt lepton.
002655508 8564_ $$81515817$$s36765$$uhttp://cds.cern.ch/record/2655508/files/w44_unfolded_data_binW_Response_DeltaPhiJJ_isZCRmmjj___ST.png$$y00044 The measured generator-level differential cross-sections in the \mumujj channel, where an additional selection of $\st > 600~\GeV$ has been applied. The data are unfolded bin-by-bin exclusively to the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515818$$s36841$$uhttp://cds.cern.ch/record/2655508/files/w96_unfolded_data_binW_Response_DeltaEtaJJ_isZCReejj___ST.png$$y00096 The measured generator-level differential cross-sections in the \eejj channel, where an additional selection of $\st > 600~\GeV$ has been applied. The data are unfolded bin-by-bin exclusively to the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515819$$s35660$$uhttp://cds.cern.ch/record/2655508/files/w2_unfolded_data_binW_Response_DeltaEtaJJ_isCRemjj__.png$$y00002 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass. The data are unfolded bin-by-bin exclusively to the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515820$$s40225$$uhttp://cds.cern.ch/record/2655508/files/w71_unfolded_data_binW_Response_Ht_isZCReejj__.png$$y00071 The measured generator-level differential cross-sections in the \eejj channel. The data are unfolded bin-by-bin exclusively to the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons.
002655508 8564_ $$81515821$$s51301$$uhttp://cds.cern.ch/record/2655508/files/w76_unfolded_data_binW_Response_St_isCRemjj___ST.png$$y00076 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass, where an additional selection of $\st > 600~\GeV$ has been applied. The data are unfolded bin-by-bin exclusively to the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515822$$s44378$$uhttp://cds.cern.ch/record/2655508/files/w79_eejj_el2_pt_TR_20181220.png$$y00079 :
002655508 8564_ $$81515823$$s41383$$uhttp://cds.cern.ch/record/2655508/files/w66_mumujj_m_ll_20181220.png$$y00066 : Caption not extracted
002655508 8564_ $$81515824$$s37359$$uhttp://cds.cern.ch/record/2655508/files/w97_unfolded_data_binW_Response_DiLepPt_isCRemjj___ST.png$$y00097 Examples of the measured particle-level differential cross-sections in the extreme \eejj, \mumujj and \emujj measurement regions. The data are unfolded bin-by-bin exclusively to the dominant process in each channel (\Zee, \Zmm and \ttbar{}, respectively). The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty on the measurement which is indicated by the error bar on each point. For the leading jet \pt\ measurement, the uncertainty in the second bin is smaller because the bin-by-bin correction factor from the alternative \ttbar{} samples agrees more closely with the nominal ones than in neighbouring bins. The variable $ min \Delta \Phi (j0,l) $ refers to the minimal difference in $\phi$ between the leading jet and a prompt lepton.
002655508 8564_ $$81515825$$s38091$$uhttp://cds.cern.ch/record/2655508/files/w103_unfolded_data_binW_Response_minDeltaPhiJ0_L_isZCReejj__.png$$y00103 Examples of the measured particle-level differential cross-sections in the \eejj, \mumujj and \emujj measurement regions. The data are unfolded bin-by-bin exclusively to the dominant process in each channel (\Zee, \Zmm and \ttbar{}, respectively). The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty on the measurement which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j0,l) $ refers to the minimal difference in $\phi$ between the leading jet and a prompt lepton.
002655508 8564_ $$81515826$$s40084$$uhttp://cds.cern.ch/record/2655508/files/w51_unfolded_data_binW_Response_JetPt_subleading_isCRemjj___ST.png$$y00051 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass, where an additional selection of $\st > 600~\GeV$ has been applied. The data are unfolded bin-by-bin exclusively to the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515827$$s36981$$uhttp://cds.cern.ch/record/2655508/files/w81_unfolded_data_binW_Response_JetPt_leading_isZCRmmjj___ST.png$$y00081 Examples of the measured particle-level differential cross-sections in the extreme \eejj, \mumujj and \emujj measurement regions. The data are unfolded bin-by-bin exclusively to the dominant process in each channel (\Zee, \Zmm and \ttbar{}, respectively). The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty on the measurement which is indicated by the error bar on each point. For the leading jet \pt\ measurement, the uncertainty in the second bin is smaller because the bin-by-bin correction factor from the alternative \ttbar{} samples agrees more closely with the nominal ones than in neighbouring bins. The variable $ min \Delta \Phi (j0,l) $ refers to the minimal difference in $\phi$ between the leading jet and a prompt lepton.
002655508 8564_ $$81515828$$s37786$$uhttp://cds.cern.ch/record/2655508/files/w33_SRpaperisE.png$$y00033 :
002655508 8564_ $$81515829$$s40271$$uhttp://cds.cern.ch/record/2655508/files/w95_mumujj_m_jj_20181220.png$$y00095 : Caption not extracted
002655508 8564_ $$81515830$$s37306$$uhttp://cds.cern.ch/record/2655508/files/w67_munujj_m_jj_ttbar_20181220.png$$y00067 : Caption not extracted
002655508 8564_ $$81515831$$s47364$$uhttp://cds.cern.ch/record/2655508/files/w98_enujj_mt_20181220.png$$y00098 :
002655508 8564_ $$81515832$$s36831$$uhttp://cds.cern.ch/record/2655508/files/w55_unfolded_data_binW_Response_minDeltaPhiJ0_L_isCRemjj__.png$$y00055 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass. The data are unfolded bin-by-bin exclusively to the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515833$$s40813$$uhttp://cds.cern.ch/record/2655508/files/w20_unfolded_data_binW_Response_minDeltaPhiJ0_L_isZCRmmjj___ST.png$$y00020 Examples of the measured particle-level differential cross-sections in the extreme \eejj, \mumujj and \emujj measurement regions. The data are unfolded bin-by-bin exclusively to the dominant process in each channel (\Zee, \Zmm and \ttbar{}, respectively). The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty on the measurement which is indicated by the error bar on each point. For the leading jet \pt\ measurement, the uncertainty in the second bin is smaller because the bin-by-bin correction factor from the alternative \ttbar{} samples agrees more closely with the nominal ones than in neighbouring bins. The variable $ min \Delta \Phi (j0,l) $ refers to the minimal difference in $\phi$ between the leading jet and a prompt lepton.
002655508 8564_ $$81515834$$s39871$$uhttp://cds.cern.ch/record/2655508/files/w91_unfolded_data_binW_Response_Ht_isZCRmmjj___ST.png$$y00091 The measured generator-level differential cross-sections in the \mumujj channel, where an additional selection of $\st > 600~\GeV$ has been applied. The data are unfolded bin-by-bin exclusively to the \Zmm process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515835$$s44169$$uhttp://cds.cern.ch/record/2655508/files/w65_unfolded_data_binW_Response_DeltaPhiLL_isCRemjj___ST.png$$y00065 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass, where an additional selection of $\st > 600~\GeV$ has been applied. The data are unfolded bin-by-bin exclusively to the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515836$$s8850$$uhttp://cds.cern.ch/record/2655508/files/w90_contour_low_mass_isMu_20181220.png$$y00090 : Caption not extracted
002655508 8564_ $$81515837$$s38378$$uhttp://cds.cern.ch/record/2655508/files/w29_unfolded_data_binW_Response_DeltaPhiLL_isZCReejj__.png$$y00029 The measured generator-level differential cross-sections in the \eejj channel. The data are unfolded bin-by-bin exclusively to the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons.
002655508 8564_ $$81515838$$s36201$$uhttp://cds.cern.ch/record/2655508/files/w9_unfolded_data_binW_Response_DeltaPhiJJ_isZCReejj___ST.png$$y00009 The measured generator-level differential cross-sections in the \eejj channel, where an additional selection of $\st > 600~\GeV$ has been applied. The data are unfolded bin-by-bin exclusively to the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515839$$s50963$$uhttp://cds.cern.ch/record/2655508/files/w14_unfolded_data_binW_Response_St_isCRemjj__.png$$y00014 The measured generator-level differential cross-sections in the \emujj channel, defined as for the \eejj and \mumujj MRs, but requiring the two leptons to have different flavours, and with no requirement on the dilepton mass. The data are unfolded bin-by-bin exclusively to the \ttbar~process. The MC prediction for the dominant process is also shown. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variables $ min \Delta \Phi (j0,l) $ and $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between a prompt lepton and the leading or subleading jet respectively. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81515840$$s36985$$uhttp://cds.cern.ch/record/2655508/files/w100_unfolded_data_binW_Response_minDeltaPhiJ1_L_isZCReejj___ST.png$$y00100 The measured generator-level differential cross-sections in the \eejj channel, where an additional selection of $\st > 600~\GeV$ has been applied. The data are unfolded bin-by-bin exclusively to the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons. The variable $S_{T}$ refers to the scalar sum of the \pt of the jets and leptons.
002655508 8564_ $$81518441$$s2976$$uhttp://cds.cern.ch/record/2655508/files/LQ_FeynFigure_pair.png$$y00029  : Caption not extracted
002655508 8564_ $$81518442$$s38988$$uhttp://cds.cern.ch/record/2655508/files/unfolded_data_binW_Response_St_isZCReejj__.png$$y00086 The measured generator-level differential cross-sections in the \eejj channel, exclusively for the \Zee process. The MC prediction for the dominant process is also shown, with no $m_{jj}$ reweighting applied. The red band represents the statistical component of the total uncertainty which is indicated by the error bar on each point. The variable $ min \Delta \Phi (j1,l) $ refers to the minimal difference in $\phi$ between the subleading jet and a prompt lepton. The variable $H_{T}$ refers to the scalar sum of the jet \pt values. The variables $\Delta \eta(jj)$, $\Delta \phi(jj)$ and $\Delta \phi(ll)$ refer to the difference in $\eta$ and $\phi$ between the two leading jets or leptons.
002655508 8564_ $$82336358$$s2639918$$uhttp://cds.cern.ch/record/2655508/files/scoap.pdf$$yArticle from SCOAP3
002655508 916__ $$sn$$w201904
002655508 925__ $$b15 Feb 2019
002655508 960__ $$a13
002655508 980__ $$aATLAS_Papers
002655508 980__ $$aARTICLE