CERN Accelerating science

002255384 001__ 2255384
002255384 005__ 20240504043032.0
002255384 0248_ $$aoai:cds.cern.ch:2255384$$pcerncds:CERN$$pcerncds:CERN:FULLTEXT$$pcerncds:FULLTEXT
002255384 0247_ $$2DOI$$9bibmatch$$a10.1140/epjc/s10052-017-5007-2
002255384 037__ $$9arXiv$$aarXiv:1703.04362$$chep-ex
002255384 037__ $$aCERN-EP-2017-008
002255384 035__ $$9arXiv$$aoai:arXiv.org:1703.04362
002255384 035__ $$9Inspire$$aoai:inspirehep.net:1517194$$d2024-05-03T19:41:10Z$$h2024-05-04T02:00:27Z$$mmarcxml$$ttrue$$uhttps://inspirehep.net/api/oai2d
002255384 035__ $$9Inspire$$a1517194
002255384 041__ $$aeng
002255384 088__ $$9ATLAS-STDM-2014-11-003
002255384 100__ $$aAaboud, Morad$$iINSPIRE-00511697$$tGRID:grid.410890.4$$uOujda U.$$vFaculté des Sciences - Université Mohamed Premier and LPTPM - Oujda - Morocco
002255384 245__ $$9arXiv$$aMeasurements of electroweak $Wjj$ production and constraints on anomalous gauge couplings with the ATLAS detector
002255384 246__ $$9arXiv$$aMeasurements of electroweak $Wjj$ production and constraints on anomalous gauge couplings with the ATLAS detector
002255384 260__ $$c2017-07-17
002255384 269__ $$aGeneva$$bCERN$$c13 Mar 2017
002255384 300__ $$a103 p
002255384 500__ $$9arXiv$$a103 pages in total, author list starting page 87, 58 figures, 10 tables, submitted to EPJC. All figures and tables are available at http://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/STDM-2014-11/. This version matches the journal publication
002255384 520__ $$aMeasurements of the electroweak production of a $W$ boson in association with two jets at high dijet invariant mass are performed using $\sqrt{s} = 7$ and $8$ TeV proton--proton collision data produced by the Large Hadron Collider, corresponding respectively to 4.7 and 20.2 fb$^{-1}$ of integrated luminosity collected by the ATLAS detector. The measurements are sensitive to the production of a $W$ boson via a triple-gauge-boson vertex and include both the fiducial and differential cross sections of the electroweak process.
002255384 520__ $$9Springer$$aMeasurements of the electroweak production of a W boson in association with two jets at high dijet invariant mass are performed using $\sqrt{s} =$ 7 and 8  $\text {TeV}$  proton–proton collision data produced by the Large Hadron Collider, corresponding respectively to 4.7 and 20.2 fb$^{-1}$ of integrated luminosity collected by the ATLAS detector. The measurements are sensitive to the production of a W boson via a triple-gauge-boson vertex and include both the fiducial and differential cross sections of the electroweak process.
002255384 520__ $$9arXiv$$aMeasurements of the electroweak production of a $W$ boson in association with two jets at high dijet invariant mass are performed using $\sqrt{s} = 7$ and $8$ TeV proton-proton collision data produced by the Large Hadron Collider, corresponding respectively to 4.7 and 20.2 fb$^{-1}$ of integrated luminosity collected by the ATLAS detector. The measurements are sensitive to the production of a $W$ boson via a triple-gauge-boson vertex and include both the fiducial and differential cross sections of the electroweak process.
002255384 540__ $$3Preprint$$aCC-BY-4.0
002255384 542__ $$3Preprint$$dCERN$$g2017
002255384 65017 $$2SzGeCERN$$aParticle Physics - Experiment
002255384 65017 $$2arXiv$$ahep-ex
002255384 6531_ $$9CERN$$aelectroweak interaction
002255384 6531_ $$9CERN$$aparticle and resonance production
002255384 6531_ $$9CERN$$aexperimental results
002255384 693__ $$aCERN LHC$$eATLAS
002255384 695__ $$2INSPIRE$$ap p: colliding beams
002255384 695__ $$2INSPIRE$$aW: hadroproduction
002255384 695__ $$2INSPIRE$$ajet: associated production
002255384 695__ $$2INSPIRE$$ajet: pair production
002255384 695__ $$2INSPIRE$$acoupling: gauge
002255384 695__ $$2INSPIRE$$acoupling: (3gauge boson)
002255384 695__ $$2INSPIRE$$acoupling: anomaly
002255384 695__ $$2INSPIRE$$acoupling constant: upper limit
002255384 695__ $$2INSPIRE$$ap p: scattering
002255384 695__ $$2INSPIRE$$aelectroweak interaction
002255384 695__ $$2INSPIRE$$aATLAS
002255384 695__ $$2INSPIRE$$achannel cross section: measured
002255384 695__ $$2INSPIRE$$adifferential cross section: measured
002255384 695__ $$2INSPIRE$$amass dependence
002255384 695__ $$2INSPIRE$$arapidity dependence
002255384 695__ $$2INSPIRE$$aCERN LHC Coll
002255384 695__ $$2INSPIRE$$adijet
002255384 695__ $$2INSPIRE$$aexperimental results
002255384 695__ $$2INSPIRE$$a7000 GeV-cms8000 GeV-cms
002255384 695__ $$2INSPIRE$$e7
002255384 690C_ $$aATLAS_Papers
002255384 690C_ $$aCERN
002255384 690C_ $$aARTICLE
002255384 700__ $$aAad, Georges$$iINSPIRE-00210391$$uMarseille, CPPM
002255384 700__ $$aAbbott, Brad$$iINSPIRE-00060668$$uOklahoma U.
002255384 700__ $$aAbdallah, Jalal$$iINSPIRE-00305555$$uTexas U., Arlington
002255384 700__ $$aAbdinov, Ovsat$$iINSPIRE-00210427$$uBaku, Inst. Phys.
002255384 700__ $$aAbeloos, Baptiste$$iINSPIRE-00436210$$uOrsay, LAL
002255384 700__ $$aAbidi, Syed Haider$$iINSPIRE-00537233$$uToronto U.
002255384 700__ $$aAbouZeid, Ossama$$iINSPIRE-00286103$$uUC, Santa Cruz
002255384 700__ $$aAbraham, Nicola$$iINSPIRE-00443060$$uSussex U.
002255384 700__ $$aAbramowicz, Halina$$iINSPIRE-00060790$$uTel Aviv U.
002255384 700__ $$aAbreu, Henso$$iINSPIRE-00143063$$uTechnion
002255384 700__ $$aAbreu, Ricardo$$iINSPIRE-00367022$$uOregon U.
002255384 700__ $$aAbulaiti, Yiming$$iINSPIRE-00339001$$uStockholm U.$$uStockholm U., OKC
002255384 700__ $$aAcharya, Bobby Samir$$iINSPIRE-00060856$$uINFN, Udine$$uICTP, Trieste$$uKing's Coll. London
002255384 700__ $$aAdachi, Shunsuke$$iINSPIRE-00524597$$uTokyo U., ICEPP
002255384 700__ $$aAdamczyk, Leszek$$iINSPIRE-00172476$$uAGH-UST, Cracow
002255384 700__ $$aAdams, David$$iINSPIRE-00210440$$uBrookhaven
002255384 700__ $$aAdelman, Jahred$$iINSPIRE-00041460$$uNorthern Illinois U.
002255384 700__ $$aAdersberger, Michael$$iINSPIRE-00537240$$uMunich U.
002255384 700__ $$aAdye, Tim$$iINSPIRE-00060997$$uRutherford
002255384 700__ $$aAffolder, Tony$$iINSPIRE-00061029$$uUC, Santa Cruz
002255384 700__ $$aAgatonovic-Jovin, Tatjana$$iINSPIRE-00236479$$uBelgrade U.
002255384 700__ $$aAgheorghiesei, Catalin$$iINSPIRE-00534492$$uBucharest, IFIN-HH
002255384 700__ $$aAguilar-Saavedra, Juan Antonio$$iINSPIRE-00061050$$uLIP, Lisbon$$uCAFPE, Granada
002255384 700__ $$aAhlen, Steven$$iINSPIRE-00189655$$uBoston U.
002255384 700__ $$aAhmadov, Faig$$iINSPIRE-00332895$$uDubna, JINR$$uBaku, Inst. Phys.
002255384 700__ $$aAielli, Giulio$$iINSPIRE-00210494$$uINFN, Rome$$uRome U., Tor Vergata
002255384 700__ $$aAkatsuka, Shunichi$$iINSPIRE-00535642$$uKyoto U.
002255384 700__ $$aAkerstedt, Henrik$$iINSPIRE-00367674$$uStockholm U.$$uStockholm U., OKC
002255384 700__ $$aÅkesson, Torsten Paul Ake$$iINSPIRE-00061248$$uLund U.
002255384 700__ $$aAkimov, Andrei$$iINSPIRE-00210520$$uLebedev Inst.
002255384 700__ $$aAlberghi, Gian Luigi$$iINSPIRE-00366589$$uINFN, Bologna$$uBologna U.
002255384 700__ $$aAlbert, Justin$$iINSPIRE-00145104$$uVictoria U.
002255384 700__ $$aAlconada Verzini, Maria Josefina$$iINSPIRE-00339017$$uLa Plata U.
002255384 700__ $$aAleksa, Martin$$iINSPIRE-00210567$$uCERN
002255384 700__ $$aAleksandrov, Igor$$iINSPIRE-00210579$$uDubna, JINR
002255384 700__ $$aAlexa, Calin$$iINSPIRE-00061476$$uBucharest, IFIN-HH
002255384 700__ $$aAlexander, Gideon$$iINSPIRE-00179447$$uTel Aviv U.
002255384 700__ $$aAlexopoulos, Theodoros$$iINSPIRE-00061543$$uNatl. Tech. U., Athens
002255384 700__ $$aAlhroob, Muhammad$$iINSPIRE-00210593$$uOklahoma U.
002255384 700__ $$aAli, Babar$$iINSPIRE-00518637$$uPrague, Tech. U.
002255384 700__ $$aAliev, Malik$$iINSPIRE-00210605$$uINFN, Lecce$$uSalento U.
002255384 700__ $$aAlimonti, Gianluca$$iINSPIRE-00004775$$uINFN, Milan
002255384 700__ $$aAlison, John$$iINSPIRE-00210617$$uChicago U., EFI
002255384 700__ $$aAlkire, Steven Patrick$$iINSPIRE-00400408$$uNevis Labs, Columbia U.
002255384 700__ $$aAllbrooke, Benedict$$iINSPIRE-00235773$$uSussex U.
002255384 700__ $$aAllen, Benjamin William$$iINSPIRE-00439268$$uOregon U.
002255384 700__ $$aAllport, Phillip$$iINSPIRE-00147775$$uBirmingham U.
002255384 700__ $$aAloisio, Alberto$$iINSPIRE-00210642$$uINFN, Naples$$uNaples U.
002255384 700__ $$aAlonso, Alejandro$$iINSPIRE-00210666$$uBohr Inst.
002255384 700__ $$aAlonso, Francisco$$iINSPIRE-00291080$$uLa Plata U.
002255384 700__ $$aAlpigiani, Cristiano$$iINSPIRE-00358374$$uWashington U., Seattle
002255384 700__ $$aAlshehri, Azzah Aziz$$iINSPIRE-00439334$$uGlasgow U.
002255384 700__ $$aAlstaty, Mahmoud$$iINSPIRE-00441244$$uMarseille, CPPM
002255384 700__ $$aAlvarez Gonzalez, Barbara$$iINSPIRE-00022061$$uCERN
002255384 700__ $$aΆlvarez Piqueras, Damián$$iINSPIRE-00376986$$uValencia U., IFIC
002255384 700__ $$aAlviggi, Mariagrazia$$iINSPIRE-00210678$$uINFN, Naples$$uNaples U.
002255384 700__ $$aAmadio, Brian Thomas$$iINSPIRE-00399314$$uLBL, Berkeley
002255384 700__ $$aAmaral Coutinho, Yara$$iINSPIRE-00074762$$uRio de Janeiro Federal U.
002255384 700__ $$aAmelung, Christoph$$iINSPIRE-00210696$$uBrandeis U.
002255384 700__ $$aAmidei, Dante$$iINSPIRE-00061910$$uMichigan U.
002255384 700__ $$aAmor Dos Santos, Susana Patricia$$iINSPIRE-00291676$$uLIP, Lisbon$$uCoimbra U.
002255384 700__ $$aAmorim, Antonio$$iINSPIRE-00210710$$uLIP, Lisbon$$uLisbon U., CFNUL
002255384 700__ $$aAmoroso, Simone$$iINSPIRE-00002752$$uCERN
002255384 700__ $$aAmundsen, Glenn$$iINSPIRE-00349724$$uBrandeis U.
002255384 700__ $$aAnastopoulos, Christos$$iINSPIRE-00210733$$uSheffield U.
002255384 700__ $$aAncu, Lucian Stefan$$iINSPIRE-00025195$$uGeneva U.
002255384 700__ $$aAndari, Nansi$$iINSPIRE-00143085$$uBirmingham U.
002255384 700__ $$aAndeen, Timothy$$iINSPIRE-00005735$$uTexas U.
002255384 700__ $$aAnders, Christoph Falk$$iINSPIRE-00210745$$uHeidelberg U.
002255384 700__ $$aAnders, John Kenneth$$iINSPIRE-00399325$$uLiverpool U.
002255384 700__ $$aAnderson, Kelby$$iINSPIRE-00210757$$uChicago U., EFI
002255384 700__ $$aAndreazza, Attilio$$iINSPIRE-00062128$$uINFN, Milan$$uMilan U.
002255384 700__ $$aAndrei, George Victor$$iINSPIRE-00210769$$uKirchhoff Inst. Phys.
002255384 700__ $$aAngelidakis, Stylianos$$iINSPIRE-00009427$$uAthens U.
002255384 700__ $$aAngelozzi, Ivan$$iINSPIRE-00366961$$uFOM, Amsterdam
002255384 700__ $$aAngerami, Aaron$$iINSPIRE-00210782$$uNevis Labs, Columbia U.
002255384 700__ $$aAnghinolfi, Francis$$iINSPIRE-00210799$$uCERN
002255384 700__ $$aAnisenkov, Alexey$$iINSPIRE-00291854$$uNovosibirsk State U.$$uNovosibirsk, IYF
002255384 700__ $$aAnjos, Nuno$$iINSPIRE-00210800$$uBarcelona, IFAE
002255384 700__ $$aAnnovi, Alberto$$iINSPIRE-00041435$$uINFN, Pisa$$uPisa U.
002255384 700__ $$aAntel, Claire$$iINSPIRE-00517126$$uKirchhoff Inst. Phys.
002255384 700__ $$aAntonelli, Mario$$iINSPIRE-00210812$$uFrascati
002255384 700__ $$aAntonov, Alexey$$iINSPIRE-00173552$$uMoscow Phys. Eng. Inst.
002255384 700__ $$aAntrim, Daniel Joseph$$iINSPIRE-00524603$$uUC, Irvine
002255384 700__ $$aAnulli, Fabio$$iINSPIRE-00062462$$uINFN, Rome
002255384 700__ $$aAoki, Masato$$iINSPIRE-00001575$$uKEK, Tsukuba
002255384 700__ $$aAperio Bella, Ludovica$$iINSPIRE-00286141$$uCERN
002255384 700__ $$aArabidze, Giorgi$$iINSPIRE-00305586$$uMichigan State U.
002255384 700__ $$aArai, Yasuo$$iINSPIRE-00062629$$uKEK, Tsukuba
002255384 700__ $$aAraque, Juan Pedro$$iINSPIRE-00359999$$uLIP, Lisbon
002255384 700__ $$aAraujo Ferraz, Victor$$iINSPIRE-00389281$$uRio de Janeiro Federal U.
002255384 700__ $$aArce, Ayana$$iINSPIRE-00005140$$uDuke U.
002255384 700__ $$aArdell, Rose Elisabeth$$iINSPIRE-00517130$$uRoyal Holloway, U. of London
002255384 700__ $$aArduh, Francisco Anuar$$iINSPIRE-00371726$$uLa Plata U.
002255384 700__ $$aArguin, Jean-Francois$$iINSPIRE-00049740$$uMontreal U.
002255384 700__ $$aArgyropoulos, Spyridon$$iINSPIRE-00335900$$uIowa U.
002255384 700__ $$aArik, Metin$$iINSPIRE-00062802$$uBogazici U.
002255384 700__ $$aArmbruster, Aaron James$$iINSPIRE-00210861$$uSLAC
002255384 700__ $$aArmitage, Lewis James$$iINSPIRE-00404370$$uQueen Mary, U. of London
002255384 700__ $$aArnaez, Olivier$$iINSPIRE-00210873$$uCERN
002255384 700__ $$aArnold, Hannah$$iINSPIRE-00367502$$uFreiburg U.
002255384 700__ $$aArratia, Miguel$$iINSPIRE-00360674$$uCambridge U.
002255384 700__ $$aArslan, Ozan$$iINSPIRE-00348465$$uBonn U.
002255384 700__ $$aArtamonov, Andrei$$iINSPIRE-00320346$$uMoscow, ITEP
002255384 700__ $$aArtoni, Giacomo$$iINSPIRE-00286089$$uOxford U.
002255384 700__ $$aArtz, Sebastian$$iINSPIRE-00414333$$uMainz U.
002255384 700__ $$aAsai, Shoji$$iINSPIRE-00210270$$uTokyo U., ICEPP
002255384 700__ $$aAsbah, Nedaa$$iINSPIRE-00339731$$uDESY
002255384 700__ $$aAshkenazi, Adi$$iINSPIRE-00364725$$uTel Aviv U.
002255384 700__ $$aAsquith, Lily$$iINSPIRE-00180651$$uSussex U.
002255384 700__ $$aAssamagan, Ketevi$$iINSPIRE-00152949$$uBrookhaven
002255384 700__ $$aAstalos, Robert$$iINSPIRE-00332100$$uComenius U.
002255384 700__ $$aAtkinson, Markus$$iINSPIRE-00289610$$uIllinois U., Urbana
002255384 700__ $$aAtlay, Naim Bora$$iINSPIRE-00345712$$uSiegen U.
002255384 700__ $$aAugsten, Kamil$$iINSPIRE-00013348$$uPrague, Tech. U.
002255384 700__ $$aAvolio, Giuseppe$$iINSPIRE-00210941$$uCERN
002255384 700__ $$aAxen, Bradley$$iINSPIRE-00379148$$uLBL, Berkeley
002255384 700__ $$aAyoub, Mohamad Kassem$$iINSPIRE-00389471$$uOrsay, LAL
002255384 700__ $$aAzuelos, Georges$$iINSPIRE-00063480$$uMontreal U.$$uTRIUMF
002255384 700__ $$aBaas, Alessandra$$iINSPIRE-00365509$$uKirchhoff Inst. Phys.
002255384 700__ $$aBaca, Matthew John$$iINSPIRE-00389380$$uBirmingham U.
002255384 700__ $$aBachacou, Henri$$iINSPIRE-00210989$$uIRFU, Saclay
002255384 700__ $$aBachas, Konstantinos$$iINSPIRE-00210990$$uINFN, Lecce$$uSalento U.
002255384 700__ $$aBackes, Moritz$$iINSPIRE-00211007$$uOxford U.
002255384 700__ $$aBackhaus, Malte$$iINSPIRE-00235789$$uCERN
002255384 700__ $$aBagiacchi, Paolo$$iINSPIRE-00340186$$uINFN, Rome$$uRome U.
002255384 700__ $$aBagnaia, Paolo$$iINSPIRE-00063838$$uINFN, Rome$$uRome U.
002255384 700__ $$aBaines, John$$iINSPIRE-00063905$$uRutherford
002255384 700__ $$aBajic, Milena$$iINSPIRE-00524612$$uBohr Inst.
002255384 700__ $$aBaker, Oliver Keith$$iINSPIRE-00063962$$uYale U.
002255384 700__ $$aBaldin, Evgenii$$iINSPIRE-00057771$$uNovosibirsk State U.$$uNovosibirsk, IYF
002255384 700__ $$aBalek, Petr$$iINSPIRE-00295870$$uWeizmann Inst.
002255384 700__ $$aBalestri, Thomas$$iINSPIRE-00356981$$uSUNY, Stony Brook
002255384 700__ $$aBalli, Fabrice$$iINSPIRE-00000243$$uIRFU, Saclay
002255384 700__ $$aBalunas, William Keaton$$iINSPIRE-00421104$$uPennsylvania U.
002255384 700__ $$aBanas, Elzbieta$$iINSPIRE-00211068$$uCracow, INP
002255384 700__ $$aBanerjee, Swagato$$iINSPIRE-00064260$$uWisconsin U., Madison$$uLouisville U.
002255384 700__ $$aBannoura, Arwa A E$$iINSPIRE-00360042$$uWuppertal U.
002255384 700__ $$aBarak, Liron$$iINSPIRE-00229245$$uCERN
002255384 700__ $$aBarberio, Elisabetta Luigia$$iINSPIRE-00064366$$uMelbourne U.
002255384 700__ $$aBarberis, Dario$$iINSPIRE-00064378$$uINFN, Genoa$$uGenoa U.
002255384 700__ $$aBarbero, Marlon$$iINSPIRE-00211139$$uMarseille, CPPM
002255384 700__ $$aBarillari, Teresa$$iINSPIRE-00064533$$uMunich, Max Planck Inst.
002255384 700__ $$aBarisits, Martin-Stefan$$iINSPIRE-00473067$$uCERN
002255384 700__ $$aBarklow, Timothy$$iINSPIRE-00064576$$uSLAC
002255384 700__ $$aBarlow, Nick$$iINSPIRE-00042309$$uCambridge U.
002255384 700__ $$aBarnes, Sarah Louise$$iINSPIRE-00362038$$uShanghai Jiao Tong U.
002255384 700__ $$aBarnett, Bruce$$iINSPIRE-00211160$$uRutherford
002255384 700__ $$aBarnett, Michael$$iINSPIRE-00064676$$uLBL, Berkeley
002255384 700__ $$aBarnovska-Blenessy, Zuzana$$iINSPIRE-00265099$$uHefei, CUST
002255384 700__ $$aBaroncelli, Antonio$$iINSPIRE-00064709$$uINFN, Rome
002255384 700__ $$aBarone, Gaetano$$iINSPIRE-00235799$$uBrandeis U.
002255384 700__ $$aBarr, Alan$$iINSPIRE-00064725$$uOxford U.
002255384 700__ $$aBarranco Navarro, Laura$$iINSPIRE-00441300$$uValencia U., IFIC
002255384 700__ $$aBarreiro, Fernando$$iINSPIRE-00064758$$uMadrid, Autonoma U.
002255384 700__ $$aBarreiro Guimarães da Costa, João$$iINSPIRE-00087323$$uBeijing, Inst. High Energy Phys.
002255384 700__ $$aBartoldus, Rainer$$iINSPIRE-00064943$$uSLAC
002255384 700__ $$aBarton, Adam Edward$$iINSPIRE-00229256$$uLancaster U.
002255384 700__ $$aBartos, Pavol$$iINSPIRE-00304670$$uComenius U.
002255384 700__ $$aBasalaev, Artem$$iINSPIRE-00399337$$uSt. Petersburg, INP
002255384 700__ $$aBassalat, Ahmed$$iINSPIRE-00347533$$uOrsay, LAL$$uAn Najah Natl. U.
002255384 700__ $$aBates, Richard$$iINSPIRE-00065082$$uGlasgow U.
002255384 700__ $$aBatista, Santiago Juan$$iINSPIRE-00381632$$uToronto U.
002255384 700__ $$aBatley, Richard$$iINSPIRE-00211190$$uCambridge U.
002255384 700__ $$aBattaglia, Marco$$iINSPIRE-00065121$$uUC, Santa Cruz
002255384 700__ $$aBauce, Matteo$$iINSPIRE-00243631$$uINFN, Rome$$uRome U.
002255384 700__ $$aBauer, Florian$$iINSPIRE-00657399$$uIRFU, Saclay
002255384 700__ $$aBawa, Harinder Singh$$iINSPIRE-00316070$$uSLAC$$uFresno State
002255384 700__ $$aBeacham, James$$iINSPIRE-00344428$$uOhio State U.
002255384 700__ $$aBeattie, Michael David$$iINSPIRE-00266324$$uLancaster U.
002255384 700__ $$aBeau, Tristan$$iINSPIRE-00149690$$uParis U., VI-VII
002255384 700__ $$aBeauchemin, Pierre-Hugues$$iINSPIRE-00034698$$uTufts U.
002255384 700__ $$aBechtle, Philip$$iINSPIRE-00055190$$uBonn U.
002255384 700__ $$aBeck, Hans~Peter$$iINSPIRE-00065459$$uBern U., LHEP$$uFribourg U.
002255384 700__ $$aBecker, Kathrin$$iINSPIRE-00286180$$uOxford U.
002255384 700__ $$aBecker, Maurice$$iINSPIRE-00395743$$uMainz U.
002255384 700__ $$aBeckingham, Matthew$$iINSPIRE-00217716$$uWarwick U.
002255384 700__ $$aBecot, Cyril$$iINSPIRE-00362269$$uNew York U.
002255384 700__ $$aBeddall, Andrew$$iINSPIRE-00065527$$uIstanbul, Bahcesehir U.
002255384 700__ $$aBeddall, Ayda$$iINSPIRE-00211268$$uGaziantep U.
002255384 700__ $$aBednyakov, Vadim$$iINSPIRE-00065561$$uDubna, JINR
002255384 700__ $$aBedognetti, Matteo$$iINSPIRE-00439426$$uFOM, Amsterdam
002255384 700__ $$aBee, Christopher$$iINSPIRE-00065575$$uSUNY, Stony Brook
002255384 700__ $$aBeermann, Thomas$$iINSPIRE-00346910$$uCERN
002255384 700__ $$aBegalli, Marcia$$iINSPIRE-00065602$$uRio de Janeiro Federal U.
002255384 700__ $$aBegel, Michael$$iINSPIRE-00065614$$uBrookhaven
002255384 700__ $$aBehr, Janna Katharina$$iINSPIRE-00348133$$uDESY
002255384 700__ $$aBell, Andrew Stuart$$iINSPIRE-00441191$$uUniversity Coll. London
002255384 700__ $$aBella, Gideon$$iINSPIRE-00211305$$uTel Aviv U.
002255384 700__ $$aBellagamba, Lorenzo$$iINSPIRE-00065777$$uINFN, Bologna
002255384 700__ $$aBellerive, Alain$$iINSPIRE-00065818$$uCarleton U.
002255384 700__ $$aBellomo, Massimiliano$$iINSPIRE-00211329$$uMassachusetts U., Amherst
002255384 700__ $$aBelotskiy, Konstantin$$iINSPIRE-00211335$$uMoscow Phys. Eng. Inst.
002255384 700__ $$aBeltramello, Olga$$iINSPIRE-00211347$$uCERN
002255384 700__ $$aBelyaev, Nikita$$iINSPIRE-00421168$$uMoscow Phys. Eng. Inst.
002255384 700__ $$aBenary, Odette$$iINSPIRE-00211360$$uTel Aviv U.
002255384 700__ $$aBenchekroun, Driss$$iINSPIRE-00211372$$uCasablanca U.
002255384 700__ $$aBender, Michael$$iINSPIRE-00387486$$uMunich U.
002255384 700__ $$aBendtz, Katarina$$iINSPIRE-00286205$$uStockholm U.$$uStockholm U., OKC
002255384 700__ $$aBenekos, Nektarios$$iINSPIRE-00066029$$uNatl. Tech. U., Athens
002255384 700__ $$aBenhammou, Yan$$iINSPIRE-00211400$$uTel Aviv U.
002255384 700__ $$aBenhar Noccioli, Eleonora$$iINSPIRE-00286227$$uYale U.
002255384 700__ $$aBenitez, Jose$$iINSPIRE-00016190$$uIowa U.
002255384 700__ $$aBenjamin, Douglas$$iINSPIRE-00066086$$uDuke U.
002255384 700__ $$aBenoit, Mathieu$$iINSPIRE-00211411$$uGeneva U.
002255384 700__ $$aBensinger, James$$iINSPIRE-00066127$$uBrandeis U.
002255384 700__ $$aBentvelsen, Stan$$iINSPIRE-00066169$$uFOM, Amsterdam
002255384 700__ $$aBeresford, Lydia$$iINSPIRE-00389718$$uOxford U.
002255384 700__ $$aBeretta, Matteo$$iINSPIRE-00211424$$uFrascati
002255384 700__ $$aBerge, David$$iINSPIRE-00326772$$uFOM, Amsterdam
002255384 700__ $$aBergeaas Kuutmann, Elin$$iINSPIRE-00305615$$uUppsala U., Inst. Theor. Phys.
002255384 700__ $$aBerger, Nicolas$$iINSPIRE-00066350$$uAnnecy, LAPP
002255384 700__ $$aBeringer, Jürg$$iINSPIRE-00066414$$uLBL, Berkeley
002255384 700__ $$aBerlendis, Simon$$iINSPIRE-00441396$$uLPSC, Grenoble
002255384 700__ $$aBernard, Nathan Rogers$$iINSPIRE-00383935$$uMassachusetts U., Amherst
002255384 700__ $$aBernardi, Gregorio$$iINSPIRE-00066505$$uParis U., VI-VII
002255384 700__ $$aBernius, Catrin$$iINSPIRE-00211450$$uNew York U.
002255384 700__ $$aBernlochner, Florian Urs$$iINSPIRE-00144634$$uBonn U.
002255384 700__ $$aBerry, Tracey$$iINSPIRE-00041406$$uRoyal Holloway, U. of London
002255384 700__ $$aBerta, Peter$$iINSPIRE-00349738$$uCharles U.
002255384 700__ $$aBertella, Claudia$$iINSPIRE-00235836$$uMainz U.
002255384 700__ $$aBertoli, Gabriele$$iINSPIRE-00370978$$uStockholm U.$$uStockholm U., OKC
002255384 700__ $$aBertolucci, Federico$$iINSPIRE-00211461$$uINFN, Pisa$$uPisa U.
002255384 700__ $$aBertram, Iain Alexander$$iINSPIRE-00066653$$uLancaster U.
002255384 700__ $$aBertsche, Carolyn$$iINSPIRE-00375840$$uDESY
002255384 700__ $$aBertsche, David$$iINSPIRE-00377159$$uOklahoma U.
002255384 700__ $$aBesjes, Geert-Jan$$iINSPIRE-00286235$$uBohr Inst.
002255384 700__ $$aBessidskaia Bylund, Olga$$iINSPIRE-00348474$$uStockholm U.$$uStockholm U., OKC
002255384 700__ $$aBessner, Martin Florian$$iINSPIRE-00368451$$uDESY
002255384 700__ $$aBesson, Nathalie$$iINSPIRE-00211485$$uIRFU, Saclay
002255384 700__ $$aBetancourt, Christopher$$iINSPIRE-00362040$$uFreiburg U.
002255384 700__ $$aBethani, Agni$$iINSPIRE-00202655$$uManchester U.
002255384 700__ $$aBethke, Siegfried$$iINSPIRE-00179262$$uMunich, Max Planck Inst.
002255384 700__ $$aBevan, Adrian John$$iINSPIRE-00042361$$uQueen Mary, U. of London
002255384 700__ $$aBianchi, Riccardo-Maria$$iINSPIRE-00211497$$uPittsburgh U.
002255384 700__ $$aBianco, Michele$$iINSPIRE-00211509$$uCERN
002255384 700__ $$aBiebel, Otmar$$iINSPIRE-00066953$$uMunich U.
002255384 700__ $$aBiedermann, Dustin$$iINSPIRE-00392746$$uHumboldt U., Berlin
002255384 700__ $$aBielski, Rafal$$iINSPIRE-00437899$$uManchester U.
002255384 700__ $$aBiesuz, Nicolo Vladi$$iINSPIRE-00441490$$uINFN, Pisa$$uPisa U.
002255384 700__ $$aBiglietti, Michela$$iINSPIRE-00211510$$uINFN, Rome
002255384 700__ $$aBilbao De Mendizabal, Javier$$iINSPIRE-00347373$$uGeneva U.
002255384 700__ $$aBilloud, Thomas Remy Victor$$iINSPIRE-00512807$$uMontreal U.
002255384 700__ $$aBilokon, Halina$$iINSPIRE-00211527$$uFrascati
002255384 700__ $$aBindi, Marcello$$iINSPIRE-00172094$$uGottingen U., II. Phys. Inst.
002255384 700__ $$aBingul, Ahmet$$iINSPIRE-00211539$$uGaziantep U.
002255384 700__ $$aBini, Cesare$$iINSPIRE-00211540$$uINFN, Rome$$uRome U.
002255384 700__ $$aBiondi, Silvia$$iINSPIRE-00407321$$uINFN, Bologna$$uBologna U.
002255384 700__ $$aBisanz, Tobias$$iINSPIRE-00470148$$uGottingen U., II. Phys. Inst.
002255384 700__ $$aBittrich, Carsten$$iINSPIRE-00524633$$uDresden, Tech. U.
002255384 700__ $$aBjergaard, David Martin$$iINSPIRE-00002187$$uDuke U.
002255384 700__ $$aBlack, Curtis$$iINSPIRE-00329152$$uSydney U.
002255384 700__ $$aBlack, James$$iINSPIRE-00334293$$uSLAC
002255384 700__ $$aBlack, Kevin$$iINSPIRE-00175789$$uBoston U.
002255384 700__ $$aBlackburn, Daniel$$iINSPIRE-00342691$$uWashington U., Seattle
002255384 700__ $$aBlair, Robert$$iINSPIRE-00067327$$uArgonne
002255384 700__ $$aBlazek, Tomas$$iINSPIRE-00235878$$uComenius U.
002255384 700__ $$aBloch, Ingo$$iINSPIRE-00060307$$uDESY
002255384 700__ $$aBlocker, Craig$$iINSPIRE-00067509$$uBrandeis U.
002255384 700__ $$aBlue, Andrew$$iINSPIRE-00524643$$uGlasgow U.
002255384 700__ $$aBlum, Walter$$iINSPIRE-00211566$$uMainz U.
002255384 700__ $$aBlumenschein, Ulrike$$iINSPIRE-00211570$$uQueen Mary, U. of London
002255384 700__ $$aBlunier, Sylvain$$iINSPIRE-00412983$$uChile U., Catolica
002255384 700__ $$aBobbink, Gerjan$$iINSPIRE-00211581$$uFOM, Amsterdam
002255384 700__ $$aBobrovnikov, Victor$$iINSPIRE-00229343$$uNovosibirsk State U.$$uNovosibirsk, IYF
002255384 700__ $$aBocchetta, Simona Serena$$iINSPIRE-00235887$$uLund U.
002255384 700__ $$aBocci, Andrea$$iINSPIRE-00048999$$uDuke U.
002255384 700__ $$aBock, Christopher$$iINSPIRE-00367845$$uMunich U.
002255384 700__ $$aBoehler, Michael$$iINSPIRE-00211593$$uFreiburg U.
002255384 700__ $$aBoerner, Daniela$$iINSPIRE-00439393$$uWuppertal U.
002255384 700__ $$aBogavac, Danijela$$iINSPIRE-00407355$$uMunich U.
002255384 700__ $$aBogdanchikov, Alexander$$iINSPIRE-00229367$$uNovosibirsk State U.$$uNovosibirsk, IYF
002255384 700__ $$aBohm, Christian$$iINSPIRE-00324763$$uStockholm U.
002255384 700__ $$aBoisvert, Veronique$$iINSPIRE-00067915$$uRoyal Holloway, U. of London
002255384 700__ $$aBokan, Petar$$iINSPIRE-00451520$$uUppsala U., Inst. Theor. Phys.$$uGottingen U., II. Phys. Inst.
002255384 700__ $$aBold, Tomasz$$iINSPIRE-00172488$$uAGH-UST, Cracow
002255384 700__ $$aBoldyrev, Alexey$$iINSPIRE-00340190$$uMoscow State U.
002255384 700__ $$aBomben, Marco$$iINSPIRE-00052711$$uParis U., VI-VII
002255384 700__ $$aBona, Marcella$$iINSPIRE-00049930$$uQueen Mary, U. of London
002255384 700__ $$aBoonekamp, Maarten$$iINSPIRE-00211647$$uIRFU, Saclay
002255384 700__ $$aBorisov, Anatoly$$iINSPIRE-00226538$$uSerpukhov, IHEP
002255384 700__ $$aBorissov, Guennadi$$iINSPIRE-00068300$$uLancaster U.
002255384 700__ $$aBortfeldt, Jonathan$$iINSPIRE-00295897$$uCERN
002255384 700__ $$aBortoletto, Daniela$$iINSPIRE-00068366$$uOxford U.
002255384 700__ $$aBortolotto, Valerio$$iINSPIRE-00235896$$uHong Kong, Chinese U.$$uHong Kong U.$$uHong Kong U. Sci. Tech.
002255384 700__ $$aBos, Kors$$iINSPIRE-00068375$$uFOM, Amsterdam
002255384 700__ $$aBoscherini, Davide$$iINSPIRE-00172014$$uINFN, Bologna
002255384 700__ $$aBosman, Martine$$iINSPIRE-00227227$$uBarcelona, IFAE
002255384 700__ $$aBossio Sola, Jonathan David$$iINSPIRE-00441594$$uBuenos Aires U.
002255384 700__ $$aBoudreau, Joseph$$iINSPIRE-00068562$$uPittsburgh U.
002255384 700__ $$aBouffard, Julian$$iINSPIRE-00360686$$uSUNY, Albany
002255384 700__ $$aBouhova-Thacker, Evelina Vassileva$$iINSPIRE-00211684$$uLancaster U.
002255384 700__ $$aBoumediene, Djamel Eddine$$iINSPIRE-00050723$$uClermont-Ferrand U.
002255384 700__ $$aBourdarios, Claire$$iINSPIRE-00068610$$uOrsay, LAL
002255384 700__ $$aBoutle, Sarah Kate$$iINSPIRE-00174075$$uGlasgow U.
002255384 700__ $$aBoveia, Antonio$$iINSPIRE-00041392$$uOhio State U.
002255384 700__ $$aBoyd, James$$iINSPIRE-00226553$$uCERN
002255384 700__ $$aBoyko, Igor$$iINSPIRE-00211696$$uDubna, JINR
002255384 700__ $$aBracinik, Juraj$$iINSPIRE-00068874$$uBirmingham U.
002255384 700__ $$aBrandt, Andrew$$iINSPIRE-00300274$$uTexas U., Arlington
002255384 700__ $$aBrandt, Gerhard$$iINSPIRE-00032742$$uGottingen U., II. Phys. Inst.
002255384 700__ $$aBrandt, Oleg$$iINSPIRE-00184109$$uKirchhoff Inst. Phys.
002255384 700__ $$aBratzler, Uwe$$iINSPIRE-00211726$$uTokyo Metropolitan U.
002255384 700__ $$aBrau, Benjamin$$iINSPIRE-00069043$$uMassachusetts U., Amherst
002255384 700__ $$aBrau, James$$iINSPIRE-00069055$$uOregon U.
002255384 700__ $$aBreaden Madden, William Dmitri$$iINSPIRE-00438010$$uGlasgow U.
002255384 700__ $$aBrendlinger, Kurt$$iINSPIRE-00338116$$uDESY
002255384 700__ $$aBrennan, Amelia Jean$$iINSPIRE-00345743$$uMelbourne U.
002255384 700__ $$aBrenner, Lydia$$iINSPIRE-00386479$$uFOM, Amsterdam
002255384 700__ $$aBrenner, Richard$$iINSPIRE-00211740$$uUppsala U., Inst. Theor. Phys.
002255384 700__ $$aBressler, Shikma$$iINSPIRE-00211751$$uWeizmann Inst.
002255384 700__ $$aBriglin, Daniel Lawrence$$iINSPIRE-00536605$$uBirmingham U.
002255384 700__ $$aBristow, Timothy Michael$$iINSPIRE-00342520$$uEdinburgh U.
002255384 700__ $$aBritton, Dave$$iINSPIRE-00069310$$uGlasgow U.
002255384 700__ $$aBritzger, Daniel$$iINSPIRE-00306448$$uDESY
002255384 700__ $$aBrochu, Frederic$$iINSPIRE-00211763$$uCambridge U.
002255384 700__ $$aBrock, Ian$$iINSPIRE-00069330$$uBonn U.
002255384 700__ $$aBrock, Raymond$$iINSPIRE-00069341$$uMichigan State U.
002255384 700__ $$aBrooijmans, Gustaaf$$iINSPIRE-00069444$$uNevis Labs, Columbia U.
002255384 700__ $$aBrooks, Timothy$$iINSPIRE-00235925$$uRoyal Holloway, U. of London
002255384 700__ $$aBrooks, William$$iINSPIRE-00069460$$uSanta Maria U., Valparaiso
002255384 700__ $$aBrosamer, Jacquelyn$$iINSPIRE-00354197$$uLBL, Berkeley
002255384 700__ $$aBrost, Elizabeth$$iINSPIRE-00345015$$uNorthern Illinois U.
002255384 700__ $$aBroughton, James$$iINSPIRE-00445214$$uBirmingham U.
002255384 700__ $$aBruckman de Renstrom, Pawel$$iINSPIRE-00180299$$uCracow, INP
002255384 700__ $$aBruncko, Dusan$$iINSPIRE-00179454$$uKosice, IEF
002255384 700__ $$aBruni, Alessia$$iINSPIRE-00069652$$uINFN, Bologna
002255384 700__ $$aBruni, Graziano$$iINSPIRE-00172026$$uINFN, Bologna
002255384 700__ $$aBruni, Lucrezia Stella$$iINSPIRE-00512810$$uFOM, Amsterdam
002255384 700__ $$aBrunt, Benjamin$$iINSPIRE-00439507$$uCambridge U.
002255384 700__ $$aBruschi, Marco$$iINSPIRE-00211789$$uINFN, Bologna
002255384 700__ $$aBruscino, Nello$$iINSPIRE-00405244$$uBonn U.
002255384 700__ $$aBryant, Patrick$$iINSPIRE-00438028$$uChicago U., EFI
002255384 700__ $$aBryngemark, Lene$$iINSPIRE-00329497$$uLund U.
002255384 700__ $$aBuanes, Trygve$$iINSPIRE-00229479$$uBergen U.
002255384 700__ $$aBuat, Quentin$$iINSPIRE-00235948$$uSimon Fraser U.
002255384 700__ $$aBuchholz, Peter$$iINSPIRE-00069835$$uSiegen U.
002255384 700__ $$aBuckley, Andrew$$iINSPIRE-00211807$$uGlasgow U.
002255384 700__ $$aBudagov, Ioulian$$iINSPIRE-00211819$$uDubna, JINR
002255384 700__ $$aBuehrer, Felix$$iINSPIRE-00356527$$uFreiburg U.
002255384 700__ $$aBugge, Magnar Kopangen$$iINSPIRE-00298334$$uOslo U.
002255384 700__ $$aBulekov, Oleg$$iINSPIRE-00211832$$uMoscow Phys. Eng. Inst.
002255384 700__ $$aBullock, Daniel$$iINSPIRE-00399438$$uTexas U., Arlington
002255384 700__ $$aBurckhart, Helfried$$iINSPIRE-00211868$$uCERN
002255384 700__ $$aBurdin, Sergey$$iINSPIRE-00022855$$uLiverpool U.
002255384 700__ $$aBurgard, Carsten Daniel$$iINSPIRE-00423318$$uFreiburg U.
002255384 700__ $$aBurger, Angela Maria$$iINSPIRE-00530530$$uAnnecy, LAPP
002255384 700__ $$aBurghgrave, Blake$$iINSPIRE-00354209$$uNorthern Illinois U.
002255384 700__ $$aBurka, Klaudia$$iINSPIRE-00438133$$uCracow, INP
002255384 700__ $$aBurke, Stephen$$iINSPIRE-00211870$$uRutherford
002255384 700__ $$aBurmeister, Ingo$$iINSPIRE-00348374$$uDortmund U.
002255384 700__ $$aBurr, Jonathan Thomas Peter$$iINSPIRE-00512821$$uOxford U.
002255384 700__ $$aBusato, Emmanuel$$iINSPIRE-00051595$$uClermont-Ferrand U.
002255384 700__ $$aBüscher, Daniel$$iINSPIRE-00368463$$uFreiburg U.
002255384 700__ $$aBüscher, Volker$$iINSPIRE-00070225$$uMainz U.
002255384 700__ $$aBussey, Peter$$iINSPIRE-00070265$$uGlasgow U.
002255384 700__ $$aButler, John$$iINSPIRE-00179876$$uBoston U.
002255384 700__ $$aButtar, Craig$$iINSPIRE-00160192$$uGlasgow U.
002255384 700__ $$aButterworth, Jonathan$$iINSPIRE-00070318$$uUniversity Coll. London
002255384 700__ $$aButti, Pierfrancesco$$iINSPIRE-00358725$$uCERN
002255384 700__ $$aButtinger, William$$iINSPIRE-00229496$$uBrookhaven
002255384 700__ $$aBuzatu, Adrian$$iINSPIRE-00025104$$uTsinghua U., Beijing
002255384 700__ $$aBuzykaev, Aleksey$$iINSPIRE-00003784$$uNovosibirsk State U.$$uNovosibirsk, IYF
002255384 700__ $$aCabrera Urbán, Susana$$iINSPIRE-00211900$$uValencia U., IFIC
002255384 700__ $$aCaforio, Davide$$iINSPIRE-00211911$$uPrague, Tech. U.
002255384 700__ $$aCairo, Valentina$$iINSPIRE-00403090$$uINFN, Cosenza$$uCalabria U.
002255384 700__ $$aCakir, Orhan$$iINSPIRE-00211923$$uAnkara U.
002255384 700__ $$aCalace, Noemi$$iINSPIRE-00408949$$uGeneva U.
002255384 700__ $$aCalafiura, Paolo$$iINSPIRE-00070566$$uLBL, Berkeley
002255384 700__ $$aCalandri, Alessandro$$iINSPIRE-00366978$$uMarseille, CPPM
002255384 700__ $$aCalderini, Giovanni$$iINSPIRE-00070597$$uParis U., VI-VII
002255384 700__ $$aCalfayan, Philippe$$iINSPIRE-00032964$$uIndiana U.
002255384 700__ $$aCallea, Giuseppe$$iINSPIRE-00514504$$uINFN, Cosenza$$uCalabria U.
002255384 700__ $$aCaloba, Luiz$$iINSPIRE-00211947$$uRio de Janeiro Federal U.
002255384 700__ $$aCalvente Lopez, Sergio$$iINSPIRE-00511707$$uMadrid, Autonoma U.
002255384 700__ $$aCalvet, David$$iINSPIRE-00070696$$uClermont-Ferrand U.
002255384 700__ $$aCalvet, Samuel$$iINSPIRE-00019519$$uClermont-Ferrand U.
002255384 700__ $$aCalvet, Thomas Philippe$$iINSPIRE-00438295$$uMarseille, CPPM
002255384 700__ $$aCamacho Toro, Reina$$iINSPIRE-00235957$$uChicago U., EFI
002255384 700__ $$aCamarda, Stefano$$iINSPIRE-00012655$$uCERN
002255384 700__ $$aCamarri, Paolo$$iINSPIRE-00226571$$uINFN, Rome$$uRome U., Tor Vergata
002255384 700__ $$aCameron, David$$iINSPIRE-00226583$$uOslo U.
002255384 700__ $$aCaminal Armadans, Roger$$iINSPIRE-00337611$$uIllinois U., Urbana
002255384 700__ $$aCamincher, Clement$$iINSPIRE-00438457$$uLPSC, Grenoble
002255384 700__ $$aCampana, Simone$$iINSPIRE-00211959$$uCERN
002255384 700__ $$aCampanelli, Mario$$iINSPIRE-00070797$$uUniversity Coll. London
002255384 700__ $$aCamplani, Alessandra$$iINSPIRE-00452211$$uINFN, Milan$$uMilan U.
002255384 700__ $$aCampoverde, Angel$$iINSPIRE-00349667$$uSiegen U.
002255384 700__ $$aCanale, Vincenzo$$iINSPIRE-00211960$$uINFN, Naples$$uNaples U.
002255384 700__ $$aCano Bret, Marc$$iINSPIRE-00361241$$uShanghai Jiao Tong U.
002255384 700__ $$aCantero, Josu$$iINSPIRE-00211972$$uOklahoma State U.
002255384 700__ $$aCao, Tingting$$iINSPIRE-00334314$$uTel Aviv U.
002255384 700__ $$aCapeans Garrido, Maria Del Mar$$iINSPIRE-00083814$$uCERN
002255384 700__ $$aCaprini, Irinel$$iINSPIRE-00070986$$uBucharest, IFIN-HH
002255384 700__ $$aCaprini, Mihai$$iINSPIRE-00211990$$uBucharest, IFIN-HH
002255384 700__ $$aCapua, Marcella$$iINSPIRE-00053925$$uINFN, Cosenza$$uCalabria U.
002255384 700__ $$aCarbone, Ryne Michael$$iINSPIRE-00424300$$uNevis Labs, Columbia U.
002255384 700__ $$aCardarelli, Roberto$$iINSPIRE-00212037$$uINFN, Rome
002255384 700__ $$aCardillo, Fabio$$iINSPIRE-00407956$$uFreiburg U.
002255384 700__ $$aCarli, Ina$$iINSPIRE-00235989$$uCharles U.
002255384 700__ $$aCarli, Tancredi$$iINSPIRE-00212045$$uCERN
002255384 700__ $$aCarlino, Gianpaolo$$iINSPIRE-00212057$$uINFN, Naples
002255384 700__ $$aCarlson, Benjamin Taylor$$iINSPIRE-00340092$$uPittsburgh U.
002255384 700__ $$aCarminati, Leonardo$$iINSPIRE-00212069$$uINFN, Milan$$uMilan U.
002255384 700__ $$aCarney, Rebecca$$iINSPIRE-00524651$$uStockholm U.$$uStockholm U., OKC
002255384 700__ $$aCaron, Sascha$$iINSPIRE-00057327$$uNIKHEF, Amsterdam
002255384 700__ $$aCarquin, Edson$$iINSPIRE-00023484$$uSanta Maria U., Valparaiso
002255384 700__ $$aCarrillo-Montoya, German D$$iINSPIRE-00212072$$uCERN
002255384 700__ $$aCarvalho, João$$iINSPIRE-00226606$$uLIP, Lisbon$$uCoimbra U.
002255384 700__ $$aCasadei, Diego$$iINSPIRE-00212084$$uBirmingham U.
002255384 700__ $$aCasado, Maria Pilar$$iINSPIRE-00071410$$uBarcelona, IFAE$$uBarcelona, Autonoma U.
002255384 700__ $$aCasolino, Mirkoantonio$$iINSPIRE-00366594$$uBarcelona, IFAE
002255384 700__ $$aCasper, David William$$iINSPIRE-00071474$$uUC, Irvine
002255384 700__ $$aCastelijn, Remco$$iINSPIRE-00443025$$uFOM, Amsterdam
002255384 700__ $$aCastelli, Angelantonio$$iINSPIRE-00342579$$uFOM, Amsterdam
002255384 700__ $$aCastillo Gimenez, Victoria$$iINSPIRE-00212120$$uValencia U., IFIC
002255384 700__ $$aCastro, Nuno Filipe$$iINSPIRE-00036257$$uLIP, Lisbon$$uPorto U.
002255384 700__ $$aCatinaccio, Andrea$$iINSPIRE-00212343$$uCERN
002255384 700__ $$aCatmore, James$$iINSPIRE-00212355$$uOslo U.
002255384 700__ $$aCattai, Ariella$$iINSPIRE-00320450$$uCERN
002255384 700__ $$aCaudron, Julien$$iINSPIRE-00308115$$uBonn U.
002255384 700__ $$aCavaliere, Viviana$$iINSPIRE-00010976$$uIllinois U., Urbana
002255384 700__ $$aCavallaro, Emanuele$$iINSPIRE-00451731$$uBarcelona, IFAE
002255384 700__ $$aCavalli, Donatella$$iINSPIRE-00212386$$uINFN, Milan
002255384 700__ $$aCavalli-Sforza, Matteo$$iINSPIRE-00071735$$uBarcelona, IFAE
002255384 700__ $$aCavasinni, Vincenzo$$iINSPIRE-00212398$$uINFN, Pisa$$uPisa U.
002255384 700__ $$aCelebi, Emre$$iINSPIRE-00406045$$uBogazici U.
002255384 700__ $$aCeradini, Filippo$$iINSPIRE-00071916$$uINFN, Rome$$uRome III U.
002255384 700__ $$aCerda Alberich, Leonor$$iINSPIRE-00431162$$uValencia U., IFIC
002255384 700__ $$aSantiago Cerqueira, Augusto$$iINSPIRE-00212405$$uJuiz de Fora U.
002255384 700__ $$aCerri, Alessandro$$iINSPIRE-00050967$$uSussex U.
002255384 700__ $$aCerrito, Lucio$$iINSPIRE-00050901$$uINFN, Rome$$uRome U., Tor Vergata
002255384 700__ $$aCerutti, Fabio$$iINSPIRE-00212418$$uLBL, Berkeley
002255384 700__ $$aCervelli, Alberto$$iINSPIRE-00025073$$uBern U., LHEP
002255384 700__ $$aCetin, Serkant Ali$$iINSPIRE-00186619$$uIstanbul Bilgi U.
002255384 700__ $$aChafaq, Aziz$$iINSPIRE-00212424$$uCasablanca U.
002255384 700__ $$aChakraborty, Dhiman$$iINSPIRE-00071985$$uNorthern Illinois U.
002255384 700__ $$aChan, Stephen Kam-wah$$iINSPIRE-00445289$$uHarvard U., Phys. Dept.
002255384 700__ $$aChan, Wing Sheung$$iINSPIRE-00534577$$uFOM, Amsterdam
002255384 700__ $$aChan, Yat Long$$iINSPIRE-00436344$$uHong Kong, Chinese U.
002255384 700__ $$aChang, Philip$$iINSPIRE-00015510$$uIllinois U., Urbana
002255384 700__ $$aChapman, John Derek$$iINSPIRE-00029402$$uCambridge U.
002255384 700__ $$aCharlton, Dave$$iINSPIRE-00072301$$uBirmingham U.
002255384 700__ $$aChatterjee, Avishek$$iINSPIRE-00012825$$uGeneva U.
002255384 700__ $$aChau, Chav Chhiv$$iINSPIRE-00362051$$uToronto U.
002255384 700__ $$aChavez Barajas, Carlos Alberto$$iINSPIRE-00235990$$uSussex U.
002255384 700__ $$aChe, Siinn$$iINSPIRE-00425189$$uOhio State U.
002255384 700__ $$aCheatham, Susan$$iINSPIRE-00212448$$uINFN, Udine$$uUdine U.
002255384 700__ $$aChegwidden, Andrew$$iINSPIRE-00358737$$uMichigan State U.
002255384 700__ $$aChekanov, Sergei$$iINSPIRE-00072460$$uArgonne
002255384 700__ $$aChekulaev, Sergey$$iINSPIRE-00212450$$uTRIUMF
002255384 700__ $$aChelkov, Gueorgui$$iINSPIRE-00212473$$uDubna, JINR$$uTomsk State U.
002255384 700__ $$aChelstowska, Magda Anna$$iINSPIRE-00236000$$uCERN
002255384 700__ $$aChen, Chunhui$$iINSPIRE-00058105$$uIowa State U.
002255384 700__ $$aChen, Hucheng$$iINSPIRE-00304146$$uBrookhaven
002255384 700__ $$aChen, Shenjian$$iINSPIRE-00072626$$uNanjing U.
002255384 700__ $$aChen, Shion$$iINSPIRE-00417808$$uTokyo U., ICEPP
002255384 700__ $$aChen, Xin$$iINSPIRE-00145153$$uTsinghua U., Beijing$$uCICQM, Beijing
002255384 700__ $$aChen, Ye$$iINSPIRE-00377001$$uKobe U.
002255384 700__ $$aCheng, Hok Chuen$$iINSPIRE-00357007$$uMichigan U.
002255384 700__ $$aCheng, Huajie$$iINSPIRE-00438626$$uBeijing, Inst. High Energy Phys.
002255384 700__ $$aCheng, Yangyang$$iINSPIRE-00291862$$uChicago U., EFI
002255384 700__ $$aCheplakov, Alexander$$iINSPIRE-00001054$$uDubna, JINR
002255384 700__ $$aCheremushkina, Evgenia$$iINSPIRE-00371738$$uSerpukhov, IHEP
002255384 700__ $$aCherkaoui El Moursli, Rajaa$$iINSPIRE-00212497$$uMohammed V U., Agdal
002255384 700__ $$aChernyatin, Valeriy$$iINSPIRE-00212509$$uBrookhaven
002255384 700__ $$aCheu, Elliott$$iINSPIRE-00072813$$uArizona U.
002255384 700__ $$aChevalier, Laurent$$iINSPIRE-00212532$$uIRFU, Saclay
002255384 700__ $$aChiarella, Vitaliano$$iINSPIRE-00332290$$uFrascati
002255384 700__ $$aChiarelli, Giorgio$$iINSPIRE-00072892$$uINFN, Pisa$$uPisa U.
002255384 700__ $$aChiodini, Gabriele$$iINSPIRE-00212573$$uINFN, Lecce
002255384 700__ $$aChisholm, Andrew$$iINSPIRE-00236049$$uCERN
002255384 700__ $$aChitan, Adrian$$iINSPIRE-00236054$$uBucharest, IFIN-HH
002255384 700__ $$aChiu, Yu Him Justin$$iINSPIRE-00534627$$uVictoria U.
002255384 700__ $$aChizhov, Mihail$$iINSPIRE-00227239$$uDubna, JINR
002255384 700__ $$aChoi, Kyungeon$$iINSPIRE-00180982$$uIndiana U.
002255384 700__ $$aChomont, Arthur Rene$$iINSPIRE-00445232$$uClermont-Ferrand U.
002255384 700__ $$aChouridou, Sofia$$iINSPIRE-00212583$$uAthens U.
002255384 700__ $$aChow, Bonnie Kar Bo$$iINSPIRE-00334326$$uMunich U.
002255384 700__ $$aChristodoulou, Valentinos$$iINSPIRE-00407394$$uUniversity Coll. London
002255384 700__ $$aChromek-Burckhart, Doris$$iINSPIRE-00305640$$uCERN
002255384 700__ $$aChu, Ming Chung$$iINSPIRE-00436262$$uHong Kong, Chinese U.
002255384 700__ $$aChudoba, Jiri$$iINSPIRE-00150160$$uPrague, Inst. Phys.
002255384 700__ $$aChuinard, Annabelle Julia$$iINSPIRE-00378509$$uMcGill U.
002255384 700__ $$aChwastowski, Janusz$$iINSPIRE-00172390$$uCracow, INP
002255384 700__ $$aChytka, Ladislav$$iINSPIRE-00355090$$uPalacky U.
002255384 700__ $$aCiftci, Abbas Kenan$$iINSPIRE-00212614$$uAnkara U.
002255384 700__ $$aCinca, Diane$$iINSPIRE-00212637$$uDortmund U.
002255384 700__ $$aCindro, Vladimir$$iINSPIRE-00073566$$uStefan Inst., Ljubljana
002255384 700__ $$aCioara, Irina Antonela$$iINSPIRE-00395821$$uBonn U.
002255384 700__ $$aCiocca, Claudia$$iINSPIRE-00034559$$uINFN, Bologna$$uBologna U.
002255384 700__ $$aCiocio, Alessandra$$iINSPIRE-00073579$$uLBL, Berkeley
002255384 700__ $$aCirotto, Francesco$$iINSPIRE-00414488$$uINFN, Naples$$uNaples U.
002255384 700__ $$aCitron, Zvi Hirsh$$iINSPIRE-00241320$$uWeizmann Inst.
002255384 700__ $$aCitterio, Mauro$$iINSPIRE-00339611$$uINFN, Milan
002255384 700__ $$aCiubancan, Mihai$$iINSPIRE-00286339$$uBucharest, IFIN-HH
002255384 700__ $$aClark, Allan G$$iINSPIRE-00073664$$uGeneva U.
002255384 700__ $$aClark, Brian Lee$$iINSPIRE-00399058$$uHarvard U., Phys. Dept.
002255384 700__ $$aClark, Michael$$iINSPIRE-00443146$$uNevis Labs, Columbia U.
002255384 700__ $$aClark, Philip James$$iINSPIRE-00144539$$uEdinburgh U.
002255384 700__ $$aClarke, Robert$$iINSPIRE-00287453$$uLBL, Berkeley
002255384 700__ $$aClement, Christophe$$iINSPIRE-00147062$$uStockholm U.$$uStockholm U., OKC
002255384 700__ $$aCoadou, Yann$$iINSPIRE-00054627$$uMarseille, CPPM
002255384 700__ $$aCobal, Marina$$iINSPIRE-00073873$$uINFN, Udine$$uUdine U.
002255384 700__ $$aCoccaro, Andrea$$iINSPIRE-00212651$$uGeneva U.
002255384 700__ $$aCochran, James H$$iINSPIRE-00145182$$uIowa State U.
002255384 700__ $$aColasurdo, Luca$$iINSPIRE-00397129$$uNIKHEF, Amsterdam
002255384 700__ $$aCole, Brian$$iINSPIRE-00049517$$uNevis Labs, Columbia U.
002255384 700__ $$aColijn, Auke-Pieter$$iINSPIRE-00212675$$uFOM, Amsterdam
002255384 700__ $$aCollot, Johann$$iINSPIRE-00074106$$uLPSC, Grenoble
002255384 700__ $$aColombo, Tommaso$$iINSPIRE-00337030$$uUC, Irvine
002255384 700__ $$aConde Muiño, Patricia$$iINSPIRE-00212700$$uLIP, Lisbon$$uLisbon U., CFNUL
002255384 700__ $$aConiavitis, Elias$$iINSPIRE-00004566$$uFreiburg U.
002255384 700__ $$aConnell, Simon Henry$$iINSPIRE-00148123$$uJohannesburg U.
002255384 700__ $$aConnelly, Ian$$iINSPIRE-00352736$$uManchester U.
002255384 700__ $$aConsorti, Valerio$$iINSPIRE-00236081$$uFreiburg U.
002255384 700__ $$aConstantinescu, Serban$$iINSPIRE-00212724$$uBucharest, IFIN-HH
002255384 700__ $$aConti, Geraldine$$iINSPIRE-00260499$$uCERN
002255384 700__ $$aConventi, Francesco$$iINSPIRE-00212748$$uINFN, Naples$$uNaples, Inst. U. Navale
002255384 700__ $$aCooke, Mark$$iINSPIRE-00183948$$uLBL, Berkeley
002255384 700__ $$aCooper, Ben$$iINSPIRE-00041328$$uUniversity Coll. London
002255384 700__ $$aCooper-Sarkar, Amanda$$iINSPIRE-00074346$$uOxford U.
002255384 700__ $$aCormier, Felix$$iINSPIRE-00530543$$uBritish Columbia U.
002255384 700__ $$aCormier, Kyle James Read$$iINSPIRE-00512833$$uToronto U.
002255384 700__ $$aCornelissen, Thijs$$iINSPIRE-00212766$$uWuppertal U.
002255384 700__ $$aCorradi, Massimo$$iINSPIRE-00001854$$uINFN, Rome$$uRome U.
002255384 700__ $$aCorriveau, Francois$$iINSPIRE-00074601$$uMcGill U.$$uIPP, Canada
002255384 700__ $$aCortes-Gonzalez, Arely$$iINSPIRE-00212778$$uCERN
002255384 700__ $$aCortiana, Giorgio$$iINSPIRE-00041311$$uMunich, Max Planck Inst.
002255384 700__ $$aCosta, Giuseppe$$iINSPIRE-00212780$$uINFN, Milan
002255384 700__ $$aCosta, María José$$iINSPIRE-00212791$$uValencia U., IFIC
002255384 700__ $$aCostanzo, Davide$$iINSPIRE-00212803$$uSheffield U.
002255384 700__ $$aCottin, Giovanna$$iINSPIRE-00334334$$uCambridge U.
002255384 700__ $$aCowan, Glen$$iINSPIRE-00145177$$uRoyal Holloway, U. of London
002255384 700__ $$aCox, Brian$$iINSPIRE-00074854$$uManchester U.
002255384 700__ $$aCranmer, Kyle$$iINSPIRE-00074922$$uNew York U.
002255384 700__ $$aCrawley, Samuel Joseph$$iINSPIRE-00399580$$uGlasgow U.
002255384 700__ $$aCreager, Rachael$$iINSPIRE-00524662$$uPennsylvania U.
002255384 700__ $$aCree, Graham$$iINSPIRE-00349746$$uCarleton U.
002255384 700__ $$aCrépé-Renaudin, Sabine$$iINSPIRE-00074993$$uLPSC, Grenoble
002255384 700__ $$aCrescioli, Francesco$$iINSPIRE-00030662$$uParis U., VI-VII
002255384 700__ $$aCribbs, Wayne Allen$$iINSPIRE-00360698$$uStockholm U.$$uStockholm U., OKC
002255384 700__ $$aCrispin Ortuzar, Mireia$$iINSPIRE-00339030$$uOxford U.
002255384 700__ $$aCristinziani, Markus$$iINSPIRE-00058643$$uBonn U.
002255384 700__ $$aCroft, Vince$$iINSPIRE-00366990$$uNIKHEF, Amsterdam
002255384 700__ $$aCrosetti, Giovanni$$iINSPIRE-00212870$$uINFN, Cosenza$$uCalabria U.
002255384 700__ $$aCueto, Ana$$iINSPIRE-00517145$$uMadrid, Autonoma U.
002255384 700__ $$aCuhadar Donszelmann, Tulay$$iINSPIRE-00043040$$uSheffield U.
002255384 700__ $$aCummings, Jane$$iINSPIRE-00329170$$uYale U.
002255384 700__ $$aCuratolo, Maria$$iINSPIRE-00212948$$uFrascati
002255384 700__ $$aCúth, Jakub$$iINSPIRE-00384079$$uMainz U.
002255384 700__ $$aCzirr, Hendrik$$iINSPIRE-00229786$$uSiegen U.
002255384 700__ $$aCzodrowski, Patrick$$iINSPIRE-00236101$$uCERN
002255384 700__ $$aD'amen, Gabriele$$iINSPIRE-00508870$$uINFN, Bologna$$uBologna U.
002255384 700__ $$aD'Auria, Saverio$$iINSPIRE-00212973$$uGlasgow U.
002255384 700__ $$aD'Onofrio, Monica$$iINSPIRE-00041292$$uLiverpool U.
002255384 700__ $$aDa Cunha Sargedas De Sousa, Mario Jose$$iINSPIRE-00339043$$uLIP, Lisbon$$uLisbon U., CFNUL
002255384 700__ $$aDa Via, Cinzia$$iINSPIRE-00212924$$uManchester U.
002255384 700__ $$aDabrowski, Wladyslaw$$iINSPIRE-00178895$$uAGH-UST, Cracow
002255384 700__ $$aDado, Tomas$$iINSPIRE-00508032$$uComenius U.
002255384 700__ $$aDai, Tiesheng$$iINSPIRE-00212987$$uMichigan U.
002255384 700__ $$aDale, Orjan$$iINSPIRE-00358740$$uBergen U.
002255384 700__ $$aDallaire, Frederick$$iINSPIRE-00334341$$uMontreal U.
002255384 700__ $$aDallapiccola, Carlo$$iINSPIRE-00075606$$uMassachusetts U., Amherst
002255384 700__ $$aDam, Mogens$$iINSPIRE-00075612$$uBohr Inst.
002255384 700__ $$aDandoy, Jeffrey$$iINSPIRE-00396074$$uPennsylvania U.
002255384 700__ $$aDang, Nguyen Phuong$$iINSPIRE-00410760$$uFreiburg U.
002255384 700__ $$aDaniells, Andrew Christopher$$iINSPIRE-00338698$$uBirmingham U.
002255384 700__ $$aDann, Nicholas Stuart$$iINSPIRE-00443230$$uManchester U.
002255384 700__ $$aDanninger, Matthias$$iINSPIRE-00324867$$uBritish Columbia U.
002255384 700__ $$aDano Hoffmann, Maria$$iINSPIRE-00354223$$uIRFU, Saclay
002255384 700__ $$aDao, Valerio$$iINSPIRE-00213005$$uSUNY, Stony Brook
002255384 700__ $$aDarbo, Giovanni$$iINSPIRE-00213017$$uINFN, Genoa
002255384 700__ $$aDarmora, Smita$$iINSPIRE-00337045$$uTexas U., Arlington
002255384 700__ $$aDassoulas, James$$iINSPIRE-00286438$$uAlberta U.
002255384 700__ $$aDattagupta, Aparajita$$iINSPIRE-00221224$$uOregon U.
002255384 700__ $$aDaubney, Thomas$$iINSPIRE-00535012$$uDESY
002255384 700__ $$aDavey, Will$$iINSPIRE-00213030$$uBonn U.
002255384 700__ $$aDavid, Claire$$iINSPIRE-00342591$$uDESY
002255384 700__ $$aDavidek, Tomas$$iINSPIRE-00075913$$uCharles U.
002255384 700__ $$aDavies, Merlin$$iINSPIRE-00213066$$uTel Aviv U.
002255384 700__ $$aDavison, Peter$$iINSPIRE-00345754$$uUniversity Coll. London
002255384 700__ $$aDawe, Edmund$$iINSPIRE-00213080$$uMelbourne U.
002255384 700__ $$aDawson, Ian$$iINSPIRE-00213091$$uSheffield U.
002255384 700__ $$aDe, Kaushik$$iINSPIRE-00300320$$uTexas U., Arlington
002255384 700__ $$ade Asmundis, Riccardo$$iINSPIRE-00213110$$uINFN, Naples
002255384 700__ $$aDe Benedetti, Abraham$$iINSPIRE-00018357$$uOklahoma U.
002255384 700__ $$aDe Castro, Stefano$$iINSPIRE-00213121$$uINFN, Bologna$$uBologna U.
002255384 700__ $$aDe Cecco, Sandro$$iINSPIRE-00041280$$uParis U., VI-VII
002255384 700__ $$aDe Groot, Nicolo$$iINSPIRE-00213157$$uNIKHEF, Amsterdam
002255384 700__ $$ade Jong, Paul$$iINSPIRE-00093889$$uFOM, Amsterdam
002255384 700__ $$aDe la Torre, Hector$$iINSPIRE-00236142$$uMichigan State U.
002255384 700__ $$aDe Lorenzi, Francesco$$iINSPIRE-00257970$$uIowa State U.
002255384 700__ $$aDe Maria, Antonio$$iINSPIRE-00470316$$uGottingen U., II. Phys. Inst.
002255384 700__ $$aDe Pedis, Daniele$$iINSPIRE-00213170$$uINFN, Rome
002255384 700__ $$aDe Salvo, Alessandro$$iINSPIRE-00213182$$uINFN, Rome
002255384 700__ $$aDe Sanctis, Umberto$$iINSPIRE-00213194$$uSussex U.
002255384 700__ $$aDe Santo, Antonella$$iINSPIRE-00076214$$uSussex U.
002255384 700__ $$aDe Vasconcelos Corga, Kevin$$iINSPIRE-00535026$$uMarseille, CPPM
002255384 700__ $$aDe Vivie De Regie, Jean-Baptiste$$iINSPIRE-00213200$$uOrsay, LAL
002255384 700__ $$aDearnaley, William James$$iINSPIRE-00286454$$uLancaster U.
002255384 700__ $$aDebbe, Ramiro$$iINSPIRE-00181116$$uBrookhaven
002255384 700__ $$aDebenedetti, Chiara$$iINSPIRE-00236155$$uUC, Santa Cruz
002255384 700__ $$aDedovich, Dmitri$$iINSPIRE-00213224$$uDubna, JINR
002255384 700__ $$aDehghanian, Nooshin$$iINSPIRE-00452091$$uAlberta U.
002255384 700__ $$aDeigaard, Ingrid$$iINSPIRE-00358135$$uFOM, Amsterdam
002255384 700__ $$aDel Gaudio, Michela$$iINSPIRE-00507162$$uINFN, Cosenza$$uCalabria U.
002255384 700__ $$aDel Peso, Jose$$iINSPIRE-00173501$$uMadrid, Autonoma U.
002255384 700__ $$aDel Prete, Tarcisio$$iINSPIRE-00186417$$uINFN, Pisa$$uPisa U.
002255384 700__ $$aDelgove, David$$iINSPIRE-00396179$$uOrsay, LAL
002255384 700__ $$aDeliot, Frederic$$iINSPIRE-00076511$$uIRFU, Saclay
002255384 700__ $$aDelitzsch, Chris Malena$$iINSPIRE-00364737$$uGeneva U.
002255384 700__ $$aDell'Acqua, Andrea$$iINSPIRE-00213248$$uCERN
002255384 700__ $$aDell'Asta, Lidia$$iINSPIRE-00213250$$uBoston U.
002255384 700__ $$aDell'Orso, Mauro$$iINSPIRE-00113420$$uINFN, Pisa$$uPisa U.
002255384 700__ $$aDella Pietra, Massimo$$iINSPIRE-00213261$$uINFN, Naples$$uNaples U.
002255384 700__ $$adella Volpe, Domenico$$iINSPIRE-00134280$$uGeneva U.
002255384 700__ $$aDelmastro, Marco$$iINSPIRE-00213273$$uAnnecy, LAPP
002255384 700__ $$aDelsart, Pierre-Antoine$$iINSPIRE-00213285$$uLPSC, Grenoble
002255384 700__ $$aDeMarco, David$$iINSPIRE-00381792$$uToronto U.
002255384 700__ $$aDemers, Sarah$$iINSPIRE-00177331$$uYale U.
002255384 700__ $$aDemichev, Mikhail$$iINSPIRE-00213297$$uDubna, JINR
002255384 700__ $$aDemilly, Aurelien$$iINSPIRE-00339052$$uParis U., VI-VII
002255384 700__ $$aDenisov, Sergey$$iINSPIRE-00076710$$uSerpukhov, IHEP
002255384 700__ $$aDenysiuk, Denys$$iINSPIRE-00436410$$uIRFU, Saclay
002255384 700__ $$aDerendarz, Dominik$$iINSPIRE-00229900$$uCracow, INP
002255384 700__ $$aDerkaoui, Jamal Eddine$$iINSPIRE-00213315$$uOujda U.
002255384 700__ $$aDerue, Frederic$$iINSPIRE-00051568$$uParis U., VI-VII
002255384 700__ $$aDervan, Paul$$iINSPIRE-00076798$$uLiverpool U.
002255384 700__ $$aDesch, Klaus Kurt$$iINSPIRE-00076819$$uBonn U.
002255384 700__ $$aDeterre, Cecile$$iINSPIRE-00220614$$uDESY
002255384 700__ $$aDette, Karola$$iINSPIRE-00439451$$uDortmund U.
002255384 700__ $$aDeviveiros, Pier-Olivier$$iINSPIRE-00326955$$uCERN
002255384 700__ $$aDewhurst, Alastair$$iINSPIRE-00213327$$uRutherford
002255384 700__ $$aDhaliwal, Saminder$$iINSPIRE-00213340$$uBrandeis U.
002255384 700__ $$aDi Ciaccio, Anna$$iINSPIRE-00213364$$uINFN, Rome$$uRome U., Tor Vergata
002255384 700__ $$aDi Ciaccio, Lucia$$iINSPIRE-00213376$$uAnnecy, LAPP
002255384 700__ $$aDi Clemente, William Kennedy$$iINSPIRE-00431482$$uPennsylvania U.
002255384 700__ $$aDi Donato, Camilla$$iINSPIRE-00297740$$uINFN, Naples$$uNaples U.
002255384 700__ $$aDi Girolamo, Alessandro$$iINSPIRE-00213388$$uCERN
002255384 700__ $$aDi Girolamo, Beniamino$$iINSPIRE-00085048$$uCERN
002255384 700__ $$aDi Micco, Biagio$$iINSPIRE-00236191$$uINFN, Rome$$uRome III U.
002255384 700__ $$aDi Nardo, Roberto$$iINSPIRE-00213420$$uCERN
002255384 700__ $$aDi Petrillo, Karri Folan$$iINSPIRE-00534580$$uHarvard U., Phys. Dept.
002255384 700__ $$aDi Simone, Andrea$$iINSPIRE-00213431$$uFreiburg U.
002255384 700__ $$aDi Sipio, Riccardo$$iINSPIRE-00213443$$uToronto U.
002255384 700__ $$aDi Valentino, David$$iINSPIRE-00352611$$uCarleton U.
002255384 700__ $$aDiaconu, Cristinel$$iINSPIRE-00184938$$uMarseille, CPPM
002255384 700__ $$aDiamond, Miriam$$iINSPIRE-00389950$$uToronto U.
002255384 700__ $$aDias, Flavia$$iINSPIRE-00176100$$uEdinburgh U.
002255384 700__ $$aDiaz, Marco Aurelio$$iINSPIRE-00077083$$uChile U., Catolica
002255384 700__ $$aDiehl, Edward$$iINSPIRE-00213467$$uMichigan U.
002255384 700__ $$aDietrich, Janet$$iINSPIRE-00213479$$uHumboldt U., Berlin
002255384 700__ $$aDíez Cornell, Sergio$$iINSPIRE-00474514$$uDESY
002255384 700__ $$aDimitrievska, Aleksandra$$iINSPIRE-00358147$$uBelgrade U.
002255384 700__ $$aDingfelder, Jochen$$iINSPIRE-00049343$$uBonn U.
002255384 700__ $$aDita, Petre$$iINSPIRE-00213503$$uBucharest, IFIN-HH
002255384 700__ $$aDita, Sanda$$iINSPIRE-00306991$$uBucharest, IFIN-HH
002255384 700__ $$aDittus, Fridolin$$iINSPIRE-00077326$$uCERN
002255384 700__ $$aDjama, Fares$$iINSPIRE-00077370$$uMarseille, CPPM
002255384 700__ $$aDjobava, Tamar$$iINSPIRE-00213527$$uTbilisi State U.
002255384 700__ $$aDjuvsland, Julia Isabell$$iINSPIRE-00338727$$uKirchhoff Inst. Phys.
002255384 700__ $$aBarros do Vale, Maria Aline$$iINSPIRE-00213539$$uSao Joao del-Rei Fed. U.
002255384 700__ $$aDobos, Daniel$$iINSPIRE-00016406$$uCERN
002255384 700__ $$aDobre, Monica$$iINSPIRE-00184940$$uBucharest, IFIN-HH
002255384 700__ $$aDoglioni, Caterina$$iINSPIRE-00213578$$uLund U.
002255384 700__ $$aDolejsi, Jiri$$iINSPIRE-00077599$$uCharles U.
002255384 700__ $$aDolezal, Zdenek$$iINSPIRE-00077602$$uCharles U.
002255384 700__ $$aDonadelli, Marisilvia$$iINSPIRE-00241441$$uSao Paulo U.
002255384 700__ $$aDonati, Simone$$iINSPIRE-00041275$$uINFN, Pisa$$uPisa U.
002255384 700__ $$aDondero, Paolo$$iINSPIRE-00352917$$uINFN, Pavia$$uPavia U.
002255384 700__ $$aDonini, Julien$$iINSPIRE-00041261$$uClermont-Ferrand U.
002255384 700__ $$aDopke, Jens$$iINSPIRE-00213647$$uRutherford
002255384 700__ $$aDoria, Alessandra$$iINSPIRE-00077860$$uINFN, Naples
002255384 700__ $$aDova, Maria-Teresa$$iINSPIRE-00077959$$uLa Plata U.
002255384 700__ $$aDoyle, Tony$$iINSPIRE-00078002$$uGlasgow U.
002255384 700__ $$aDrechsler, Eric$$iINSPIRE-00390060$$uGottingen U., II. Phys. Inst.
002255384 700__ $$aDris, Manolis$$iINSPIRE-00213672$$uNatl. Tech. U., Athens
002255384 700__ $$aDu, Yanyan$$iINSPIRE-00433072$$uShandong U.
002255384 700__ $$aDuarte-Campderros, Jorge$$iINSPIRE-00308625$$uTel Aviv U.
002255384 700__ $$aDuchovni, Ehud$$iINSPIRE-00152081$$uWeizmann Inst.
002255384 700__ $$aDuckeck, Guenter$$iINSPIRE-00213690$$uMunich U.
002255384 700__ $$aDucu, Otilia Anamaria$$iINSPIRE-00349755$$uMontreal U.$$uBucharest, IFIN-HH
002255384 700__ $$aDuda, Dominik$$iINSPIRE-00291889$$uFOM, Amsterdam
002255384 700__ $$aDudarev, Alexey$$iINSPIRE-00213702$$uCERN
002255384 700__ $$aDudder, Andreas Christian$$iINSPIRE-00518600$$uMainz U.
002255384 700__ $$aDuffield, Emily Marie$$iINSPIRE-00506863$$uLBL, Berkeley
002255384 700__ $$aDuflot, Laurent$$iINSPIRE-00078379$$uOrsay, LAL
002255384 700__ $$aDührssen, Michael$$iINSPIRE-00213726$$uCERN
002255384 700__ $$aDumancic, Mirta$$iINSPIRE-00441682$$uWeizmann Inst.
002255384 700__ $$aDumitriu, Ana Elena$$iINSPIRE-00540528$$uBucharest, IFIN-HH
002255384 700__ $$aDuncan, Anna Kathryn$$iINSPIRE-00534608$$uGlasgow U.
002255384 700__ $$aDunford, Monica$$iINSPIRE-00029703$$uKirchhoff Inst. Phys.
002255384 700__ $$aDuran Yildiz, Hatice$$iINSPIRE-00213740$$uAnkara U.
002255384 700__ $$aDüren, Michael$$iINSPIRE-00078621$$uGiessen U.
002255384 700__ $$aDurglishvili, Archil$$iINSPIRE-00362063$$uTbilisi State U.
002255384 700__ $$aDuschinger, Dirk$$iINSPIRE-00384038$$uDresden, Tech. U.
002255384 700__ $$aDutta, Baishali$$iINSPIRE-00431294$$uDESY
002255384 700__ $$aDyndal, Mateusz$$iINSPIRE-00359621$$uDESY
002255384 700__ $$aEckardt, Christoph$$iINSPIRE-00397250$$uDESY
002255384 700__ $$aEcker, Katharina Maria$$iINSPIRE-00387516$$uMunich, Max Planck Inst.
002255384 700__ $$aEdgar, Ryan Christopher$$iINSPIRE-00265484$$uMichigan U.
002255384 700__ $$aEifert, Till$$iINSPIRE-00305775$$uCERN
002255384 700__ $$aEigen, Gerald$$iINSPIRE-00079187$$uBergen U.
002255384 700__ $$aEinsweiler, Kevin$$iINSPIRE-00213832$$uLBL, Berkeley
002255384 700__ $$aEkelof, Tord$$iINSPIRE-00079263$$uUppsala U., Inst. Theor. Phys.
002255384 700__ $$aEl Kacimi, Mohamed$$iINSPIRE-00213844$$uCadi Ayyad U., Marrakech
002255384 700__ $$aEllajosyula, Venugopal$$iINSPIRE-00438789$$uMarseille, CPPM
002255384 700__ $$aEllert, Mattias$$iINSPIRE-00079322$$uUppsala U., Inst. Theor. Phys.
002255384 700__ $$aElles, Sabine$$iINSPIRE-00213856$$uAnnecy, LAPP
002255384 700__ $$aEllinghaus, Frank$$iINSPIRE-00241510$$uWuppertal U.
002255384 700__ $$aElliot, Alison$$iINSPIRE-00379232$$uVictoria U.
002255384 700__ $$aEllis, Nicolas$$iINSPIRE-00079357$$uCERN
002255384 700__ $$aElmsheuser, Johannes$$iINSPIRE-00039089$$uBrookhaven
002255384 700__ $$aElsing, Markus$$iINSPIRE-00213874$$uCERN
002255384 700__ $$aEmeliyanov, Dmitry$$iINSPIRE-00213886$$uRutherford
002255384 700__ $$aEnari, Yuji$$iINSPIRE-00079531$$uTokyo U., ICEPP
002255384 700__ $$aEndner, Oliver Chris$$iINSPIRE-00338702$$uMainz U.
002255384 700__ $$aEnnis, Joseph Stanford$$iINSPIRE-00524680$$uWarwick U.
002255384 700__ $$aErdmann, Johannes$$iINSPIRE-00213911$$uDortmund U.
002255384 700__ $$aEreditato, Antonio$$iINSPIRE-00079760$$uBern U., LHEP
002255384 700__ $$aErnis, Gunar$$iINSPIRE-00345588$$uWuppertal U.
002255384 700__ $$aErnst, Michael$$iINSPIRE-00213947$$uBrookhaven
002255384 700__ $$aErrede, Steven$$iINSPIRE-00079889$$uIllinois U., Urbana
002255384 700__ $$aErtel, Eugen$$iINSPIRE-00213960$$uMainz U.
002255384 700__ $$aEscalier, Marc$$iINSPIRE-00025013$$uOrsay, LAL
002255384 700__ $$aEsch, Hendrik$$iINSPIRE-00288596$$uDortmund U.
002255384 700__ $$aEscobar, Carlos$$iINSPIRE-00213977$$uPittsburgh U.
002255384 700__ $$aEsposito, Bellisario$$iINSPIRE-00213990$$uFrascati
002255384 700__ $$aEtienvre, Anne-Isabelle$$iINSPIRE-00240439$$uIRFU, Saclay
002255384 700__ $$aEtzion, Erez$$iINSPIRE-00080055$$uTel Aviv U.
002255384 700__ $$aEvans, Hal$$iINSPIRE-00080060$$uIndiana U.
002255384 700__ $$aEzhilov, Alexey$$iINSPIRE-00367680$$uSt. Petersburg, INP
002255384 700__ $$aFabbri, Federica$$iINSPIRE-00445370$$uINFN, Bologna$$uBologna U.
002255384 700__ $$aFabbri, Laura$$iINSPIRE-00283861$$uINFN, Bologna$$uBologna U.
002255384 700__ $$aFacini, Gabriel$$iINSPIRE-00019223$$uChicago U., EFI
002255384 700__ $$aFakhrutdinov, Rinat$$iINSPIRE-00214014$$uSerpukhov, IHEP
002255384 700__ $$aFalciano, Speranza$$iINSPIRE-00214026$$uINFN, Rome
002255384 700__ $$aFalla, Rebecca Jane$$iINSPIRE-00368475$$uUniversity Coll. London
002255384 700__ $$aFaltova, Jana$$iINSPIRE-00221190$$uCERN
002255384 700__ $$aFang, Yaquan$$iINSPIRE-00214038$$uBeijing, Inst. High Energy Phys.
002255384 700__ $$aFanti, Marcello$$iINSPIRE-00214040$$uINFN, Milan$$uMilan U.
002255384 700__ $$aFarbin, Amir$$iINSPIRE-00214051$$uTexas U., Arlington
002255384 700__ $$aFarilla, Addolorata$$iINSPIRE-00214063$$uINFN, Rome
002255384 700__ $$aFarina, Christian$$iINSPIRE-00438945$$uPittsburgh U.
002255384 700__ $$aFarina, Edoardo Maria$$iINSPIRE-00508881$$uINFN, Pavia$$uPavia U.
002255384 700__ $$aFarooque, Trisha$$iINSPIRE-00013478$$uMichigan State U.
002255384 700__ $$aFarrell, Steven$$iINSPIRE-00014247$$uLBL, Berkeley
002255384 700__ $$aFarrington, Sinead$$iINSPIRE-00060080$$uWarwick U.
002255384 700__ $$aFarthouat, Philippe$$iINSPIRE-00080462$$uCERN
002255384 700__ $$aFassi, Farida$$iINSPIRE-00308854$$uMohammed V U., Agdal
002255384 700__ $$aFassnacht, Patrick$$iINSPIRE-00080473$$uCERN
002255384 700__ $$aFassouliotis, Dimitrios$$iINSPIRE-00214081$$uAthens U.
002255384 700__ $$aFaucci Giannelli, Michele$$iINSPIRE-00352701$$uRoyal Holloway, U. of London
002255384 700__ $$aFavareto, Andrea$$iINSPIRE-00286492$$uINFN, Genoa$$uGenoa U.
002255384 700__ $$aFawcett, William James$$iINSPIRE-00389502$$uOxford U.
002255384 700__ $$aFayard, Louis$$iINSPIRE-00143071$$uOrsay, LAL
002255384 700__ $$aFedin, Oleg$$iINSPIRE-00305797$$uSt. Petersburg, INP$$uSt. Petersburg Polytechnic Inst.
002255384 700__ $$aFedorko, Wojciech$$iINSPIRE-00041224$$uBritish Columbia U.
002255384 700__ $$aFeigl, Simon$$iINSPIRE-00356540$$uOslo U.
002255384 700__ $$aFeligioni, Lorenzo$$iINSPIRE-00039073$$uMarseille, CPPM
002255384 700__ $$aFeng, Cunfeng$$iINSPIRE-00214142$$uShandong U.
002255384 700__ $$aFeng, Eric$$iINSPIRE-00214154$$uCERN
002255384 700__ $$aFeng, Haolu$$iINSPIRE-00332900$$uMichigan U.
002255384 700__ $$aFenyuk, Alexander$$iINSPIRE-00214166$$uSerpukhov, IHEP
002255384 700__ $$aFeremenga, Last$$iINSPIRE-00228200$$uTexas U., Arlington
002255384 700__ $$aFernandez Martinez, Patricia$$iINSPIRE-00366613$$uValencia U., IFIC
002255384 700__ $$aFernandez Perez, Sonia$$iINSPIRE-00356553$$uBarcelona, IFAE
002255384 700__ $$aFerrando, James$$iINSPIRE-00027519$$uDESY
002255384 700__ $$aFerrari, Arnaud$$iINSPIRE-00300636$$uUppsala U., Inst. Theor. Phys.
002255384 700__ $$aFerrari, Pamela$$iINSPIRE-00214210$$uFOM, Amsterdam
002255384 700__ $$aFerrari, Roberto$$iINSPIRE-00214221$$uINFN, Pavia
002255384 700__ $$aFerreira de Lima, Danilo Enoque$$iINSPIRE-00286519$$uHeidelberg U.
002255384 700__ $$aFerrer, Antonio$$iINSPIRE-00080972$$uValencia U., IFIC
002255384 700__ $$aFerrere, Didier$$iINSPIRE-00188574$$uGeneva U.
002255384 700__ $$aFerretti, Claudio$$iINSPIRE-00028525$$uMichigan U.
002255384 700__ $$aFiedler, Frank$$iINSPIRE-00081065$$uMainz U.
002255384 700__ $$aFilipčič, Andrej$$iINSPIRE-00081160$$uStefan Inst., Ljubljana
002255384 700__ $$aFilipuzzi, Marco$$iINSPIRE-00342629$$uDESY
002255384 700__ $$aFilthaut, Frank$$iINSPIRE-00081209$$uNIKHEF, Amsterdam
002255384 700__ $$aFincke-Keeler, Margret$$iINSPIRE-00081234$$uVictoria U.
002255384 700__ $$aFinelli, Kevin Daniel$$iINSPIRE-00337620$$uSydney U.
002255384 700__ $$aFiolhais, Miguel$$iINSPIRE-00214269$$uLIP, Lisbon$$uCoimbra U.$$uBMCC, New York
002255384 700__ $$aFiorini, Luca$$iINSPIRE-00214275$$uValencia U., IFIC
002255384 700__ $$aFischer, Adam$$iINSPIRE-00376085$$uSUNY, Albany
002255384 700__ $$aFischer, Cora$$iINSPIRE-00387867$$uBarcelona, IFAE
002255384 700__ $$aFischer, Julia$$iINSPIRE-00336608$$uWuppertal U.
002255384 700__ $$aFisher, Wade Cameron$$iINSPIRE-00052479$$uMichigan State U.
002255384 700__ $$aFlaschel, Nils$$iINSPIRE-00371327$$uDESY
002255384 700__ $$aFleck, Ivor$$iINSPIRE-00081605$$uSiegen U.
002255384 700__ $$aFleischmann, Philipp$$iINSPIRE-00214324$$uMichigan U.
002255384 700__ $$aFletcher, Rob Roy MacGregor$$iINSPIRE-00405355$$uPennsylvania U.
002255384 700__ $$aFlick, Tobias$$iINSPIRE-00214348$$uWuppertal U.
002255384 700__ $$aFlierl, Bernhard Matthias$$iINSPIRE-00542102$$uMunich U.
002255384 700__ $$aFlores Castillo, Luis$$iINSPIRE-00041212$$uHong Kong, Chinese U.
002255384 700__ $$aFlowerdew, Michael$$iINSPIRE-00214350$$uMunich, Max Planck Inst.
002255384 700__ $$aForcolin, Giulio Tiziano$$iINSPIRE-00406118$$uManchester U.
002255384 700__ $$aFormica, Andrea$$iINSPIRE-00081940$$uIRFU, Saclay
002255384 700__ $$aForti, Alessandra$$iINSPIRE-00027700$$uManchester U.
002255384 700__ $$aFoster, Andrew Geoffrey$$iINSPIRE-00445427$$uBirmingham U.
002255384 700__ $$aFournier, Daniel$$iINSPIRE-00144690$$uOrsay, LAL
002255384 700__ $$aFox, Harald$$iINSPIRE-00082068$$uLancaster U.
002255384 700__ $$aFracchia, Silvia$$iINSPIRE-00361393$$uBarcelona, IFAE
002255384 700__ $$aFrancavilla, Paolo$$iINSPIRE-00305814$$uParis U., VI-VII
002255384 700__ $$aFranchini, Matteo$$iINSPIRE-00293056$$uINFN, Bologna$$uBologna U.
002255384 700__ $$aFrancis, David$$iINSPIRE-00214393$$uCERN
002255384 700__ $$aFranconi, Laura$$iINSPIRE-00371528$$uOslo U.
002255384 700__ $$aFranklin, Melissa$$iINSPIRE-00082230$$uHarvard U., Phys. Dept.
002255384 700__ $$aFrate, Meghan$$iINSPIRE-00408123$$uUC, Irvine
002255384 700__ $$aFraternali, Marco$$iINSPIRE-00214419$$uINFN, Pavia$$uPavia U.
002255384 700__ $$aFreeborn, David$$iINSPIRE-00365510$$uUniversity Coll. London
002255384 700__ $$aFressard-Batraneanu, Silvia$$iINSPIRE-00389614$$uCERN
002255384 700__ $$aFreund, Benjamin$$iINSPIRE-00506444$$uMontreal U.
002255384 700__ $$aFroidevaux, Daniel$$iINSPIRE-00082670$$uCERN
002255384 700__ $$aFrost, James$$iINSPIRE-00171541$$uOxford U.
002255384 700__ $$aFukunaga, Chikara$$iINSPIRE-00214432$$uTokyo Metropolitan U.
002255384 700__ $$aFullana Torregrosa, Esteban$$iINSPIRE-00002800$$uMainz U.
002255384 700__ $$aFusayasu, Takahiro$$iINSPIRE-00241597$$uNagasaki Inst. Appl. Sci.
002255384 700__ $$aFuster, Juan$$iINSPIRE-00214444$$uValencia U., IFIC
002255384 700__ $$aGabaldon, Carolina$$iINSPIRE-00214457$$uLPSC, Grenoble
002255384 700__ $$aGabizon, Ofir$$iINSPIRE-00214469$$uTechnion
002255384 700__ $$aGabrielli, Alessandro$$iINSPIRE-00342638$$uINFN, Bologna$$uBologna U.
002255384 700__ $$aGabrielli, Andrea$$iINSPIRE-00339066$$uLBL, Berkeley
002255384 700__ $$aGach, Grzegorz$$iINSPIRE-00184415$$uAGH-UST, Cracow
002255384 700__ $$aGadatsch, Stefan$$iINSPIRE-00342641$$uCERN
002255384 700__ $$aGadomski, Szymon$$iINSPIRE-00083092$$uRoyal Holloway, U. of London
002255384 700__ $$aGagliardi, Guido$$iINSPIRE-00214470$$uINFN, Genoa$$uGenoa U.
002255384 700__ $$aGagnon, Louis Guillaume$$iINSPIRE-00441787$$uMontreal U.
002255384 700__ $$aGagnon, Pauline$$iINSPIRE-00083104$$uIndiana U.
002255384 700__ $$aGalea, Cristina$$iINSPIRE-00039048$$uNIKHEF, Amsterdam
002255384 700__ $$aGalhardo, Bruno$$iINSPIRE-00291919$$uLIP, Lisbon$$uCoimbra U.
002255384 700__ $$aGallas, Elizabeth$$iINSPIRE-00083337$$uOxford U.
002255384 700__ $$aGallop, Bruce$$iINSPIRE-00214494$$uRutherford
002255384 700__ $$aGallus, Petr$$iINSPIRE-00015179$$uPrague, Tech. U.
002255384 700__ $$aGalster, Gorm Aske Gram Krohn$$iINSPIRE-00353273$$uBohr Inst.
002255384 700__ $$aGan, KK$$iINSPIRE-00083439$$uOhio State U.
002255384 700__ $$aGanguly, Sanmay$$iINSPIRE-00225996$$uClermont-Ferrand U.
002255384 700__ $$aGao, Jun$$iINSPIRE-00349762$$uHefei, CUST
002255384 700__ $$aGao, Yanyan$$iINSPIRE-00145255$$uLiverpool U.
002255384 700__ $$aGao, Yongsheng$$iINSPIRE-00083520$$uSLAC$$uFresno State
002255384 700__ $$aGaray Walls, Francisca$$iINSPIRE-00336691$$uEdinburgh U.
002255384 700__ $$aGarcía, Carmen$$iINSPIRE-00214518$$uValencia U., IFIC
002255384 700__ $$aGarcía Navarro, José Enrique$$iINSPIRE-00022084$$uValencia U., IFIC
002255384 700__ $$aGarcia-Sciveres, Maurice$$iINSPIRE-00083629$$uLBL, Berkeley
002255384 700__ $$aGardner, Robert$$iINSPIRE-00083694$$uChicago U., EFI
002255384 700__ $$aGarelli, Nicoletta$$iINSPIRE-00214520$$uSLAC
002255384 700__ $$aGaronne, Vincent$$iINSPIRE-00214543$$uOslo U.
002255384 700__ $$aGascon Bravo, Alberto$$iINSPIRE-00212894$$uDESY
002255384 700__ $$aGasnikova, Ksenia$$iINSPIRE-00425340$$uDESY
002255384 700__ $$aGatti, Claudio$$iINSPIRE-00214550$$uFrascati
002255384 700__ $$aGaudiello, Andrea$$iINSPIRE-00399154$$uINFN, Genoa$$uGenoa U.
002255384 700__ $$aGaudio, Gabriella$$iINSPIRE-00214561$$uINFN, Pavia
002255384 700__ $$aGavrilenko, Igor$$iINSPIRE-00214609$$uLebedev Inst.
002255384 700__ $$aGay, Colin$$iINSPIRE-00214610$$uBritish Columbia U.
002255384 700__ $$aGaycken, Goetz$$iINSPIRE-00214622$$uBonn U.
002255384 700__ $$aGazis, Evangelos$$iINSPIRE-00084094$$uNatl. Tech. U., Athens
002255384 700__ $$aGee, Norman$$iINSPIRE-00214646$$uRutherford
002255384 700__ $$aGeisen, Marc$$iINSPIRE-00443406$$uMainz U.
002255384 700__ $$aGeisler, Manuel Patrice$$iINSPIRE-00399680$$uKirchhoff Inst. Phys.
002255384 700__ $$aGellerstedt, Karl$$iINSPIRE-00214664$$uStockholm U.$$uStockholm U., OKC
002255384 700__ $$aGemme, Claudia$$iINSPIRE-00214676$$uINFN, Genoa
002255384 700__ $$aGenest, Marie-Hélène$$iINSPIRE-00016112$$uLPSC, Grenoble
002255384 700__ $$aGeng, Cong$$iINSPIRE-00423506$$uHefei, CUST$$uMichigan U.
002255384 700__ $$aGentile, Simonetta$$iINSPIRE-00214688$$uINFN, Rome$$uRome U.
002255384 700__ $$aGentsos, Christos$$iINSPIRE-00380612$$uAristotle U., Thessaloniki
002255384 700__ $$aGeorge, Simon$$iINSPIRE-00084316$$uRoyal Holloway, U. of London
002255384 700__ $$aGerbaudo, Davide$$iINSPIRE-00047907$$uBarcelona, IFAE
002255384 700__ $$aGershon, Avi$$iINSPIRE-00214690$$uTel Aviv U.
002255384 700__ $$aGhasemi, Sara$$iINSPIRE-00409400$$uSiegen U.
002255384 700__ $$aGhneimat, Mazuza$$iINSPIRE-00443494$$uBonn U.
002255384 700__ $$aGiacobbe, Benedetto$$iINSPIRE-00214725$$uINFN, Bologna
002255384 700__ $$aGiagu, Stefano$$iINSPIRE-00084627$$uINFN, Rome$$uRome U.
002255384 700__ $$aGiannetti, Paola$$iINSPIRE-00003904$$uINFN, Pisa$$uPisa U.
002255384 700__ $$aGibson, Stephen$$iINSPIRE-00214737$$uRoyal Holloway, U. of London
002255384 700__ $$aGignac, Matthew$$iINSPIRE-00425540$$uBritish Columbia U.
002255384 700__ $$aGilchriese, Murdock$$iINSPIRE-00084816$$uLBL, Berkeley
002255384 700__ $$aGillberg, Dag$$iINSPIRE-00006756$$uCarleton U.
002255384 700__ $$aGilles, Geoffrey$$iINSPIRE-00364250$$uWuppertal U.
002255384 700__ $$aGingrich, Douglas$$iINSPIRE-00084876$$uAlberta U.$$uTRIUMF
002255384 700__ $$aGiokaris, Nikos$$iINSPIRE-00084938$$uAthens U.
002255384 700__ $$aGiordani, MarioPaolo$$iINSPIRE-00084948$$uINFN, Udine$$uUdine U.
002255384 700__ $$aGiorgi, Filippo Maria$$iINSPIRE-00214779$$uINFN, Bologna
002255384 700__ $$aGiraud, Pierre-Francois$$iINSPIRE-00214780$$uIRFU, Saclay
002255384 700__ $$aGiromini, Paolo$$iINSPIRE-00085050$$uHarvard U., Phys. Dept.
002255384 700__ $$aGiugni, Danilo$$iINSPIRE-00214804$$uINFN, Milan
002255384 700__ $$aGiuli, Francesco$$iINSPIRE-00544699$$uOxford U.
002255384 700__ $$aGiuliani, Claudia$$iINSPIRE-00339743$$uMunich, Max Planck Inst.
002255384 700__ $$aGiulini, Maddalena$$iINSPIRE-00362075$$uHeidelberg U.
002255384 700__ $$aGjelsten, Børge Kile$$iINSPIRE-00214821$$uOslo U.
002255384 700__ $$aGkaitatzis, Stamatios$$iINSPIRE-00372074$$uAristotle U., Thessaloniki
002255384 700__ $$aGkialas, Ioannis$$iINSPIRE-00236266$$uAthens U.
002255384 700__ $$aGkougkousis, Evangelos Leonidas$$iINSPIRE-00380163$$uUC, Santa Cruz
002255384 700__ $$aGladilin, Leonid$$iINSPIRE-00173602$$uMoscow State U.
002255384 700__ $$aGlasman, Claudia$$iINSPIRE-00173488$$uMadrid, Autonoma U.
002255384 700__ $$aGlatzer, Julian$$iINSPIRE-00013837$$uBarcelona, IFAE
002255384 700__ $$aGlaysher, Paul$$iINSPIRE-00359633$$uDESY
002255384 700__ $$aGlazov, Alexandre$$iINSPIRE-00326794$$uDESY
002255384 700__ $$aGoblirsch-Kolb, Maximilian$$iINSPIRE-00339087$$uBrandeis U.
002255384 700__ $$aGodlewski, Jan$$iINSPIRE-00214851$$uCracow, INP
002255384 700__ $$aGoldfarb, Steven$$iINSPIRE-00085461$$uMelbourne U.
002255384 700__ $$aGolling, Tobias$$iINSPIRE-00085610$$uGeneva U.
002255384 700__ $$aGolubkov, Dmitry$$iINSPIRE-00260751$$uSerpukhov, IHEP
002255384 700__ $$aGomes, Agostinho$$iINSPIRE-00226662$$uLIP, Lisbon$$uLisbon U., CFNUL
002255384 700__ $$aGonçalo, Ricardo$$iINSPIRE-00171282$$uLIP, Lisbon
002255384 700__ $$aGoncalves Gama, Rafael$$iINSPIRE-00377697$$uRio de Janeiro Federal U.
002255384 700__ $$aGoncalves Pinto Firmino Da Costa, Joao$$iINSPIRE-00238024$$uIRFU, Saclay
002255384 700__ $$aGonella, Giulia$$iINSPIRE-00508891$$uFreiburg U.
002255384 700__ $$aGonella, Laura$$iINSPIRE-00001730$$uBirmingham U.
002255384 700__ $$aGongadze, Alexi$$iINSPIRE-00439573$$uDubna, JINR
002255384 700__ $$aGonzález de la Hoz, Santiago$$iINSPIRE-00214978$$uValencia U., IFIC
002255384 700__ $$aGonzalez-Sevilla, Sergio$$iINSPIRE-00214993$$uGeneva U.
002255384 700__ $$aGoossens, Luc$$iINSPIRE-00215005$$uCERN
002255384 700__ $$aGorbounov, Petr Andreevich$$iINSPIRE-00085929$$uMoscow, ITEP
002255384 700__ $$aGordon, Howard$$iINSPIRE-00085936$$uBrookhaven
002255384 700__ $$aGorelov, Igor$$iINSPIRE-00048110$$uNew Mexico U.
002255384 700__ $$aGorini, Benedetto$$iINSPIRE-00215017$$uCERN
002255384 700__ $$aGorini, Edoardo$$iINSPIRE-00085978$$uINFN, Lecce$$uSalento U.
002255384 700__ $$aGorišek, Andrej$$iINSPIRE-00215023$$uStefan Inst., Ljubljana
002255384 700__ $$aGoshaw, Alfred$$iINSPIRE-00086006$$uDuke U.
002255384 700__ $$aGössling, Claus$$iINSPIRE-00189086$$uDortmund U.
002255384 700__ $$aGostkin, Mikhail Ivanovitch$$iINSPIRE-00215072$$uDubna, JINR
002255384 700__ $$aGoudet, Christophe Raymond$$iINSPIRE-00436282$$uOrsay, LAL
002255384 700__ $$aGoujdami, Driss$$iINSPIRE-00215096$$uCadi Ayyad U., Marrakech
002255384 700__ $$aGoussiou, Anna$$iINSPIRE-00086179$$uWashington U., Seattle
002255384 700__ $$aGovender, Nicolin$$iINSPIRE-00335913$$uJohannesburg U.$$uCHPC, Cape Town
002255384 700__ $$aGozani, Eitan$$iINSPIRE-00423098$$uTechnion
002255384 700__ $$aGraber, Lars$$iINSPIRE-00336619$$uGottingen U., II. Phys. Inst.
002255384 700__ $$aGrabowska-Bold, Iwona$$iINSPIRE-00172493$$uAGH-UST, Cracow
002255384 700__ $$aGradin, Per Olov Joakim$$iINSPIRE-00413032$$uLPSC, Grenoble
002255384 700__ $$aGramling, Johanna$$iINSPIRE-00245767$$uGeneva U.
002255384 700__ $$aGramstad, Eirik$$iINSPIRE-00328259$$uOslo U.
002255384 700__ $$aGrancagnolo, Sergio$$iINSPIRE-00041686$$uHumboldt U., Berlin
002255384 700__ $$aGratchev, Vadim$$iINSPIRE-00215138$$uSt. Petersburg, INP
002255384 700__ $$aGravila, Paul Mircea$$iINSPIRE-00443594$$uWest Timisoara U.
002255384 700__ $$aGray, Heather$$iINSPIRE-00032771$$uCERN
002255384 700__ $$aGreenwood, Zeno Dixon$$iINSPIRE-00086666$$uLouisiana Tech. U.
002255384 700__ $$aGrefe, Christian$$iINSPIRE-00166555$$uBonn U.
002255384 700__ $$aGregersen, Kristian$$iINSPIRE-00236292$$uUniversity Coll. London
002255384 700__ $$aGregor, Ingrid-Maria$$iINSPIRE-00086670$$uDESY
002255384 700__ $$aGrenier, Philippe$$iINSPIRE-00050339$$uSLAC
002255384 700__ $$aGrevtsov, Kirill$$iINSPIRE-00436367$$uAnnecy, LAPP
002255384 700__ $$aGriffiths, Justin$$iINSPIRE-00036544$$uTexas U., Arlington
002255384 700__ $$aGrillo, Alexander$$iINSPIRE-00086795$$uUC, Santa Cruz
002255384 700__ $$aGrimm, Kathryn$$iINSPIRE-00301388$$uLancaster U.
002255384 700__ $$aGrinstein, Sebastian$$iINSPIRE-00086810$$uBarcelona, IFAE$$uICREA, Barcelona
002255384 700__ $$aGris, Philippe Luc Yves$$iINSPIRE-00086824$$uClermont-Ferrand U.
002255384 700__ $$aGrivaz, Jean-Francois$$iINSPIRE-00086861$$uOrsay, LAL
002255384 700__ $$aGroh, Sabrina$$iINSPIRE-00381611$$uMainz U.
002255384 700__ $$aGross, Eilam$$iINSPIRE-00086983$$uWeizmann Inst.
002255384 700__ $$aGrosse-Knetter, Joern$$iINSPIRE-00087004$$uGottingen U., II. Phys. Inst.
002255384 700__ $$aGrossi, Giulio Cornelio$$iINSPIRE-00349774$$uLouisiana Tech. U.
002255384 700__ $$aGrout, Zara Jane$$iINSPIRE-00346926$$uUniversity Coll. London
002255384 700__ $$aGuan, Liang$$iINSPIRE-00361789$$uMichigan U.
002255384 700__ $$aGuan, Wen$$iINSPIRE-00011690$$uWisconsin U., Madison
002255384 700__ $$aGuenther, Jaroslav$$iINSPIRE-00215268$$uInnsbruck U.
002255384 700__ $$aGuescini, Francesco$$iINSPIRE-00339090$$uTRIUMF
002255384 700__ $$aGuest, Daniel$$iINSPIRE-00236307$$uUC, Irvine
002255384 700__ $$aGueta, Orel$$iINSPIRE-00227648$$uTel Aviv U.
002255384 700__ $$aGui, Bin$$iINSPIRE-00262919$$uOhio State U.
002255384 700__ $$aGuido, Elisa$$iINSPIRE-00144592$$uINFN, Genoa$$uGenoa U.
002255384 700__ $$aGuillemin, Thibault$$iINSPIRE-00180576$$uAnnecy, LAPP
002255384 700__ $$aGuindon, Stefan$$iINSPIRE-00230412$$uSUNY, Albany
002255384 700__ $$aGul, Umar$$iINSPIRE-00160612$$uGlasgow U.
002255384 700__ $$aGumpert, Christian$$iINSPIRE-00349786$$uCERN
002255384 700__ $$aGuo, Jun$$iINSPIRE-00047393$$uShanghai Jiao Tong U.
002255384 700__ $$aGuo, Wen$$iINSPIRE-00533031$$uMichigan U.
002255384 700__ $$aGuo, Yicheng$$iINSPIRE-00407534$$uHefei, CUST
002255384 700__ $$aGupta, Ruchi$$iINSPIRE-00204451$$uSouthern Methodist U.
002255384 700__ $$aGupta, Shaun$$iINSPIRE-00337636$$uOxford U.
002255384 700__ $$aGustavino, Giuliano$$iINSPIRE-00394284$$uINFN, Rome$$uRome U.
002255384 700__ $$aGutierrez, Phillip$$iINSPIRE-00087527$$uOklahoma U.
002255384 700__ $$aGutierrez Ortiz, Nicolas Gilberto$$iINSPIRE-00245190$$uUniversity Coll. London
002255384 700__ $$aGutschow, Christian$$iINSPIRE-00346139$$uUniversity Coll. London
002255384 700__ $$aGuyot, Claude$$iINSPIRE-00087556$$uIRFU, Saclay
002255384 700__ $$aGuzik, Marcin Pawel$$iINSPIRE-00337935$$uAGH-UST, Cracow
002255384 700__ $$aGwenlan, Claire$$iINSPIRE-00173806$$uOxford U.
002255384 700__ $$aGwilliam, Carl$$iINSPIRE-00215301$$uLiverpool U.
002255384 700__ $$aHaas, Andy$$iINSPIRE-00053405$$uNew York U.
002255384 700__ $$aHaber, Carl$$iINSPIRE-00087660$$uLBL, Berkeley
002255384 700__ $$aHadavand, Haleh Khani$$iINSPIRE-00042933$$uTexas U., Arlington
002255384 700__ $$aHadef, Asma$$iINSPIRE-00439100$$uMarseille, CPPM
002255384 700__ $$aHageböck, Stephan$$iINSPIRE-00346932$$uBonn U.
002255384 700__ $$aHagihara, Mutsuto$$iINSPIRE-00524693$$uTsukuba U.
002255384 700__ $$aHakobyan, Hrachya$$iINSPIRE-00215325$$uYerevan Phys. Inst.
002255384 700__ $$aHaleem, Mahsana$$iINSPIRE-00039197$$uDESY
002255384 700__ $$aHaley, Joseph$$iINSPIRE-00006781$$uOklahoma State U.
002255384 700__ $$aHalladjian, Garabed$$iINSPIRE-00334418$$uMichigan State U.
002255384 700__ $$aHallewell, Gregory David$$iINSPIRE-00088110$$uMarseille, CPPM
002255384 700__ $$aHamacher, Klaus$$iINSPIRE-00088237$$uWuppertal U.
002255384 700__ $$aHamal, Petr$$iINSPIRE-00286535$$uPalacky U.
002255384 700__ $$aHamano, Kenji$$iINSPIRE-00041649$$uVictoria U.
002255384 700__ $$aHamilton, Andrew$$iINSPIRE-00088319$$uCape Town U.
002255384 700__ $$aHamity, Guillermo Nicolas$$iINSPIRE-00375233$$uSheffield U.
002255384 700__ $$aHamnett, Phillip George$$iINSPIRE-00362099$$uDESY
002255384 700__ $$aHan, Liang$$iINSPIRE-00037384$$uHefei, CUST
002255384 700__ $$aHan, Shuo$$iINSPIRE-00530966$$uBeijing, Inst. High Energy Phys.
002255384 700__ $$aHanagaki, Kazunori$$iINSPIRE-00215349$$uKEK, Tsukuba$$uOsaka U.
002255384 700__ $$aHanawa, Keita$$iINSPIRE-00236320$$uTokyo U., ICEPP
002255384 700__ $$aHance, Michael$$iINSPIRE-00215350$$uUC, Santa Cruz
002255384 700__ $$aHaney, Bijan$$iINSPIRE-00403295$$uPennsylvania U.
002255384 700__ $$aHanke, Paul$$iINSPIRE-00088446$$uKirchhoff Inst. Phys.
002255384 700__ $$aHanna, Remie$$iINSPIRE-00362100$$uIRFU, Saclay
002255384 700__ $$aHansen, Jørgen Beck$$iINSPIRE-00215374$$uBohr Inst.
002255384 700__ $$aHansen, Jorn Dines$$iINSPIRE-00088500$$uBohr Inst.
002255384 700__ $$aHansen, Maike Christina$$iINSPIRE-00395987$$uBonn U.
002255384 700__ $$aHansen, Peter Henrik$$iINSPIRE-00215386$$uBohr Inst.
002255384 700__ $$aHara, Kazuhiko$$iINSPIRE-00300064$$uTsukuba U.
002255384 700__ $$aHard, Andrew$$iINSPIRE-00334429$$uWisconsin U., Madison
002255384 700__ $$aHarenberg, Torsten$$iINSPIRE-00215424$$uWuppertal U.
002255384 700__ $$aHariri, Faten$$iINSPIRE-00367006$$uOrsay, LAL
002255384 700__ $$aHarkusha, Siarhei$$iINSPIRE-00236332$$uMinsk, Inst. Phys.
002255384 700__ $$aHarrington, Robert$$iINSPIRE-00088743$$uEdinburgh U.
002255384 700__ $$aHarrison, Paul Fraser$$iINSPIRE-00088800$$uWarwick U.
002255384 700__ $$aHartjes, Fred$$iINSPIRE-00215450$$uFOM, Amsterdam
002255384 700__ $$aHartmann, Nikolai Marcel$$iINSPIRE-00452386$$uMunich U.
002255384 700__ $$aHasegawa, Makoto$$iINSPIRE-00376747$$uKobe U.
002255384 700__ $$aHasegawa, Yoji$$iINSPIRE-00089003$$uShinshu U.
002255384 700__ $$aHasib, Ahmed$$iINSPIRE-00359645$$uEdinburgh U.
002255384 700__ $$aHassani, Samira$$iINSPIRE-00215473$$uIRFU, Saclay
002255384 700__ $$aHaug, Sigve$$iINSPIRE-00215485$$uBern U., LHEP
002255384 700__ $$aHauser, Reiner$$iINSPIRE-00215503$$uMichigan State U.
002255384 700__ $$aHauswald, Lorenz$$iINSPIRE-00387053$$uDresden, Tech. U.
002255384 700__ $$aHavener, Laura Brittany$$iINSPIRE-00436609$$uNevis Labs, Columbia U.
002255384 700__ $$aHavranek, Miroslav$$iINSPIRE-00021242$$uPrague, Tech. U.
002255384 700__ $$aHawkes, Christopher$$iINSPIRE-00089196$$uBirmingham U.
002255384 700__ $$aHawkings, Richard John$$iINSPIRE-00148070$$uCERN
002255384 700__ $$aHayakawa, Daiki$$iINSPIRE-00514524$$uTokyo Inst. Tech.
002255384 700__ $$aHayden, Daniel$$iINSPIRE-00286543$$uMichigan State U.
002255384 700__ $$aHays, Chris$$iINSPIRE-00050513$$uOxford U.
002255384 700__ $$aHays, Jonathan Michael$$iINSPIRE-00005408$$uQueen Mary, U. of London
002255384 700__ $$aHayward, Helen$$iINSPIRE-00142771$$uLiverpool U.
002255384 700__ $$aHaywood, Stephen$$iINSPIRE-00089254$$uRutherford
002255384 700__ $$aHead, Simon$$iINSPIRE-00260677$$uBirmingham U.
002255384 700__ $$aHeck, Tobias$$iINSPIRE-00335580$$uMainz U.
002255384 700__ $$aHedberg, Vincent$$iINSPIRE-00215527$$uLund U.
002255384 700__ $$aHeelan, Louise$$iINSPIRE-00215539$$uTexas U., Arlington
002255384 700__ $$aHeidegger, Kim Katrin$$iINSPIRE-00224321$$uFreiburg U.
002255384 700__ $$aHeim, Sarah$$iINSPIRE-00215540$$uDESY
002255384 700__ $$aHeim, Timon$$iINSPIRE-00356268$$uLBL, Berkeley
002255384 700__ $$aHeinemann, Beate$$iINSPIRE-00089482$$uDESY$$uFreiburg U.
002255384 700__ $$aHeinrich, Jochen Jens$$iINSPIRE-00441872$$uMunich U.
002255384 700__ $$aHeinrich, Lukas$$iINSPIRE-00356271$$uNew York U.
002255384 700__ $$aHeinz, Christian$$iINSPIRE-00439219$$uGiessen U.
002255384 700__ $$aHejbal, Jiri$$iINSPIRE-00339101$$uPrague, Inst. Phys.
002255384 700__ $$aHelary, Louis$$iINSPIRE-00215564$$uCERN
002255384 700__ $$aHeld, Alexander$$iINSPIRE-00536620$$uBritish Columbia U.
002255384 700__ $$aHellman, Sten$$iINSPIRE-00089640$$uStockholm U.$$uStockholm U., OKC
002255384 700__ $$aHelsens, Clement$$iINSPIRE-00215588$$uCERN
002255384 700__ $$aHenderson, James$$iINSPIRE-00339118$$uOxford U.
002255384 700__ $$aHenderson, Robert$$iINSPIRE-00037338$$uLancaster U.
002255384 700__ $$aHeng, Yang$$iINSPIRE-00334432$$uWisconsin U., Madison
002255384 700__ $$aHenkelmann, Steffen$$iINSPIRE-00407415$$uBritish Columbia U.
002255384 700__ $$aHenriques Correia, Ana Maria$$iINSPIRE-00305891$$uCERN
002255384 700__ $$aHenrot-Versille, Sophie$$iINSPIRE-00089793$$uOrsay, LAL
002255384 700__ $$aHerbert, Geoffrey Henry$$iINSPIRE-00337055$$uHumboldt U., Berlin
002255384 700__ $$aHerde, Hannah$$iINSPIRE-00524702$$uBrandeis U.
002255384 700__ $$aHerget, Verena$$iINSPIRE-00524714$$uWurzburg U.
002255384 700__ $$aHernández Jiménez, Yesenia$$iINSPIRE-00215618$$uWitwatersrand U.
002255384 700__ $$aHerten, Gregor$$iINSPIRE-00089942$$uFreiburg U.
002255384 700__ $$aHertenberger, Ralf$$iINSPIRE-00215631$$uMunich U.
002255384 700__ $$aHervas, Luis$$iINSPIRE-00215643$$uCERN
002255384 700__ $$aHerwig, Theodor Christian$$iINSPIRE-00535667$$uPennsylvania U.
002255384 700__ $$aHesketh, Gavin Grant$$iINSPIRE-00054306$$uUniversity Coll. London
002255384 700__ $$aHessey, Nigel$$iINSPIRE-00090012$$uTRIUMF
002255384 700__ $$aHetherly, Jeffrey Wayne$$iINSPIRE-00392821$$uSouthern Methodist U.
002255384 700__ $$aHigashino, Satoshi$$iINSPIRE-00536635$$uKEK, Tsukuba
002255384 700__ $$aHigón-Rodriguez, Emilio$$iINSPIRE-00215655$$uValencia U., IFIC
002255384 700__ $$aHill, Ewan$$iINSPIRE-00345031$$uVictoria U.
002255384 700__ $$aHill, John$$iINSPIRE-00090279$$uCambridge U.
002255384 700__ $$aHiller, Karl Heinz$$iINSPIRE-00185199$$uDESY
002255384 700__ $$aHillier, Stephen$$iINSPIRE-00090318$$uBirmingham U.
002255384 700__ $$aHinchliffe, Ian$$iINSPIRE-00161746$$uLBL, Berkeley
002255384 700__ $$aHirose, Minoru$$iINSPIRE-00215710$$uFreiburg U.
002255384 700__ $$aHirschbuehl, Dominic$$iINSPIRE-00041134$$uWuppertal U.
002255384 700__ $$aHiti, Bojan$$iINSPIRE-00541780$$uStefan Inst., Ljubljana
002255384 700__ $$aHladik, Ondrej$$iINSPIRE-00512847$$uPrague, Inst. Phys.
002255384 700__ $$aHoad, Xanthe$$iINSPIRE-00441925$$uEdinburgh U.
002255384 700__ $$aHobbs, John$$iINSPIRE-00090491$$uSUNY, Stony Brook
002255384 700__ $$aHod, Noam$$iINSPIRE-00215734$$uTRIUMF
002255384 700__ $$aHodgkinson, Mark$$iINSPIRE-00030600$$uSheffield U.
002255384 700__ $$aHodgson, Paul$$iINSPIRE-00215746$$uSheffield U.
002255384 700__ $$aHoecker, Andreas$$iINSPIRE-00090516$$uCERN
002255384 700__ $$aHoeferkamp, Martin$$iINSPIRE-00021230$$uNew Mexico U.
002255384 700__ $$aHoenig, Friedrich$$iINSPIRE-00376466$$uMunich U.
002255384 700__ $$aHohn, David$$iINSPIRE-00392879$$uBonn U.
002255384 700__ $$aHolmes, Tova Ray$$iINSPIRE-00349798$$uLBL, Berkeley
002255384 700__ $$aHomann, Michael$$iINSPIRE-00381480$$uDortmund U.
002255384 700__ $$aHonda, Shunsuke$$iINSPIRE-00524723$$uTsukuba U.
002255384 700__ $$aHonda, Takuya$$iINSPIRE-00524733$$uKEK, Tsukuba
002255384 700__ $$aHong, Tae Min$$iINSPIRE-00042918$$uPittsburgh U.
002255384 700__ $$aHooberman, Benjamin Henry$$iINSPIRE-00017664$$uIllinois U., Urbana
002255384 700__ $$aHopkins, Walter$$iINSPIRE-00009068$$uOregon U.
002255384 700__ $$aHorii, Yasuyuki$$iINSPIRE-00370685$$uNagoya U.
002255384 700__ $$aHorton, Arthur James$$iINSPIRE-00376759$$uSimon Fraser U.
002255384 700__ $$aHostachy, Jean-Yves$$iINSPIRE-00215837$$uLPSC, Grenoble
002255384 700__ $$aHou, Suen$$iINSPIRE-00091198$$uTaiwan, Inst. Phys.
002255384 700__ $$aHoummada, Abdeslam$$iINSPIRE-00215849$$uCasablanca U.
002255384 700__ $$aHowarth, James$$iINSPIRE-00230643$$uDESY
002255384 700__ $$aHoya, Joaquin$$iINSPIRE-00517879$$uLa Plata U.
002255384 700__ $$aHrabovsky, Miroslav$$iINSPIRE-00334449$$uPalacky U.
002255384 700__ $$aHristova, Ivana$$iINSPIRE-00286578$$uHumboldt U., Berlin
002255384 700__ $$aHrivnac, Julius$$iINSPIRE-00215850$$uOrsay, LAL
002255384 700__ $$aHryn'ova, Tetiana$$iINSPIRE-00049739$$uAnnecy, LAPP
002255384 700__ $$aHrynevich, Aliaksei$$iINSPIRE-00383643$$uMinsk, High Energy Phys. Ctr.
002255384 700__ $$aHsu, Pai-hsien Jennifer$$iINSPIRE-00036505$$uTaiwan, Natl. Tsing Hua U.
002255384 700__ $$aHsu, Shih-Chieh$$iINSPIRE-00041120$$uWashington U., Seattle
002255384 700__ $$aHu, Qipeng$$iINSPIRE-00386928$$uHefei, CUST
002255384 700__ $$aHu, Shuyang$$iINSPIRE-00388803$$uShanghai Jiao Tong U.
002255384 700__ $$aHuang, Yanping$$iINSPIRE-00340219$$uBeijing, Inst. High Energy Phys.
002255384 700__ $$aHubacek, Zdenek$$iINSPIRE-00032940$$uPrague, Tech. U.
002255384 700__ $$aHubaut, Fabrice$$iINSPIRE-00215862$$uMarseille, CPPM
002255384 700__ $$aHuegging, Fabian$$iINSPIRE-00215874$$uBonn U.
002255384 700__ $$aHuffman, Todd Brian$$iINSPIRE-00215888$$uOxford U.
002255384 700__ $$aHughes, Emlyn$$iINSPIRE-00091540$$uNevis Labs, Columbia U.
002255384 700__ $$aHughes, Gareth$$iINSPIRE-00091551$$uLancaster U.
002255384 700__ $$aHuhtinen, Mika$$iINSPIRE-00320486$$uCERN
002255384 700__ $$aHuo, Peng$$iINSPIRE-00386180$$uSUNY, Stony Brook
002255384 700__ $$aHuseynov, Nazim$$iINSPIRE-00215894$$uDubna, JINR$$uBaku, Inst. Phys.
002255384 700__ $$aHuston, Joey$$iINSPIRE-00091715$$uMichigan State U.
002255384 700__ $$aHuth, John$$iINSPIRE-00091758$$uHarvard U., Phys. Dept.
002255384 700__ $$aIacobucci, Giuseppe$$iINSPIRE-00172036$$uGeneva U.
002255384 700__ $$aIakovidis, Georgios$$iINSPIRE-00215906$$uBrookhaven
002255384 700__ $$aIbragimov, Iskander$$iINSPIRE-00215918$$uSiegen U.
002255384 700__ $$aIconomidou-Fayard, Lydia$$iINSPIRE-00215920$$uOrsay, LAL
002255384 700__ $$aIengo, Paolo$$iINSPIRE-00215943$$uCERN
002255384 700__ $$aIgonkina, Olga$$iINSPIRE-00057191$$uFOM, Amsterdam$$uNIKHEF, Amsterdam
002255384 700__ $$aIizawa, Tomoya$$iINSPIRE-00353645$$uWaseda U.
002255384 700__ $$aIkegami, Yoichi$$iINSPIRE-00215955$$uKEK, Tsukuba
002255384 700__ $$aIkeno, Masahiro$$iINSPIRE-00215967$$uKEK, Tsukuba
002255384 700__ $$aIlchenko, Yuriy$$iINSPIRE-00180687$$uTexas U.
002255384 700__ $$aIliadis, Dimitrios$$iINSPIRE-00215979$$uAristotle U., Thessaloniki
002255384 700__ $$aIlic, Nikolina$$iINSPIRE-00236423$$uSLAC
002255384 700__ $$aIntrozzi, Gianluca$$iINSPIRE-00092229$$uINFN, Pavia$$uPavia U.
002255384 700__ $$aIoannou, Pavlos$$iINSPIRE-00214597$$uAthens U.
002255384 700__ $$aIodice, Mauro$$iINSPIRE-00215987$$uINFN, Rome
002255384 700__ $$aIordanidou, Kalliopi$$iINSPIRE-00286590$$uNevis Labs, Columbia U.
002255384 700__ $$aIppolito, Valerio$$iINSPIRE-00286608$$uHarvard U., Phys. Dept.
002255384 700__ $$aIshijima, Naoki$$iINSPIRE-00417878$$uOsaka U.
002255384 700__ $$aIshino, Masaya$$iINSPIRE-00092428$$uTokyo U., ICEPP
002255384 700__ $$aIshitsuka, Masaki$$iINSPIRE-00184437$$uTokyo Inst. Tech.
002255384 700__ $$aIssever, Cigdem$$iINSPIRE-00178101$$uOxford U.
002255384 700__ $$aIstin, Serhat$$iINSPIRE-00216012$$uBogazici U.
002255384 700__ $$aIto, Fumiaki$$iINSPIRE-00441977$$uTsukuba U.
002255384 700__ $$aIturbe Ponce, Julia Mariana$$iINSPIRE-00358758$$uManchester U.
002255384 700__ $$aIuppa, Roberto$$iINSPIRE-00368483$$uTIFPA-INFN, Trento$$uTrento U.
002255384 700__ $$aIwasaki, Hiroyuki$$iINSPIRE-00216040$$uKEK, Tsukuba
002255384 700__ $$aIzen, Joseph$$iINSPIRE-00092738$$uTexas U., Dallas
002255384 700__ $$aIzzo, Vincenzo$$iINSPIRE-00216053$$uINFN, Naples
002255384 700__ $$aJabbar, Samina$$iINSPIRE-00377064$$uAlberta U.
002255384 700__ $$aJackson, Paul$$iINSPIRE-00042110$$uAdelaide U., Sch. Chem. Phys.
002255384 700__ $$aJain, Vivek$$iINSPIRE-00093006$$uSUNY, Albany
002255384 700__ $$aJakobi, Katharina Bianca$$iINSPIRE-00381934$$uMainz U.
002255384 700__ $$aJakobs, Karl$$iINSPIRE-00093013$$uFreiburg U.
002255384 700__ $$aJakobsen, Sune$$iINSPIRE-00216083$$uCERN
002255384 700__ $$aJakoubek, Tomas$$iINSPIRE-00236452$$uPrague, Inst. Phys.
002255384 700__ $$aJamin, David Olivier$$iINSPIRE-00019160$$uOklahoma State U.
002255384 700__ $$aJana, Dilip$$iINSPIRE-00216107$$uLouisiana Tech. U.
002255384 700__ $$aJansky, Roland$$iINSPIRE-00389298$$uInnsbruck U.
002255384 700__ $$aJanssen, Jens$$iINSPIRE-00339121$$uBonn U.
002255384 700__ $$aJanus, Michel$$iINSPIRE-00216144$$uGottingen U., II. Phys. Inst.
002255384 700__ $$aJanus, Piotr Andrzej$$iINSPIRE-00524744$$uAGH-UST, Cracow
002255384 700__ $$aJarlskog, Göran$$iINSPIRE-00175123$$uLund U.
002255384 700__ $$aJavadov, Namig$$iINSPIRE-00358780$$uDubna, JINR$$uBaku, Inst. Phys.
002255384 700__ $$aJavůrek, Tomáš$$iINSPIRE-00359657$$uFreiburg U.
002255384 700__ $$aJavurkova, Martina$$iINSPIRE-00359670$$uFreiburg U.
002255384 700__ $$aJeanneau, Fabien$$iINSPIRE-00380308$$uIRFU, Saclay
002255384 700__ $$aJeanty, Laura$$iINSPIRE-00216156$$uLBL, Berkeley
002255384 700__ $$aJejelava, Juansher$$iINSPIRE-00396142$$uTbilisi, Inst. Phys.$$uIlia State U.
002255384 700__ $$aJelinskas, Adomas$$iINSPIRE-00537773$$uWarwick U.
002255384 700__ $$aJenni, Peter$$iINSPIRE-00093290$$uFreiburg U.$$uCERN
002255384 700__ $$aJeske, Carl$$iINSPIRE-00337640$$uWarwick U.
002255384 700__ $$aJézéquel, Stéphane$$iINSPIRE-00216174$$uAnnecy, LAPP
002255384 700__ $$aJi, Haoshuang$$iINSPIRE-00216186$$uWisconsin U., Madison
002255384 700__ $$aJia, Jiangyong$$iINSPIRE-00241915$$uSUNY, Stony Brook
002255384 700__ $$aJiang, Hai$$iINSPIRE-00431393$$uIowa State U.
002255384 700__ $$aJiang, Yi$$iINSPIRE-00216201$$uHefei, CUST
002255384 700__ $$aJiang, Zihao$$iINSPIRE-00524754$$uSLAC
002255384 700__ $$aJiggins, Stephen$$iINSPIRE-00392933$$uUniversity Coll. London
002255384 700__ $$aJimenez Pena, Javier$$iINSPIRE-00386283$$uValencia U., IFIC
002255384 700__ $$aJin, Shan$$iINSPIRE-00216225$$uBeijing, Inst. High Energy Phys.
002255384 700__ $$aJinaru, Adam$$iINSPIRE-00349814$$uBucharest, IFIN-HH
002255384 700__ $$aJinnouchi, Osamu$$iINSPIRE-00241926$$uTokyo Inst. Tech.
002255384 700__ $$aJivan, Harshna$$iINSPIRE-00507050$$uWitwatersrand U.
002255384 700__ $$aJohansson, Per$$iINSPIRE-00305905$$uSheffield U.
002255384 700__ $$aJohns, Kenneth$$iINSPIRE-00093591$$uArizona U.
002255384 700__ $$aJohnson, Christian$$iINSPIRE-00512851$$uIndiana U.
002255384 700__ $$aJohnson, William Joseph$$iINSPIRE-00424402$$uWashington U., Seattle
002255384 700__ $$aJon-And, Kerstin$$iINSPIRE-00180510$$uStockholm U.$$uStockholm U., OKC
002255384 700__ $$aJones, Roger$$iINSPIRE-00216280$$uLancaster U.
002255384 700__ $$aJones, Sarah$$iINSPIRE-00439605$$uArizona U.
002255384 700__ $$aJones, Tim$$iINSPIRE-00227120$$uLiverpool U.
002255384 700__ $$aJongmanns, Jan$$iINSPIRE-00362112$$uKirchhoff Inst. Phys.
002255384 700__ $$aJorge, Pedro$$iINSPIRE-00227131$$uLIP, Lisbon$$uLisbon U., CFNUL
002255384 700__ $$aJovicevic, Jelena$$iINSPIRE-00286620$$uTRIUMF
002255384 700__ $$aJu, Xiangyang$$iINSPIRE-00230799$$uWisconsin U., Madison
002255384 700__ $$aJuste Rozas, Aurelio$$iINSPIRE-00094149$$uBarcelona, IFAE$$uICREA, Barcelona
002255384 700__ $$aKöhler, Markus Konrad$$iINSPIRE-00244603$$uWeizmann Inst.
002255384 700__ $$aKaczmarska, Anna$$iINSPIRE-00216330$$uCracow, INP
002255384 700__ $$aKado, Marumi$$iINSPIRE-00216354$$uOrsay, LAL
002255384 700__ $$aKagan, Harris$$iINSPIRE-00144825$$uOhio State U.
002255384 700__ $$aKagan, Michael$$iINSPIRE-00008953$$uSLAC
002255384 700__ $$aKahn, Sebastien Jonathan$$iINSPIRE-00388044$$uMarseille, CPPM
002255384 700__ $$aKaji, Toshiaki$$iINSPIRE-00517162$$uWaseda U.
002255384 700__ $$aKajomovitz, Enrique$$iINSPIRE-00216378$$uDuke U.
002255384 700__ $$aKalderon, Charles William$$iINSPIRE-00358313$$uLund U.
002255384 700__ $$aKaluza, Adam$$iINSPIRE-00375925$$uMainz U.
002255384 700__ $$aKama, Sami$$iINSPIRE-00216391$$uSouthern Methodist U.
002255384 700__ $$aKamenshchikov, Andrey$$iINSPIRE-00374470$$uSerpukhov, IHEP
002255384 700__ $$aKanaya, Naoko$$iINSPIRE-00197922$$uTokyo U., ICEPP
002255384 700__ $$aKaneti, Steven$$iINSPIRE-00236623$$uCambridge U.
002255384 700__ $$aKanjir, Luka$$iINSPIRE-00405560$$uStefan Inst., Ljubljana
002255384 700__ $$aKantserov, Vadim$$iINSPIRE-00216415$$uMoscow Phys. Eng. Inst.
002255384 700__ $$aKanzaki, Junichi$$iINSPIRE-00216427$$uKEK, Tsukuba
002255384 700__ $$aKaplan, Benjamin$$iINSPIRE-00216439$$uNew York U.
002255384 700__ $$aKaplan, Laser Seymour$$iINSPIRE-00407495$$uWisconsin U., Madison
002255384 700__ $$aKar, Deepak$$iINSPIRE-00022031$$uWitwatersrand U.
002255384 700__ $$aKarakostas, Konstantinos$$iINSPIRE-00339134$$uNatl. Tech. U., Athens
002255384 700__ $$aKarastathis, Nikolaos$$iINSPIRE-00349829$$uNatl. Tech. U., Athens
002255384 700__ $$aKareem, Mohammad Jawad$$iINSPIRE-00384533$$uGottingen U., II. Phys. Inst.
002255384 700__ $$aKarentzos, Efstathios$$iINSPIRE-00409082$$uNatl. Tech. U., Athens
002255384 700__ $$aKarpov, Sergey$$iINSPIRE-00236647$$uDubna, JINR
002255384 700__ $$aKarpova, Zoya$$iINSPIRE-00236653$$uDubna, JINR
002255384 700__ $$aKarthik, Krishnaiyengar$$iINSPIRE-00346141$$uNew York U.
002255384 700__ $$aKartvelishvili, Vakhtang$$iINSPIRE-00188948$$uLancaster U.
002255384 700__ $$aKaryukhin, Andrey$$iINSPIRE-00216469$$uSerpukhov, IHEP
002255384 700__ $$aKasahara, Kota$$iINSPIRE-00417950$$uTsukuba U.
002255384 700__ $$aKashif, Lashkar$$iINSPIRE-00005306$$uWisconsin U., Madison
002255384 700__ $$aKass, Richard$$iINSPIRE-00144848$$uOhio State U.
002255384 700__ $$aKastanas, Alex$$iINSPIRE-00216472$$uRoyal Inst. Tech., Stockholm
002255384 700__ $$aKataoka, Yousuke$$iINSPIRE-00216508$$uTokyo U., ICEPP
002255384 700__ $$aKato, Chikuma$$iINSPIRE-00413068$$uTokyo U., ICEPP
002255384 700__ $$aKatre, Akshay$$iINSPIRE-00345043$$uGeneva U.
002255384 700__ $$aKatzy, Judith$$iINSPIRE-00185240$$uDESY
002255384 700__ $$aKawade, Kentaro$$iINSPIRE-00419409$$uNagoya U.
002255384 700__ $$aKawagoe, Kiyotomo$$iINSPIRE-00095283$$uKyushu U.
002255384 700__ $$aKawamoto, Tatsuo$$iINSPIRE-00216510$$uTokyo U., ICEPP
002255384 700__ $$aKawamura, Gen$$iINSPIRE-00216521$$uGottingen U., II. Phys. Inst.
002255384 700__ $$aKay, Ellis$$iINSPIRE-00536644$$uLiverpool U.
002255384 700__ $$aKazanin, Vassili$$iINSPIRE-00216540$$uNovosibirsk State U.$$uNovosibirsk, IYF
002255384 700__ $$aKeeler, Richard$$iINSPIRE-00095435$$uVictoria U.
002255384 700__ $$aKehoe, Robert$$iINSPIRE-00095456$$uSouthern Methodist U.
002255384 700__ $$aKeller, John$$iINSPIRE-00334458$$uDESY
002255384 700__ $$aKempster, Jacob Julian$$iINSPIRE-00371337$$uRoyal Holloway, U. of London
002255384 700__ $$aKeoshkerian, Houry$$iINSPIRE-00334460$$uToronto U.
002255384 700__ $$aKepka, Oldrich$$iINSPIRE-00026678$$uPrague, Inst. Phys.
002255384 700__ $$aKerševan, Borut Paul$$iINSPIRE-00216670$$uStefan Inst., Ljubljana
002255384 700__ $$aKersten, Susanne$$iINSPIRE-00095720$$uWuppertal U.
002255384 700__ $$aKeyes, Robert$$iINSPIRE-00377077$$uMcGill U.
002255384 700__ $$aKhader, Mazin$$iINSPIRE-00517175$$uIllinois U., Urbana
002255384 700__ $$aKhalil-zada, Farkhad$$iINSPIRE-00216693$$uBaku, Inst. Phys.
002255384 700__ $$aKhanov, Alexander$$iINSPIRE-00053352$$uOklahoma State U.
002255384 700__ $$aKharlamov, Alexey$$iINSPIRE-00297758$$uNovosibirsk State U.$$uNovosibirsk, IYF
002255384 700__ $$aKharlamova, Tatyana$$iINSPIRE-00524947$$uNovosibirsk State U.$$uNovosibirsk, IYF
002255384 700__ $$aKhodinov, Alexander$$iINSPIRE-00216729$$uTomsk State U.
002255384 700__ $$aKhoo, Teng Jian$$iINSPIRE-00230858$$uGeneva U.
002255384 700__ $$aKhovanskiy, Valery$$iINSPIRE-00216747$$uMoscow, ITEP
002255384 700__ $$aKhramov, Evgeniy$$iINSPIRE-00305942$$uDubna, JINR
002255384 700__ $$aKhubua, Jemal$$iINSPIRE-00305959$$uTbilisi State U.$$uGTU, Tbilisi
002255384 700__ $$aKido, Shogo$$iINSPIRE-00413107$$uKobe U.
002255384 700__ $$aKilby, Callum$$iINSPIRE-00514530$$uRoyal Holloway, U. of London
002255384 700__ $$aKim, Hee Yeun$$iINSPIRE-00356588$$uTexas U., Arlington
002255384 700__ $$aKim, Shinhong$$iINSPIRE-00019770$$uTsukuba U.
002255384 700__ $$aKim, Young-Kee$$iINSPIRE-00096350$$uChicago U., EFI
002255384 700__ $$aKimura, Naoki$$iINSPIRE-00008600$$uAristotle U., Thessaloniki
002255384 700__ $$aKind, Oliver Maria$$iINSPIRE-00191251$$uHumboldt U., Berlin
002255384 700__ $$aKing, Barry$$iINSPIRE-00039391$$uLiverpool U.
002255384 700__ $$aKirchmeier, David$$iINSPIRE-00524951$$uDresden, Tech. U.
002255384 700__ $$aKirk, Julie$$iINSPIRE-00216784$$uRutherford
002255384 700__ $$aKiryunin, Andrey$$iINSPIRE-00216808$$uMunich, Max Planck Inst.
002255384 700__ $$aKishimoto, Tomoe$$iINSPIRE-00236684$$uTokyo U., ICEPP
002255384 700__ $$aKisielewska, Danuta$$iINSPIRE-00172500$$uAGH-UST, Cracow
002255384 700__ $$aKiuchi, Kenji$$iINSPIRE-00287960$$uTsukuba U.
002255384 700__ $$aKivernyk, Oleh$$iINSPIRE-00408270$$uIRFU, Saclay
002255384 700__ $$aKladiva, Eduard$$iINSPIRE-00216810$$uKosice, IEF
002255384 700__ $$aKlapdor-Kleingrothaus, Thorwald$$iINSPIRE-00534640$$uFreiburg U.
002255384 700__ $$aKlein, Matthew Henry$$iINSPIRE-00380915$$uNevis Labs, Columbia U.
002255384 700__ $$aKlein, Max$$iINSPIRE-00096790$$uLiverpool U.
002255384 700__ $$aKlein, Uta$$iINSPIRE-00172660$$uLiverpool U.
002255384 700__ $$aKleinknecht, Konrad$$iINSPIRE-00157115$$uMainz U.
002255384 700__ $$aKlimek, Pawel$$iINSPIRE-00236698$$uNorthern Illinois U.
002255384 700__ $$aKlimentov, Alexei$$iINSPIRE-00216840$$uBrookhaven
002255384 700__ $$aKlingenberg, Reiner$$iINSPIRE-00189090$$uDortmund U.
002255384 700__ $$aKlioutchnikova, Tatiana$$iINSPIRE-00216863$$uCERN
002255384 700__ $$aKluge, Eike-Erik$$iINSPIRE-00157565$$uKirchhoff Inst. Phys.
002255384 700__ $$aKluit, Peter$$iINSPIRE-00096892$$uFOM, Amsterdam
002255384 700__ $$aKluth, Stefan$$iINSPIRE-00096918$$uMunich, Max Planck Inst.
002255384 700__ $$aKnapik, Joanna$$iINSPIRE-00389577$$uCracow, INP
002255384 700__ $$aKneringer, Emmerich$$iINSPIRE-00096974$$uInnsbruck U.
002255384 700__ $$aKnoops, Edith$$iINSPIRE-00096991$$uMarseille, CPPM
002255384 700__ $$aKnue, Andrea$$iINSPIRE-00230947$$uMunich, Max Planck Inst.
002255384 700__ $$aKobayashi, Aine$$iINSPIRE-00403465$$uTokyo U., ICEPP
002255384 700__ $$aKobayashi, Dai$$iINSPIRE-00374480$$uTokyo Inst. Tech.
002255384 700__ $$aKobayashi, Tomio$$iINSPIRE-00210282$$uTokyo U., ICEPP
002255384 700__ $$aKobel, Michael$$iINSPIRE-00097070$$uDresden, Tech. U.
002255384 700__ $$aKocian, Martin$$iINSPIRE-00041830$$uSLAC
002255384 700__ $$aKodys, Peter$$iINSPIRE-00216912$$uCharles U.
002255384 700__ $$aKoffas, Thomas$$iINSPIRE-00218105$$uCarleton U.
002255384 700__ $$aKoffeman, Els$$iINSPIRE-00173731$$uFOM, Amsterdam
002255384 700__ $$aKöhler, Nicolas Maximilian$$iINSPIRE-00517182$$uMunich, Max Planck Inst.
002255384 700__ $$aKoi, Tatsumi$$iINSPIRE-00035594$$uSLAC
002255384 700__ $$aKolb, Mathis$$iINSPIRE-00417839$$uHeidelberg U.
002255384 700__ $$aKoletsou, Iro$$iINSPIRE-00015902$$uAnnecy, LAPP
002255384 700__ $$aKomar, Aston$$iINSPIRE-00218307$$uLebedev Inst.
002255384 700__ $$aKomori, Yuto$$iINSPIRE-00236718$$uTokyo U., ICEPP
002255384 700__ $$aKondo, Takahiko$$iINSPIRE-00097562$$uKEK, Tsukuba
002255384 700__ $$aKondrashova, Nataliia$$iINSPIRE-00345331$$uShanghai Jiao Tong U.
002255384 700__ $$aKöneke, Karsten$$iINSPIRE-00042236$$uFreiburg U.
002255384 700__ $$aKönig, Adriaan$$iINSPIRE-00097590$$uNIKHEF, Amsterdam
002255384 700__ $$aKono, Takanori$$iINSPIRE-00218319$$uKEK, Tsukuba$$uOchanomizu U.
002255384 700__ $$aKonoplich, Rostislav$$iINSPIRE-00097654$$uNew York U.$$uManhattan Coll., Riverdale
002255384 700__ $$aKonstantinidis, Nikolaos$$iINSPIRE-00097667$$uUniversity Coll. London
002255384 700__ $$aKopeliansky, Revital$$iINSPIRE-00337069$$uIndiana U.
002255384 700__ $$aKoperny, Stefan$$iINSPIRE-00218320$$uAGH-UST, Cracow
002255384 700__ $$aKopp, Anna Katharina$$iINSPIRE-00332927$$uFreiburg U.
002255384 700__ $$aKorcyl, Krzysztof$$iINSPIRE-00097773$$uCracow, INP
002255384 700__ $$aKordas, Kostantinos$$iINSPIRE-00218332$$uAristotle U., Thessaloniki
002255384 700__ $$aKorn, Andreas$$iINSPIRE-00052183$$uUniversity Coll. London
002255384 700__ $$aKorol, Aleksandr$$iINSPIRE-00032898$$uNovosibirsk State U.$$uNovosibirsk, IYF
002255384 700__ $$aKorolkov, Ilya$$iINSPIRE-00097847$$uBarcelona, IFAE
002255384 700__ $$aKorolkova, Elena$$iINSPIRE-00218344$$uSheffield U.
002255384 700__ $$aKortner, Oliver$$iINSPIRE-00218368$$uMunich, Max Planck Inst.
002255384 700__ $$aKortner, Sandra$$iINSPIRE-00215825$$uMunich, Max Planck Inst.
002255384 700__ $$aKosek, Tomas$$iINSPIRE-00364770$$uCharles U.
002255384 700__ $$aKostyukhin, Vadim$$iINSPIRE-00218374$$uBonn U.
002255384 700__ $$aKotwal, Ashutosh$$iINSPIRE-00097984$$uDuke U.
002255384 700__ $$aKoulouris, Aimilianos$$iINSPIRE-00524960$$uNatl. Tech. U., Athens
002255384 700__ $$aKourkoumeli-Charalampidi, Athina$$iINSPIRE-00365526$$uINFN, Pavia$$uPavia U.
002255384 700__ $$aKourkoumelis, Christine$$iINSPIRE-00218386$$uAthens U.
002255384 700__ $$aKouskoura, Vasiliki$$iINSPIRE-00286669$$uBrookhaven
002255384 700__ $$aKowalewska, Anna Bozena$$iINSPIRE-00431470$$uCracow, INP
002255384 700__ $$aKowalewski, Robert Victor$$iINSPIRE-00098130$$uVictoria U.
002255384 700__ $$aKowalski, Tadeusz$$iINSPIRE-00305987$$uAGH-UST, Cracow
002255384 700__ $$aKozakai, Chihiro$$iINSPIRE-00452631$$uTokyo U., ICEPP
002255384 700__ $$aKozanecki, Witold$$iINSPIRE-00098207$$uIRFU, Saclay
002255384 700__ $$aKozhin, Anatoly$$iINSPIRE-00218400$$uSerpukhov, IHEP
002255384 700__ $$aKramarenko, Viktor$$iINSPIRE-00218423$$uMoscow State U.
002255384 700__ $$aKramberger, Gregor$$iINSPIRE-00098259$$uStefan Inst., Ljubljana
002255384 700__ $$aKrasnopevtsev, Dimitriy$$iINSPIRE-00349845$$uMoscow Phys. Eng. Inst.
002255384 700__ $$aKrasny, Mieczyslaw Witold$$iINSPIRE-00218435$$uParis U., VI-VII
002255384 700__ $$aKrasznahorkay, Attila$$iINSPIRE-00218447$$uCERN
002255384 700__ $$aKrauss, Dominik$$iINSPIRE-00540551$$uMunich, Max Planck Inst.
002255384 700__ $$aKravchenko, Anton$$iINSPIRE-00334471$$uBrookhaven
002255384 700__ $$aKremer, Jakub Andrzej$$iINSPIRE-00524978$$uAGH-UST, Cracow
002255384 700__ $$aKretz, Moritz$$iINSPIRE-00358345$$uHeidelberg U.
002255384 700__ $$aKretzschmar, Jan$$iINSPIRE-00185292$$uLiverpool U.
002255384 700__ $$aKreutzfeldt, Kristof$$iINSPIRE-00329505$$uGiessen U.
002255384 700__ $$aKrieger, Peter$$iINSPIRE-00195228$$uToronto U.
002255384 700__ $$aKrizka, Karol$$iINSPIRE-00384270$$uChicago U., EFI
002255384 700__ $$aKroeninger, Kevin$$iINSPIRE-00218479$$uDortmund U.
002255384 700__ $$aKroha, Hubert$$iINSPIRE-00218480$$uMunich, Max Planck Inst.
002255384 700__ $$aKroll, Joe$$iINSPIRE-00098670$$uPennsylvania U.
002255384 700__ $$aKroseberg, Juergen$$iINSPIRE-00042884$$uBonn U.
002255384 700__ $$aKrstic, Jelena$$iINSPIRE-00218492$$uBelgrade U.
002255384 700__ $$aKruchonak, Uladzimir$$iINSPIRE-00218504$$uDubna, JINR
002255384 700__ $$aKrüger, Hans$$iINSPIRE-00218516$$uBonn U.
002255384 700__ $$aKrumnack, Nils$$iINSPIRE-00055045$$uIowa State U.
002255384 700__ $$aKruse, Mark$$iINSPIRE-00098798$$uDuke U.
002255384 700__ $$aKruskal, Michael$$iINSPIRE-00342652$$uBoston U.
002255384 700__ $$aKubota, Takashi$$iINSPIRE-00218541$$uMelbourne U.
002255384 700__ $$aKucuk, Hilal$$iINSPIRE-00370994$$uUniversity Coll. London
002255384 700__ $$aKuday, Sinan$$iINSPIRE-00236766$$uIstanbul Aydin U.
002255384 700__ $$aKuechler, Jan Thomas$$iINSPIRE-00439671$$uWuppertal U.
002255384 700__ $$aKuehn, Susanne$$iINSPIRE-00218553$$uFreiburg U.
002255384 700__ $$aKugel, Andreas$$iINSPIRE-00218560$$uHeidelberg U.
002255384 700__ $$aKuger, Fabian$$iINSPIRE-00387450$$uWurzburg U.
002255384 700__ $$aKuhl, Thorsten$$iINSPIRE-00051546$$uDESY
002255384 700__ $$aKukhtin, Victor$$iINSPIRE-00218599$$uDubna, JINR
002255384 700__ $$aKukla, Romain$$iINSPIRE-00388150$$uMarseille, CPPM
002255384 700__ $$aKulchitsky, Yuri$$iINSPIRE-00098974$$uMinsk, Inst. Phys.
002255384 700__ $$aKuleshov, Sergey$$iINSPIRE-00320322$$uSanta Maria U., Valparaiso
002255384 700__ $$aKulinich, Yakov Petrovich$$iINSPIRE-00517193$$uIllinois U., Urbana
002255384 700__ $$aKuna, Marine$$iINSPIRE-00218612$$uINFN, Rome$$uRome U.
002255384 700__ $$aKunigo, Takuto$$iINSPIRE-00381656$$uKyoto U.
002255384 700__ $$aKupco, Alexander$$iINSPIRE-00099163$$uPrague, Inst. Phys.
002255384 700__ $$aKuprash, Oleg$$iINSPIRE-00173407$$uTel Aviv U.
002255384 700__ $$aKurashige, Hisaya$$iINSPIRE-00099197$$uKobe U.
002255384 700__ $$aKurchaninov, Leonid$$iINSPIRE-00524990$$uTRIUMF
002255384 700__ $$aKurochkin, Yurii$$iINSPIRE-00218636$$uMinsk, Inst. Phys.
002255384 700__ $$aKurth, Matthew Glenn$$iINSPIRE-00537264$$uBeijing, Inst. High Energy Phys.
002255384 700__ $$aKus, Vlastimil$$iINSPIRE-00218642$$uPrague, Inst. Phys.
002255384 700__ $$aKuwertz, Emma Sian$$iINSPIRE-00286685$$uVictoria U.
002255384 700__ $$aKuze, Masahiro$$iINSPIRE-00099360$$uTokyo Inst. Tech.
002255384 700__ $$aKvita, Jiri$$iINSPIRE-00038915$$uPalacky U.
002255384 700__ $$aKwan, Tony$$iINSPIRE-00379325$$uVictoria U.
002255384 700__ $$aKyriazopoulos, Dimitrios$$iINSPIRE-00374537$$uSheffield U.
002255384 700__ $$aLa Rosa, Alessandro$$iINSPIRE-00218666$$uMunich, Max Planck Inst.
002255384 700__ $$aLa Rosa Navarro, Jose Luis$$iINSPIRE-00379447$$uSao Paulo U.
002255384 700__ $$aLa Rotonda, Laura$$iINSPIRE-00218678$$uINFN, Cosenza$$uCalabria U.
002255384 700__ $$aLacasta, Carlos$$iINSPIRE-00099524$$uValencia U., IFIC
002255384 700__ $$aLacava, Francesco$$iINSPIRE-00218690$$uINFN, Rome$$uRome U.
002255384 700__ $$aLacey, James$$iINSPIRE-00334483$$uDESY
002255384 700__ $$aLacker, Heiko$$iINSPIRE-00042702$$uHumboldt U., Berlin
002255384 700__ $$aLacour, Didier$$iINSPIRE-00099578$$uParis U., VI-VII
002255384 700__ $$aLadygin, Evgueni$$iINSPIRE-00099592$$uDubna, JINR
002255384 700__ $$aLafaye, Remi$$iINSPIRE-00218717$$uAnnecy, LAPP
002255384 700__ $$aLaforge, Bertrand$$iINSPIRE-00057788$$uParis U., VI-VII
002255384 700__ $$aLagouri, Theodota$$iINSPIRE-00218740$$uYale U.
002255384 700__ $$aLai, Stanley$$iINSPIRE-00218758$$uGottingen U., II. Phys. Inst.
002255384 700__ $$aLammers, Sabine$$iINSPIRE-00051670$$uIndiana U.
002255384 700__ $$aLampl, Walter$$iINSPIRE-00218776$$uArizona U.
002255384 700__ $$aLançon, Eric$$iINSPIRE-00218788$$uBrookhaven
002255384 700__ $$aLandgraf, Ulrich$$iINSPIRE-00218790$$uFreiburg U.
002255384 700__ $$aLandon, Murrough$$iINSPIRE-00099860$$uQueen Mary, U. of London
002255384 700__ $$aLanfermann, Marie Christine$$iINSPIRE-00508917$$uGeneva U.
002255384 700__ $$aLang, Valerie Susanne$$iINSPIRE-00286700$$uKirchhoff Inst. Phys.
002255384 700__ $$aLange, J örn Christian$$iINSPIRE-00397348$$uBarcelona, IFAE
002255384 700__ $$aLankford, Andrew$$iINSPIRE-00100028$$uUC, Irvine
002255384 700__ $$aLanni, Francesco$$iINSPIRE-00100030$$uBrookhaven
002255384 700__ $$aLantzsch, Kerstin$$iINSPIRE-00218824$$uBonn U.
002255384 700__ $$aLanza, Agostino$$iINSPIRE-00218836$$uINFN, Pavia
002255384 700__ $$aLapertosa, Alessandro$$iINSPIRE-00536668$$uINFN, Genoa$$uGenoa U.
002255384 700__ $$aLaplace, Sandrine$$iINSPIRE-00032441$$uParis U., VI-VII
002255384 700__ $$aLaporte, Jean-Francois$$iINSPIRE-00218850$$uIRFU, Saclay
002255384 700__ $$aLari, Tommaso$$iINSPIRE-00240476$$uINFN, Milan
002255384 700__ $$aLasagni Manghi, Federico$$iINSPIRE-00378808$$uINFN, Bologna$$uBologna U.
002255384 700__ $$aLassnig, Mario$$iINSPIRE-00218873$$uCERN
002255384 700__ $$aLaurelli, Paolo$$iINSPIRE-00100213$$uFrascati
002255384 700__ $$aLavrijsen, Wim$$iINSPIRE-00055620$$uLBL, Berkeley
002255384 700__ $$aLaw, Alexander$$iINSPIRE-00348140$$uUC, Santa Cruz
002255384 700__ $$aLaycock, Paul$$iINSPIRE-00037318$$uLiverpool U.
002255384 700__ $$aLazovich, Tomo$$iINSPIRE-00015492$$uHarvard U., Phys. Dept.
002255384 700__ $$aLazzaroni, Massimo$$iINSPIRE-00445566$$uINFN, Milan$$uMilan U.
002255384 700__ $$aLe, Brian$$iINSPIRE-00507250$$uMelbourne U.
002255384 700__ $$aLe Dortz, Olivier$$iINSPIRE-00218897$$uParis U., VI-VII
002255384 700__ $$aLe Guirriec, Emmanuel$$iINSPIRE-00218909$$uMarseille, CPPM
002255384 700__ $$aLe Quilleuc, Eloi$$iINSPIRE-00439709$$uIRFU, Saclay
002255384 700__ $$aLeBlanc, Matthew Edgar$$iINSPIRE-00397460$$uVictoria U.
002255384 700__ $$aLeCompte, Thomas$$iINSPIRE-00100495$$uArgonne
002255384 700__ $$aLedroit-Guillon, Fabienne$$iINSPIRE-00200437$$uLPSC, Grenoble
002255384 700__ $$aLee, Claire Alexandra$$iINSPIRE-00048758$$uBrookhaven
002255384 700__ $$aLee, Shih-Chang$$iINSPIRE-00100720$$uTaiwan, Inst. Phys.
002255384 700__ $$aLee, Lawrence$$iINSPIRE-00231146$$uAdelaide U., Sch. Chem. Phys.
002255384 700__ $$aLefebvre, Benoit$$iINSPIRE-00426582$$uMcGill U.
002255384 700__ $$aLefebvre, Guillaume$$iINSPIRE-00339142$$uParis U., VI-VII
002255384 700__ $$aLefebvre, Michel$$iINSPIRE-00198481$$uVictoria U.
002255384 700__ $$aLegger, Federica$$iINSPIRE-00218990$$uMunich U.
002255384 700__ $$aLeggett, Charles$$iINSPIRE-00100895$$uLBL, Berkeley
002255384 700__ $$aLehan, Allan$$iINSPIRE-00342678$$uLiverpool U.
002255384 700__ $$aLehmann Miotto, Giovanna$$iINSPIRE-00100928$$uCERN
002255384 700__ $$aLei, Xiaowen$$iINSPIRE-00219018$$uArizona U.
002255384 700__ $$aLeight, William Axel$$iINSPIRE-00182253$$uDESY
002255384 700__ $$aLeister, Andrew Gerard$$iINSPIRE-00329227$$uYale U.
002255384 700__ $$aLeite, Marco Aurelio Lisboa$$iINSPIRE-00242334$$uSao Paulo U.
002255384 700__ $$aLeitner, Rupert$$iINSPIRE-00301106$$uCharles U.
002255384 700__ $$aLellouch, Daniel$$iINSPIRE-00101050$$uWeizmann Inst.
002255384 700__ $$aLemmer, Boris$$iINSPIRE-00236819$$uGottingen U., II. Phys. Inst.
002255384 700__ $$aLeney, Katharine$$iINSPIRE-00192210$$uUniversity Coll. London
002255384 700__ $$aLenz, Tatjana$$iINSPIRE-00219020$$uBonn U.
002255384 700__ $$aLenzi, Bruno$$iINSPIRE-00242346$$uCERN
002255384 700__ $$aLeone, Robert$$iINSPIRE-00263632$$uArizona U.
002255384 700__ $$aLeone, Sandra$$iINSPIRE-00101163$$uINFN, Pisa$$uPisa U.
002255384 700__ $$aLeonidopoulos, Christos$$iINSPIRE-00101179$$uEdinburgh U.
002255384 700__ $$aLerner, Giuseppe$$iINSPIRE-00442062$$uSussex U.
002255384 700__ $$aLeroy, Claude$$iINSPIRE-00149161$$uMontreal U.
002255384 700__ $$aLesage, Arthur$$iINSPIRE-00439764$$uIRFU, Saclay
002255384 700__ $$aLester, Christopher$$iINSPIRE-00101328$$uCambridge U.
002255384 700__ $$aLevchenko, Mikhail$$iINSPIRE-00358155$$uSt. Petersburg, INP
002255384 700__ $$aLevêque, Jessica$$iINSPIRE-00038900$$uAnnecy, LAPP
002255384 700__ $$aLevin, Daniel$$iINSPIRE-00101433$$uMichigan U.
002255384 700__ $$aLevinson, Lorne$$iINSPIRE-00101477$$uWeizmann Inst.
002255384 700__ $$aLevy, Mark$$iINSPIRE-00365538$$uBirmingham U.
002255384 700__ $$aLewis, Dave$$iINSPIRE-00443670$$uQueen Mary, U. of London
002255384 700__ $$aLeyton, Michael$$iINSPIRE-00219067$$uTexas U., Dallas
002255384 700__ $$aLi, Bing$$iINSPIRE-00329518$$uHefei, CUST$$uMichigan U.
002255384 700__ $$aLi, Changqiao$$iINSPIRE-00512869$$uHefei, CUST
002255384 700__ $$aLi, Haifeng$$iINSPIRE-00219079$$uSUNY, Stony Brook
002255384 700__ $$aLi, Lei$$iINSPIRE-00358161$$uDuke U.
002255384 700__ $$aLi, Liang$$iINSPIRE-00300470$$uShanghai Jiao Tong U.
002255384 700__ $$aLi, Qi$$iINSPIRE-00439752$$uBeijing, Inst. High Energy Phys.
002255384 700__ $$aLi, Shu$$iINSPIRE-00231230$$uDuke U.
002255384 700__ $$aLi, Xingguo$$iINSPIRE-00388243$$uShanghai Jiao Tong U.
002255384 700__ $$aLi, Yichen$$iINSPIRE-00364274$$uSiegen U.
002255384 700__ $$aLiang, Zhijun$$iINSPIRE-00219122$$uBeijing, Inst. High Energy Phys.
002255384 700__ $$aLiberti, Barbara$$iINSPIRE-00219134$$uINFN, Rome
002255384 700__ $$aLiblong, Aaron$$iINSPIRE-00392999$$uToronto U.
002255384 700__ $$aLie, Ki$$iINSPIRE-00219158$$uIllinois U., Urbana
002255384 700__ $$aLiebal, Jessica$$iINSPIRE-00336627$$uBonn U.
002255384 700__ $$aLiebig, Wolfgang$$iINSPIRE-00219160$$uBergen U.
002255384 700__ $$aLimosani, Antonio$$iINSPIRE-00219183$$uSydney U.
002255384 700__ $$aLin, Simon$$iINSPIRE-00219207$$uTaiwan, Inst. Phys.
002255384 700__ $$aLin, Tai-Hua$$iINSPIRE-00368490$$uMainz U.
002255384 700__ $$aLindquist, Brian Edward$$iINSPIRE-00016188$$uSUNY, Stony Brook
002255384 700__ $$aLionti, Anthony Eric$$iINSPIRE-00443766$$uGeneva U.
002255384 700__ $$aLipeles, Elliot$$iINSPIRE-00102076$$uPennsylvania U.
002255384 700__ $$aLipniacka, Anna$$iINSPIRE-00219225$$uBergen U.
002255384 700__ $$aLisovyi, Mykhailo$$iINSPIRE-00172687$$uHeidelberg U.
002255384 700__ $$aLiss, Tony$$iINSPIRE-00102136$$uIllinois U., Urbana
002255384 700__ $$aLister, Alison$$iINSPIRE-00149260$$uBritish Columbia U.
002255384 700__ $$aLitke, Alan$$iINSPIRE-00219237$$uUC, Santa Cruz
002255384 700__ $$aLiu, Bo$$iINSPIRE-00354242$$uTaiwan, Inst. Phys.$$uShandong U.
002255384 700__ $$aLiu, Hao$$iINSPIRE-00407622$$uMichigan U.
002255384 700__ $$aLiu, Hongbin$$iINSPIRE-00445642$$uBrookhaven
002255384 700__ $$aLiu, Jian$$iINSPIRE-00381015$$uShandong U.
002255384 700__ $$aLiu, Jianbei$$iINSPIRE-00219262$$uHefei, CUST
002255384 700__ $$aLiu, Kun$$iINSPIRE-00337073$$uMarseille, CPPM
002255384 700__ $$aLiu, Lulu$$iINSPIRE-00287494$$uIllinois U., Urbana
002255384 700__ $$aLiu, Minghui$$iINSPIRE-00219274$$uHefei, CUST
002255384 700__ $$aLiu, Yanlin$$iINSPIRE-00436733$$uHefei, CUST
002255384 700__ $$aLiu, Yanwen$$iINSPIRE-00034400$$uHefei, CUST
002255384 700__ $$aLivan, Michele$$iINSPIRE-00102290$$uINFN, Pavia$$uPavia U.
002255384 700__ $$aLleres, Annick$$iINSPIRE-00300681$$uLPSC, Grenoble
002255384 700__ $$aLlorente Merino, Javier$$iINSPIRE-00236900$$uBeijing, Inst. High Energy Phys.
002255384 700__ $$aLloyd, Stephen$$iINSPIRE-00102350$$uQueen Mary, U. of London
002255384 700__ $$aLo, Cheuk Yee$$iINSPIRE-00436780$$uHong Kong U.
002255384 700__ $$aLo Sterzo, Francesco$$iINSPIRE-00286726$$uTaiwan, Inst. Phys.
002255384 700__ $$aLobodzinska, Ewelina Maria$$iINSPIRE-00172692$$uDESY
002255384 700__ $$aLoch, Peter$$iINSPIRE-00102360$$uArizona U.
002255384 700__ $$aLoebinger, Fred$$iINSPIRE-00102415$$uManchester U.
002255384 700__ $$aLoew, Kevin Michael$$iINSPIRE-00431566$$uBrandeis U.
002255384 700__ $$aLoginov, Andrey$$iINSPIRE-00025442$$uYale U.
002255384 700__ $$aLohse, Thomas$$iINSPIRE-00219316$$uHumboldt U., Berlin
002255384 700__ $$aLohwasser, Kristin$$iINSPIRE-00219328$$uDESY
002255384 700__ $$aLokajicek, Milos$$iINSPIRE-00278790$$uPrague, Inst. Phys.
002255384 700__ $$aLong, Brian Alexander$$iINSPIRE-00371005$$uBoston U.
002255384 700__ $$aLong, Jonathan David$$iINSPIRE-00349854$$uIllinois U., Urbana
002255384 700__ $$aLong, Robin Eamonn$$iINSPIRE-00219330$$uLancaster U.
002255384 700__ $$aLongo, Luigi$$iINSPIRE-00298644$$uINFN, Lecce$$uSalento U.
002255384 700__ $$aLooper, Kristina Anne$$iINSPIRE-00390156$$uOhio State U.
002255384 700__ $$aLopez, Jorge$$iINSPIRE-00511724$$uSanta Maria U., Valparaiso
002255384 700__ $$aLopez Mateos, David$$iINSPIRE-00219353$$uHarvard U., Phys. Dept.
002255384 700__ $$aLopez Paz, Ivan$$iINSPIRE-00372192$$uBarcelona, IFAE
002255384 700__ $$aLopez Solis, Alvaro$$iINSPIRE-00439816$$uParis U., VI-VII
002255384 700__ $$aLorenz, Jeanette$$iINSPIRE-00236914$$uMunich U.
002255384 700__ $$aLorenzo Martinez, Narei$$iINSPIRE-00236921$$uIndiana U.
002255384 700__ $$aLosada, Marta$$iINSPIRE-00102690$$uAntonio Narino U.
002255384 700__ $$aLösel, Philipp Jonathan$$iINSPIRE-00389527$$uMunich U.
002255384 700__ $$aLou, XinChou$$iINSPIRE-00102733$$uBeijing, Inst. High Energy Phys.
002255384 700__ $$aLounis, Abdenour$$iINSPIRE-00219420$$uOrsay, LAL
002255384 700__ $$aLove, Jeremy$$iINSPIRE-00007273$$uArgonne
002255384 700__ $$aLove, Peter$$iINSPIRE-00006364$$uLancaster U.
002255384 700__ $$aLu, Haonan$$iINSPIRE-00436841$$uHong Kong, Chinese U.
002255384 700__ $$aLu, Nan$$iINSPIRE-00378788$$uMichigan U.
002255384 700__ $$aLu, Yun-Ju$$iINSPIRE-00191837$$uTaiwan, Natl. Tsing Hua U.
002255384 700__ $$aLubatti, Henry$$iINSPIRE-00102893$$uWashington U., Seattle
002255384 700__ $$aLuci, Claudio$$iINSPIRE-00102930$$uINFN, Rome$$uRome U.
002255384 700__ $$aLucotte, Arnaud$$iINSPIRE-00102945$$uLPSC, Grenoble
002255384 700__ $$aLuedtke, Christian$$iINSPIRE-00418008$$uFreiburg U.
002255384 700__ $$aLuehring, Frederick$$iINSPIRE-00102988$$uIndiana U.
002255384 700__ $$aLukas, Wolfgang$$iINSPIRE-00332935$$uInnsbruck U.
002255384 700__ $$aLuminari, Lamberto$$iINSPIRE-00219493$$uINFN, Rome
002255384 700__ $$aLundberg, Olof$$iINSPIRE-00286734$$uStockholm U.$$uStockholm U., OKC
002255384 700__ $$aLund-Jensen, Bengt$$iINSPIRE-00103080$$uRoyal Inst. Tech., Stockholm
002255384 700__ $$aLuzi, Pierre Marc$$iINSPIRE-00442158$$uParis U., VI-VII
002255384 700__ $$aLynn, David$$iINSPIRE-00219523$$uBrookhaven
002255384 700__ $$aLysak, Roman$$iINSPIRE-00040995$$uPrague, Inst. Phys.
002255384 700__ $$aLytken, Else$$iINSPIRE-00040983$$uLund U.
002255384 700__ $$aLyubushkin, Vladimir$$iINSPIRE-00056876$$uDubna, JINR
002255384 700__ $$aMa, Hong$$iINSPIRE-00103432$$uBrookhaven
002255384 700__ $$aMa, Lian Liang$$iINSPIRE-00219535$$uShandong U.
002255384 700__ $$aMa, Yanhui$$iINSPIRE-00445756$$uShandong U.
002255384 700__ $$aMaccarrone, Giovanni$$iINSPIRE-00219559$$uFrascati
002255384 700__ $$aMacchiolo, Anna$$iINSPIRE-00219560$$uMunich, Max Planck Inst.
002255384 700__ $$aMacdonald, Calum Michael$$iINSPIRE-00389031$$uSheffield U.
002255384 700__ $$aMaček, Boštjan$$iINSPIRE-00219572$$uStefan Inst., Ljubljana
002255384 700__ $$aMachado Miguens, Joana$$iINSPIRE-00219584$$uPennsylvania U.$$uLisbon U., CFNUL
002255384 700__ $$aMadaffari, Daniele$$iINSPIRE-00358553$$uMarseille, CPPM
002255384 700__ $$aMadar, Romain$$iINSPIRE-00301124$$uClermont-Ferrand U.
002255384 700__ $$aMaddocks, Harvey Jonathan$$iINSPIRE-00349868$$uUppsala U., Inst. Theor. Phys.
002255384 700__ $$aMader, Wolfgang$$iINSPIRE-00103627$$uDresden, Tech. U.
002255384 700__ $$aMadsen, Alexander$$iINSPIRE-00333100$$uDESY
002255384 700__ $$aMaeda, Junpei$$iINSPIRE-00030940$$uKobe U.
002255384 700__ $$aMaeland, Steffen$$iINSPIRE-00389670$$uBergen U.
002255384 700__ $$aMaeno, Tadashi$$iINSPIRE-00219608$$uBrookhaven
002255384 700__ $$aMaevskiy, Artem$$iINSPIRE-00377096$$uMoscow State U.
002255384 700__ $$aMagradze, Erekle$$iINSPIRE-00219638$$uGottingen U., II. Phys. Inst.
002255384 700__ $$aMahlstedt, Joern$$iINSPIRE-00291935$$uFOM, Amsterdam
002255384 700__ $$aMaiani, Camilla$$iINSPIRE-00219665$$uOrsay, LAL
002255384 700__ $$aMaidantchik, Carmen$$iINSPIRE-00219677$$uRio de Janeiro Federal U.
002255384 700__ $$aMaier, Andreas Alexander$$iINSPIRE-00372204$$uMunich, Max Planck Inst.
002255384 700__ $$aMaier, Thomas$$iINSPIRE-00393059$$uMunich U.
002255384 700__ $$aMaio, Amélia$$iINSPIRE-00219689$$uLIP, Lisbon$$uLisbon U., CFNUL
002255384 700__ $$aMajewski, Stephanie$$iINSPIRE-00041779$$uOregon U.
002255384 700__ $$aMakida, Yasuhiro$$iINSPIRE-00219690$$uKEK, Tsukuba
002255384 700__ $$aMakovec, Nikola$$iINSPIRE-00006510$$uOrsay, LAL
002255384 700__ $$aMalaescu, Bogdan$$iINSPIRE-00144706$$uParis U., VI-VII
002255384 700__ $$aMalecki, Pawel$$iINSPIRE-00219707$$uCracow, INP
002255384 700__ $$aMaleev, Victor$$iINSPIRE-00219720$$uSt. Petersburg, INP
002255384 700__ $$aMalek, Fairouz$$iINSPIRE-00104125$$uLPSC, Grenoble
002255384 700__ $$aMallik, Usha$$iINSPIRE-00104172$$uIowa U.
002255384 700__ $$aMalon, David$$iINSPIRE-00219732$$uArgonne
002255384 700__ $$aMalone, Claire$$iINSPIRE-00439828$$uCambridge U.
002255384 700__ $$aMaltezos, Stavros$$iINSPIRE-00219744$$uNatl. Tech. U., Athens
002255384 700__ $$aMalyukov, Sergei$$iINSPIRE-00219768$$uCERN
002255384 700__ $$aMamuzic, Judita$$iINSPIRE-00219793$$uValencia U., IFIC
002255384 700__ $$aMancini, Giada$$iINSPIRE-00389811$$uFrascati
002255384 700__ $$aMandelli, Luciano$$iINSPIRE-00219806$$uINFN, Milan
002255384 700__ $$aMandić, Igor$$iINSPIRE-00219818$$uStefan Inst., Ljubljana
002255384 700__ $$aManeira, José$$iINSPIRE-00219831$$uLIP, Lisbon$$uLisbon U., CFNUL
002255384 700__ $$aManhaes de Andrade Filho, Luciano$$iINSPIRE-00236954$$uJuiz de Fora U.
002255384 700__ $$aManjarres Ramos, Joany$$iINSPIRE-00332115$$uYork U., Canada
002255384 700__ $$aMann, Alexander$$iINSPIRE-00219853$$uMunich U.
002255384 700__ $$aManousos, Athanasios$$iINSPIRE-00508922$$uCERN
002255384 700__ $$aMansoulie, Bruno$$iINSPIRE-00104458$$uIRFU, Saclay
002255384 700__ $$aMansour, Jason Dhia$$iINSPIRE-00281038$$uBeijing, Inst. High Energy Phys.
002255384 700__ $$aMantifel, Rodger$$iINSPIRE-00332945$$uMcGill U.
002255384 700__ $$aMantoani, Matteo$$iINSPIRE-00384468$$uGottingen U., II. Phys. Inst.
002255384 700__ $$aManzoni, Stefano$$iINSPIRE-00436885$$uINFN, Milan$$uMilan U.
002255384 700__ $$aMapelli, Livio$$iINSPIRE-00219888$$uCERN
002255384 700__ $$aMarceca, Gino$$iINSPIRE-00443931$$uBuenos Aires U.
002255384 700__ $$aMarch, Luis$$iINSPIRE-00219890$$uGeneva U.
002255384 700__ $$aMarchiori, Giovanni$$iINSPIRE-00041986$$uParis U., VI-VII
002255384 700__ $$aMarcisovsky, Michal$$iINSPIRE-00021119$$uPrague, Inst. Phys.
002255384 700__ $$aMarjanovic, Marija$$iINSPIRE-00355110$$uClermont-Ferrand U.
002255384 700__ $$aMarley, Daniel$$iINSPIRE-00407608$$uMichigan U.
002255384 700__ $$aMarroquim, Fernando$$iINSPIRE-00195269$$uRio de Janeiro Federal U.
002255384 700__ $$aMarsden, Stephen Philip$$iINSPIRE-00345603$$uManchester U.
002255384 700__ $$aMarshall, Zach$$iINSPIRE-00219927$$uLBL, Berkeley
002255384 700__ $$aMartensson, Mikael$$iINSPIRE-00530554$$uUppsala U., Inst. Theor. Phys.
002255384 700__ $$aMarti-Garcia, Salvador$$iINSPIRE-00050327$$uValencia U., IFIC
002255384 700__ $$aMartin, Christopher Blake$$iINSPIRE-00374510$$uOhio State U.
002255384 700__ $$aMartin, Tim$$iINSPIRE-00219969$$uWarwick U.
002255384 700__ $$aMartin, Victoria Jane$$iINSPIRE-00105165$$uEdinburgh U.
002255384 700__ $$aMartin dit Latour, Bertrand$$iINSPIRE-00001472$$uBergen U.
002255384 700__ $$aMartinez, Mario$$iINSPIRE-00105204$$uBarcelona, IFAE$$uICREA, Barcelona
002255384 700__ $$aMartinez Outschoorn, Verena$$iINSPIRE-00256761$$uIllinois U., Urbana
002255384 700__ $$aMartin-Haugh, Stewart$$iINSPIRE-00236968$$uRutherford
002255384 700__ $$aMartoiu, Victor Sorin$$iINSPIRE-00388336$$uBucharest, IFIN-HH
002255384 700__ $$aMartyniuk, Alex$$iINSPIRE-00219970$$uUniversity Coll. London
002255384 700__ $$aMarzin, Antoine$$iINSPIRE-00220006$$uOklahoma U.
002255384 700__ $$aMasetti, Lucia$$iINSPIRE-00220018$$uMainz U.
002255384 700__ $$aMashimo, Tetsuro$$iINSPIRE-00220020$$uTokyo U., ICEPP
002255384 700__ $$aMashinistov, Ruslan$$iINSPIRE-00220031$$uLebedev Inst.
002255384 700__ $$aMasik, Jiri$$iINSPIRE-00220043$$uManchester U.
002255384 700__ $$aMaslennikov, Alexey$$iINSPIRE-00220055$$uNovosibirsk State U.$$uNovosibirsk, IYF
002255384 700__ $$aMassa, Lorenzo$$iINSPIRE-00388313$$uINFN, Rome$$uRome U., Tor Vergata
002255384 700__ $$aMastrandrea, Paolo$$iINSPIRE-00030630$$uAnnecy, LAPP
002255384 700__ $$aMastroberardino, Anna$$iINSPIRE-00172288$$uINFN, Cosenza$$uCalabria U.
002255384 700__ $$aMasubuchi, Tatsuya$$iINSPIRE-00030446$$uTokyo U., ICEPP
002255384 700__ $$aMättig, Peter$$iINSPIRE-00105833$$uWuppertal U.
002255384 700__ $$aMaurer, Julien$$iINSPIRE-00236977$$uBucharest, IFIN-HH
002255384 700__ $$aMaxfield, Stephen$$iINSPIRE-00105929$$uLiverpool U.
002255384 700__ $$aMaximov, Dmitriy$$iINSPIRE-00236989$$uNovosibirsk State U.$$uNovosibirsk, IYF
002255384 700__ $$aMazini, Rachid$$iINSPIRE-00220110$$uTaiwan, Inst. Phys.
002255384 700__ $$aMaznas, Ioannis$$iINSPIRE-00525014$$uAristotle U., Thessaloniki
002255384 700__ $$aMazza, Simone Michele$$iINSPIRE-00386351$$uINFN, Milan$$uMilan U.
002255384 700__ $$aMc Fadden, Neil Christopher$$iINSPIRE-00439697$$uNew Mexico U.
002255384 700__ $$aMc Goldrick, Garrin$$iINSPIRE-00349874$$uToronto U.
002255384 700__ $$aMc Kee, Shawn Patrick$$iINSPIRE-00260714$$uMichigan U.
002255384 700__ $$aMcCarn, Allison$$iINSPIRE-00220122$$uMichigan U.
002255384 700__ $$aMcCarthy, Robert$$iINSPIRE-00106112$$uSUNY, Stony Brook
002255384 700__ $$aMcCarthy, Tom$$iINSPIRE-00220136$$uMunich, Max Planck Inst.
002255384 700__ $$aMcClymont, Laurie$$iINSPIRE-00439886$$uUniversity Coll. London
002255384 700__ $$aMcDonald, Emily$$iINSPIRE-00507462$$uMelbourne U.
002255384 700__ $$aMcfayden, Josh$$iINSPIRE-00231570$$uUniversity Coll. London
002255384 700__ $$aMchedlidze, Gvantsa$$iINSPIRE-00306035$$uGottingen U., II. Phys. Inst.
002255384 700__ $$aMcMahon, Steve$$iINSPIRE-00220148$$uRutherford
002255384 700__ $$aMcNamara, Peter Charles$$iINSPIRE-00535046$$uMelbourne U.
002255384 700__ $$aMcPherson, Robert$$iINSPIRE-00106476$$uVictoria U.$$uIPP, Canada
002255384 700__ $$aMeehan, Samuel$$iINSPIRE-00298342$$uWashington U., Seattle
002255384 700__ $$aMegy, Theo Jean$$iINSPIRE-00548858$$uFreiburg U.
002255384 700__ $$aMehlhase, Sascha$$iINSPIRE-00220289$$uMunich U.
002255384 700__ $$aMehta, Andrew$$iINSPIRE-00300183$$uLiverpool U.
002255384 700__ $$aMeideck, Thomas$$iINSPIRE-00535671$$uLPSC, Grenoble
002255384 700__ $$aMeier, Karlheinz$$iINSPIRE-00106610$$uKirchhoff Inst. Phys.
002255384 700__ $$aMeineck, Christian$$iINSPIRE-00334493$$uMunich U.
002255384 700__ $$aMeirose, Bernhard$$iINSPIRE-00220290$$uTexas U., Dallas
002255384 700__ $$aMelini, Davide$$iINSPIRE-00442240$$uValencia U., IFIC$$uCAFPE, Granada
002255384 700__ $$aMellado Garcia, Bruce Rafael$$iINSPIRE-00005240$$uWitwatersrand U.
002255384 700__ $$aMelo, Matej$$iINSPIRE-00508306$$uComenius U.
002255384 700__ $$aMeloni, Federico$$iINSPIRE-00286780$$uBern U., LHEP
002255384 700__ $$aMenary, Stephen Burns$$iINSPIRE-00529690$$uManchester U.
002255384 700__ $$aMeng, Lingxin$$iINSPIRE-00533043$$uLiverpool U.
002255384 700__ $$aMeng, Xiangting$$iINSPIRE-00535687$$uMichigan U.
002255384 700__ $$aMengarelli, Alberto$$iINSPIRE-00231636$$uINFN, Bologna$$uBologna U.
002255384 700__ $$aMenke, Sven$$iINSPIRE-00106910$$uMunich, Max Planck Inst.
002255384 700__ $$aMeoni, Evelin$$iINSPIRE-00220314$$uTufts U.
002255384 700__ $$aMergelmeyer, Sebastian$$iINSPIRE-00239978$$uHumboldt U., Berlin
002255384 700__ $$aMermod, Philippe$$iINSPIRE-00220326$$uGeneva U.
002255384 700__ $$aMerola, Leonardo$$iINSPIRE-00107018$$uINFN, Naples$$uNaples U.
002255384 700__ $$aMeroni, Chiara$$iINSPIRE-00107020$$uINFN, Milan
002255384 700__ $$aMerritt, Frank$$iINSPIRE-00107035$$uChicago U., EFI
002255384 700__ $$aMessina, Andrea$$iINSPIRE-00220338$$uINFN, Rome$$uRome U.
002255384 700__ $$aMetcalfe, Jessica$$iINSPIRE-00220340$$uArgonne
002255384 700__ $$aMete, Alaettin Serhan$$iINSPIRE-00220356$$uUC, Irvine
002255384 700__ $$aMeyer, Christopher$$iINSPIRE-00237016$$uPennsylvania U.
002255384 700__ $$aMeyer, Jean-Pierre$$iINSPIRE-00220370$$uIRFU, Saclay
002255384 700__ $$aMeyer, Jochen$$iINSPIRE-00220381$$uFOM, Amsterdam
002255384 700__ $$aMeyer Zu Theenhausen, Hanno$$iINSPIRE-00413137$$uKirchhoff Inst. Phys.
002255384 700__ $$aMiano, Fabrizio$$iINSPIRE-00452972$$uSussex U.
002255384 700__ $$aMiddleton, Robin$$iINSPIRE-00107429$$uRutherford
002255384 700__ $$aMiglioranzi, Silvia$$iINSPIRE-00320164$$uINFN, Genoa$$uGenoa U.
002255384 700__ $$aMijović, Liza$$iINSPIRE-00220450$$uEdinburgh U.
002255384 700__ $$aMikenberg, Giora$$iINSPIRE-00107520$$uWeizmann Inst.
002255384 700__ $$aMikestikova, Marcela$$iINSPIRE-00220462$$uPrague, Inst. Phys.
002255384 700__ $$aMikuž, Marko$$iINSPIRE-00220474$$uStefan Inst., Ljubljana
002255384 700__ $$aMilesi, Marco$$iINSPIRE-00396260$$uMelbourne U.
002255384 700__ $$aMilic, Adriana$$iINSPIRE-00371740$$uBrookhaven
002255384 700__ $$aMiller, David$$iINSPIRE-00023943$$uChicago U., EFI
002255384 700__ $$aMills, Corrinne$$iINSPIRE-00226703$$uEdinburgh U.
002255384 700__ $$aMilov, Alexander$$iINSPIRE-00056451$$uWeizmann Inst.
002255384 700__ $$aMilstead, David$$iINSPIRE-00220498$$uStockholm U.$$uStockholm U., OKC
002255384 700__ $$aMinaenko, Andrey$$iINSPIRE-00220511$$uSerpukhov, IHEP
002255384 700__ $$aMinami, Yuto$$iINSPIRE-00378210$$uTokyo U., ICEPP
002255384 700__ $$aMinashvili, Irakli$$iINSPIRE-00306048$$uDubna, JINR
002255384 700__ $$aMincer, Allen$$iINSPIRE-00107849$$uNew York U.
002255384 700__ $$aMindur, Bartosz$$iINSPIRE-00220535$$uAGH-UST, Cracow
002255384 700__ $$aMineev, Mikhail$$iINSPIRE-00220541$$uDubna, JINR
002255384 700__ $$aMinegishi, Yuji$$iINSPIRE-00525023$$uTokyo U., ICEPP
002255384 700__ $$aMing, Yao$$iINSPIRE-00220553$$uWisconsin U., Madison
002255384 700__ $$aMir, Lluisa-Maria$$iINSPIRE-00220565$$uBarcelona, IFAE
002255384 700__ $$aMistry, Khilesh$$iINSPIRE-00403633$$uPennsylvania U.
002255384 700__ $$aMitani, Takashi$$iINSPIRE-00342753$$uWaseda U.
002255384 700__ $$aMitrevski, Jovan$$iINSPIRE-00038843$$uMunich U.
002255384 700__ $$aMitsou, Vasiliki A$$iINSPIRE-00108110$$uValencia U., IFIC
002255384 700__ $$aMiucci, Antonio$$iINSPIRE-00362129$$uBern U., LHEP
002255384 700__ $$aMiyagawa, Paul$$iINSPIRE-00049051$$uSheffield U.
002255384 700__ $$aMizukami, Atsushi$$iINSPIRE-00525035$$uKEK, Tsukuba
002255384 700__ $$aMjörnmark, Jan-Ulf$$iINSPIRE-00220668$$uLund U.
002255384 700__ $$aMlynarikova, Michaela$$iINSPIRE-00525048$$uCharles U.
002255384 700__ $$aMoa, Torbjoern$$iINSPIRE-00108216$$uStockholm U.$$uStockholm U., OKC
002255384 700__ $$aMochizuki, Kazuya$$iINSPIRE-00359682$$uMontreal U.
002255384 700__ $$aMogg, Philipp$$iINSPIRE-00540560$$uFreiburg U.
002255384 700__ $$aMohapatra, Soumya$$iINSPIRE-00231736$$uNevis Labs, Columbia U.
002255384 700__ $$aMolander, Simon$$iINSPIRE-00342710$$uStockholm U.$$uStockholm U., OKC
002255384 700__ $$aMoles-Valls, Regina$$iINSPIRE-00220705$$uBonn U.
002255384 700__ $$aMonden, Ryutaro$$iINSPIRE-00417891$$uKyoto U.
002255384 700__ $$aMondragon, Matthew Craig$$iINSPIRE-00383685$$uMichigan State U.
002255384 700__ $$aMönig, Klaus$$iINSPIRE-00108503$$uDESY
002255384 700__ $$aMonk, James$$iINSPIRE-00046573$$uBohr Inst.
002255384 700__ $$aMonnier, Emmanuel$$iINSPIRE-00326813$$uMarseille, CPPM
002255384 700__ $$aMontalbano, Alyssa$$iINSPIRE-00386528$$uSUNY, Stony Brook
002255384 700__ $$aMontejo Berlingen, Javier$$iINSPIRE-00286815$$uCERN
002255384 700__ $$aMonticelli, Fernando$$iINSPIRE-00220717$$uLa Plata U.
002255384 700__ $$aMonzani, Simone$$iINSPIRE-00231765$$uINFN, Milan$$uMilan U.
002255384 700__ $$aMoore, Roger$$iINSPIRE-00038831$$uAlberta U.
002255384 700__ $$aMorange, Nicolas$$iINSPIRE-00231774$$uOrsay, LAL
002255384 700__ $$aMoreno, Deywis$$iINSPIRE-00220759$$uAntonio Narino U.
002255384 700__ $$aMoreno Llácer, María$$iINSPIRE-00332523$$uGottingen U., II. Phys. Inst.
002255384 700__ $$aMorettini, Paolo$$iINSPIRE-00220772$$uINFN, Genoa
002255384 700__ $$aMorgenstern, Stefanie$$iINSPIRE-00511715$$uCERN
002255384 700__ $$aMori, Daniel$$iINSPIRE-00410854$$uSimon Fraser U.
002255384 700__ $$aMori, Tatsuya$$iINSPIRE-00399773$$uTokyo U., ICEPP
002255384 700__ $$aMorii, Masahiro$$iINSPIRE-00108914$$uHarvard U., Phys. Dept.
002255384 700__ $$aMorinaga, Masahiro$$iINSPIRE-00381150$$uTokyo U., ICEPP
002255384 700__ $$aMorisbak, Vanja$$iINSPIRE-00379515$$uOslo U.
002255384 700__ $$aMorley, Anthony Keith$$iINSPIRE-00201749$$uSydney U.
002255384 700__ $$aMornacchi, Giuseppe$$iINSPIRE-00220784$$uCERN
002255384 700__ $$aMorris, John$$iINSPIRE-00220796$$uQueen Mary, U. of London
002255384 700__ $$aMorvaj, Ljiljana$$iINSPIRE-00237030$$uSUNY, Stony Brook
002255384 700__ $$aMoschovakos, Paris$$iINSPIRE-00529702$$uNatl. Tech. U., Athens
002255384 700__ $$aMosidze, Maia$$iINSPIRE-00306063$$uTbilisi State U.
002255384 700__ $$aMoss, Harry James$$iINSPIRE-00449187$$uSheffield U.
002255384 700__ $$aMoss, Josh$$iINSPIRE-00220808$$uSLAC$$uCal State, Sacramento
002255384 700__ $$aMotohashi, Kazuki$$iINSPIRE-00372213$$uTokyo Inst. Tech.
002255384 700__ $$aMount, Richard$$iINSPIRE-00059638$$uSLAC
002255384 700__ $$aMountricha, Eleni$$iINSPIRE-00220810$$uBrookhaven
002255384 700__ $$aMoyse, Edward$$iINSPIRE-00220821$$uMassachusetts U., Amherst
002255384 700__ $$aMuanza, Steve$$iINSPIRE-00109389$$uMarseille, CPPM
002255384 700__ $$aMudd, Richard$$iINSPIRE-00338755$$uBirmingham U.
002255384 700__ $$aMueller, Felix$$iINSPIRE-00220833$$uMunich, Max Planck Inst.
002255384 700__ $$aMueller, James$$iINSPIRE-00109443$$uPittsburgh U.
002255384 700__ $$aMueller, Ralph Soeren Peter$$iINSPIRE-00389964$$uMunich U.
002255384 700__ $$aMuenstermann, Daniel$$iINSPIRE-00220841$$uLancaster U.
002255384 700__ $$aMullen, Paul$$iINSPIRE-00367030$$uGlasgow U.
002255384 700__ $$aMullier, Geoffrey$$iINSPIRE-00407702$$uBern U., LHEP
002255384 700__ $$aMunoz Sanchez, Francisca Javiela$$iINSPIRE-00017703$$uManchester U.
002255384 700__ $$aMurray, Bill$$iINSPIRE-00109809$$uWarwick U.$$uRutherford
002255384 700__ $$aMusheghyan, Haykuhi$$iINSPIRE-00367045$$uGottingen U., II. Phys. Inst.
002255384 700__ $$aMuškinja, Miha$$iINSPIRE-00452370$$uStefan Inst., Ljubljana
002255384 700__ $$aMyagkov, Alexey$$iINSPIRE-00220926$$uSerpukhov, IHEP$$uMoscow, MIPT
002255384 700__ $$aMyska, Miroslav$$iINSPIRE-00220932$$uPrague, Tech. U.
002255384 700__ $$aNachman, Benjamin Philip$$iINSPIRE-00376212$$uLBL, Berkeley
002255384 700__ $$aNackenhorst, Olaf$$iINSPIRE-00286840$$uGeneva U.
002255384 700__ $$aNagai, Koichi$$iINSPIRE-00220956$$uOxford U.
002255384 700__ $$aNagai, Ryo$$iINSPIRE-00288829$$uKEK, Tsukuba$$uOchanomizu U.
002255384 700__ $$aNagano, Kunihiro$$iINSPIRE-00110036$$uKEK, Tsukuba
002255384 700__ $$aNagasaka, Yasushi$$iINSPIRE-00220968$$uHiroshima Inst. Tech.
002255384 700__ $$aNagata, Kazuki$$iINSPIRE-00379571$$uTsukuba U.
002255384 700__ $$aNagel, Martin$$iINSPIRE-00030110$$uFreiburg U.
002255384 700__ $$aNagy, Elemer$$iINSPIRE-00110088$$uMarseille, CPPM
002255384 700__ $$aNairz, Armin Michael$$iINSPIRE-00220970$$uCERN
002255384 700__ $$aNakahama, Yu$$iINSPIRE-00286861$$uNagoya U.
002255384 700__ $$aNakamura, Koji$$iINSPIRE-00047824$$uKEK, Tsukuba
002255384 700__ $$aNakamura, Tomoaki$$iINSPIRE-00110240$$uTokyo U., ICEPP
002255384 700__ $$aNakano, Itsuo$$iINSPIRE-00040923$$uOkayama U.
002255384 700__ $$aNaranjo Garcia, Roger Felipe$$iINSPIRE-00381918$$uDESY
002255384 700__ $$aNarayan, Rohin$$iINSPIRE-00237051$$uTexas U.
002255384 700__ $$aNarrias Villar, Daniel Isaac$$iINSPIRE-00390052$$uKirchhoff Inst. Phys.
002255384 700__ $$aNaryshkin, Iouri$$iINSPIRE-00439969$$uSt. Petersburg, INP
002255384 700__ $$aNaumann, Thomas$$iINSPIRE-00110648$$uDESY
002255384 700__ $$aNavarro, Gabriela$$iINSPIRE-00221017$$uAntonio Narino U.
002255384 700__ $$aNayyar, Ruchika$$iINSPIRE-00301151$$uArizona U.
002255384 700__ $$aNeal, Homer$$iINSPIRE-00300519$$uMichigan U.
002255384 700__ $$aNechaeva, Polina$$iINSPIRE-00221047$$uLebedev Inst.
002255384 700__ $$aNeep, Thomas James$$iINSPIRE-00286870$$uIRFU, Saclay
002255384 700__ $$aNegri, Andrea$$iINSPIRE-00306082$$uINFN, Pavia$$uPavia U.
002255384 700__ $$aNegrini, Matteo$$iINSPIRE-00054399$$uINFN, Bologna
002255384 700__ $$aNektarijevic, Snezana$$iINSPIRE-00231852$$uNIKHEF, Amsterdam
002255384 700__ $$aNellist, Clara$$iINSPIRE-00304438$$uOrsay, LAL
002255384 700__ $$aNelson, Andrew$$iINSPIRE-00221060$$uUC, Irvine
002255384 700__ $$aNemecek, Stanislav$$iINSPIRE-00110909$$uPrague, Inst. Phys.
002255384 700__ $$aNemethy, Peter$$iINSPIRE-00321590$$uNew York U.
002255384 700__ $$aNepomuceno, Andre Asevedo$$iINSPIRE-00221072$$uRio de Janeiro Federal U.
002255384 700__ $$aNessi, Marzio$$iINSPIRE-00221084$$uCERN$$uGeneva U.
002255384 700__ $$aNeubauer, Mark$$iINSPIRE-00110982$$uIllinois U., Urbana
002255384 700__ $$aNeumann, Manuel$$iINSPIRE-00288618$$uWuppertal U.
002255384 700__ $$aNeves, Ricardo$$iINSPIRE-00221104$$uNew York U.
002255384 700__ $$aNevski, Pavel$$iINSPIRE-00221110$$uBrookhaven
002255384 700__ $$aNewman, Paul$$iINSPIRE-00111158$$uBirmingham U.
002255384 700__ $$aNg, Tsz Yu$$iINSPIRE-00536671$$uHong Kong U. Sci. Tech.
002255384 700__ $$aNguyen Manh, Tuan$$iINSPIRE-00417989$$uMontreal U.
002255384 700__ $$aNickerson, Richard$$iINSPIRE-00221121$$uOxford U.
002255384 700__ $$aNicolaidou, Rosy$$iINSPIRE-00216944$$uIRFU, Saclay
002255384 700__ $$aNielsen, Jason$$iINSPIRE-00111400$$uUC, Santa Cruz
002255384 700__ $$aNikolaenko, Vladimir$$iINSPIRE-00231894$$uSerpukhov, IHEP$$uMoscow, MIPT
002255384 700__ $$aNikolic-Audit, Irena$$iINSPIRE-00306103$$uParis U., VI-VII
002255384 700__ $$aNikolopoulos, Konstantinos$$iINSPIRE-00221145$$uBirmingham U.
002255384 700__ $$aNilsen, Jon Kerr$$iINSPIRE-00393094$$uOslo U.
002255384 700__ $$aNilsson, Paul$$iINSPIRE-00221150$$uBrookhaven
002255384 700__ $$aNinomiya, Yoichi$$iINSPIRE-00231907$$uTokyo U., ICEPP
002255384 700__ $$aNisati, Aleandro$$iINSPIRE-00221160$$uINFN, Rome
002255384 700__ $$aNishu, Nishu$$iINSPIRE-00311000$$uTsinghua U., Beijing
002255384 700__ $$aNisius, Richard$$iINSPIRE-00111714$$uMunich, Max Planck Inst.
002255384 700__ $$aNobe, Takuya$$iINSPIRE-00286888$$uTokyo U., ICEPP
002255384 700__ $$aNoguchi, Yohei$$iINSPIRE-00534663$$uKyoto U.
002255384 700__ $$aNomachi, Masaharu$$iINSPIRE-00111877$$uOsaka U.
002255384 700__ $$aNomidis, Ioannis$$iINSPIRE-00221178$$uCarleton U.
002255384 700__ $$aNomura, Marcelo Ayumu$$iINSPIRE-00535055$$uBrookhaven
002255384 700__ $$aNooney, Tamsin$$iINSPIRE-00389111$$uQueen Mary, U. of London
002255384 700__ $$aNordberg, Markus$$iINSPIRE-00111954$$uCERN
002255384 700__ $$aNorjoharuddeen, Nurfikri$$iINSPIRE-00442949$$uOxford U.
002255384 700__ $$aNovgorodova, Olga$$iINSPIRE-00285705$$uDresden, Tech. U.
002255384 700__ $$aNowak, Sebastian$$iINSPIRE-00390105$$uMunich, Max Planck Inst.
002255384 700__ $$aNozaki, Mitsuaki$$iINSPIRE-00226787$$uKEK, Tsukuba
002255384 700__ $$aNozka, Libor$$iINSPIRE-00152530$$uPalacky U.
002255384 700__ $$aNtekas, Konstantinos$$iINSPIRE-00349891$$uUC, Irvine
002255384 700__ $$aNurse, Emily$$iINSPIRE-00052439$$uUniversity Coll. London
002255384 700__ $$aNuti, Francesco$$iINSPIRE-00346170$$uMelbourne U.
002255384 700__ $$aO'Neil, Dugan$$iINSPIRE-00112324$$uSimon Fraser U.
002255384 700__ $$aO'Rourke, Abigail Alexandra$$iINSPIRE-00431615$$uDESY
002255384 700__ $$aO'Shea, Val$$iINSPIRE-00112370$$uGlasgow U.
002255384 700__ $$aOakham, Gerald$$iINSPIRE-00112393$$uCarleton U.$$uTRIUMF
002255384 700__ $$aOberlack, Horst$$iINSPIRE-00112415$$uMunich, Max Planck Inst.
002255384 700__ $$aObermann, Theresa$$iINSPIRE-00362697$$uBonn U.
002255384 700__ $$aOcariz, Jose$$iINSPIRE-00112459$$uParis U., VI-VII
002255384 700__ $$aOchi, Atsuhiko$$iINSPIRE-00112469$$uKobe U.
002255384 700__ $$aOchoa, Ines$$iINSPIRE-00335577$$uNevis Labs, Columbia U.
002255384 700__ $$aOchoa-Ricoux, Juan Pedro$$iINSPIRE-00404468$$uChile U., Catolica
002255384 700__ $$aOda, Susumu$$iINSPIRE-00036017$$uKyushu U.
002255384 700__ $$aOdaka, Shigeru$$iINSPIRE-00221251$$uKEK, Tsukuba
002255384 700__ $$aOgren, Harold$$iINSPIRE-00112633$$uIndiana U.
002255384 700__ $$aOh, Alexander$$iINSPIRE-00320498$$uManchester U.
002255384 700__ $$aOh, Seog$$iINSPIRE-00112667$$uDuke U.
002255384 700__ $$aOhm, Christian$$iINSPIRE-00221275$$uLBL, Berkeley
002255384 700__ $$aOhman, Henrik$$iINSPIRE-00342728$$uUppsala U., Inst. Theor. Phys.
002255384 700__ $$aOide, Hideyuki$$iINSPIRE-00379657$$uINFN, Genoa$$uGenoa U.
002255384 700__ $$aOkawa, Hideki$$iINSPIRE-00221308$$uTsukuba U.
002255384 700__ $$aOkumura, Yasuyuki$$iINSPIRE-00221310$$uTokyo U., ICEPP
002255384 700__ $$aOkuyama, Toyonobu$$iINSPIRE-00226798$$uKEK, Tsukuba
002255384 700__ $$aOlariu, Albert$$iINSPIRE-00237105$$uBucharest, IFIN-HH
002255384 700__ $$aOleiro Seabra, Luis Filipe$$iINSPIRE-00514541$$uLIP, Lisbon
002255384 700__ $$aOlivares Pino, Sebastian Andres$$iINSPIRE-00286912$$uEdinburgh U.
002255384 700__ $$aOliveira Damazio, Denis$$iINSPIRE-00221335$$uBrookhaven
002255384 700__ $$aOlszewski, Andrzej$$iINSPIRE-00256380$$uCracow, INP
002255384 700__ $$aOlszowska, Jolanta$$iINSPIRE-00221360$$uCracow, INP
002255384 700__ $$aOnofre, António$$iINSPIRE-00221372$$uLIP, Lisbon$$uMinho U.
002255384 700__ $$aOnogi, Kouta$$iINSPIRE-00415586$$uNagoya U.
002255384 700__ $$aOnyisi, Peter$$iINSPIRE-00057397$$uTexas U.
002255384 700__ $$aOreglia, Mark$$iINSPIRE-00113317$$uChicago U., EFI
002255384 700__ $$aOren, Yona$$iINSPIRE-00221389$$uTel Aviv U.
002255384 700__ $$aOrestano, Domizia$$iINSPIRE-00113321$$uINFN, Rome$$uRome III U.
002255384 700__ $$aOrlando, Nicola$$iINSPIRE-00286920$$uHong Kong U.
002255384 700__ $$aOrr, Robert$$iINSPIRE-00113411$$uToronto U.
002255384 700__ $$aOsculati, Bianca$$iINSPIRE-00221407$$uINFN, Genoa$$uGenoa U.
002255384 700__ $$aOspanov, Rustem$$iINSPIRE-00029272$$uManchester U.
002255384 700__ $$aOtero y Garzon, Gustavo$$iINSPIRE-00046137$$uBuenos Aires U.
002255384 700__ $$aOtono, Hidetoshi$$iINSPIRE-00348488$$uKyushu U.
002255384 700__ $$aOuchrif, Mohamed$$iINSPIRE-00232012$$uOujda U.
002255384 700__ $$aOuld-Saada, Farid$$iINSPIRE-00221439$$uOslo U.
002255384 700__ $$aOuraou, Ahmimed$$iINSPIRE-00221444$$uIRFU, Saclay
002255384 700__ $$aOussoren, Koen Pieter$$iINSPIRE-00342930$$uFOM, Amsterdam
002255384 700__ $$aOuyang, Qun$$iINSPIRE-00221456$$uBeijing, Inst. High Energy Phys.
002255384 700__ $$aOwen, Mark$$iINSPIRE-00007985$$uGlasgow U.
002255384 700__ $$aOwen, Rhys Edward$$iINSPIRE-00390165$$uBirmingham U.
002255384 700__ $$aOzcan, Veysi Erkcan$$iINSPIRE-00221480$$uBogazici U.
002255384 700__ $$aOzturk, Nurcan$$iINSPIRE-00026861$$uTexas U., Arlington
002255384 700__ $$aPachal, Katherine$$iINSPIRE-00337371$$uSimon Fraser U.
002255384 700__ $$aPacheco Pages, Andres$$iINSPIRE-00221495$$uBarcelona, IFAE
002255384 700__ $$aPacheco Rodriguez, Laura$$iINSPIRE-00511732$$uIRFU, Saclay
002255384 700__ $$aPadilla Aranda, Cristobal$$iINSPIRE-00306128$$uBarcelona, IFAE
002255384 700__ $$aPagan Griso, Simone$$iINSPIRE-00022647$$uLBL, Berkeley
002255384 700__ $$aPaganini, Michela$$iINSPIRE-00452535$$uYale U.
002255384 700__ $$aPaige, Frank$$iINSPIRE-00221520$$uBrookhaven
002255384 700__ $$aPais, Preema$$iINSPIRE-00237142$$uMassachusetts U., Amherst
002255384 700__ $$aPalacino, Gabriel$$iINSPIRE-00237152$$uIndiana U.
002255384 700__ $$aPalazzo, Serena$$iINSPIRE-00511747$$uINFN, Cosenza$$uCalabria U.
002255384 700__ $$aPalestini, Sandro$$iINSPIRE-00221549$$uCERN
002255384 700__ $$aPalka, Marek$$iINSPIRE-00371751$$uJagiellonian U.
002255384 700__ $$aPallin, Dominique$$iINSPIRE-00221552$$uClermont-Ferrand U.
002255384 700__ $$aPanagiotopoulou, Evgenia$$iINSPIRE-00232057$$uNatl. Tech. U., Athens
002255384 700__ $$aPanagoulias, Ilias$$iINSPIRE-00185557$$uNatl. Tech. U., Athens
002255384 700__ $$aPandini, Carlo Enrico$$iINSPIRE-00388516$$uParis U., VI-VII
002255384 700__ $$aPanduro Vazquez, William$$iINSPIRE-00042480$$uRoyal Holloway, U. of London
002255384 700__ $$aPani, Priscilla$$iINSPIRE-00291943$$uCERN
002255384 700__ $$aPanitkin, Sergey$$iINSPIRE-00114270$$uBrookhaven
002255384 700__ $$aPantea, Dan$$iINSPIRE-00114319$$uBucharest, IFIN-HH
002255384 700__ $$aPaolozzi, Lorenzo$$iINSPIRE-00349900$$uGeneva U.
002255384 700__ $$aPapadopoulou, Theodora$$iINSPIRE-00185572$$uNatl. Tech. U., Athens
002255384 700__ $$aPapageorgiou, Konstantinos$$iINSPIRE-00114455$$uAthens U.
002255384 700__ $$aParamonov, Alexander$$iINSPIRE-00040880$$uArgonne
002255384 700__ $$aParedes Hernandez, Daniela$$iINSPIRE-00286969$$uYale U.
002255384 700__ $$aParker, Adam Jackson$$iINSPIRE-00511754$$uLancaster U.
002255384 700__ $$aParker, Michael Andrew$$iINSPIRE-00114726$$uCambridge U.
002255384 700__ $$aParker, Kerry Ann$$iINSPIRE-00371766$$uDESY
002255384 700__ $$aParodi, Fabrizio$$iINSPIRE-00339598$$uINFN, Genoa$$uGenoa U.
002255384 700__ $$aParsons, John$$iINSPIRE-00114789$$uNevis Labs, Columbia U.
002255384 700__ $$aParzefall, Ulrich$$iINSPIRE-00114827$$uFreiburg U.
002255384 700__ $$aPascuzzi, Vincent$$iINSPIRE-00423665$$uToronto U.
002255384 700__ $$aPasner, Jacob Martin$$iINSPIRE-00540573$$uUC, Santa Cruz
002255384 700__ $$aPasqualucci, Enrico$$iINSPIRE-00221595$$uINFN, Rome
002255384 700__ $$aPassaggio, Stefano$$iINSPIRE-00114912$$uINFN, Genoa
002255384 700__ $$aPastore, Francesca$$iINSPIRE-00221618$$uRoyal Holloway, U. of London
002255384 700__ $$aPataraia, Sophio$$iINSPIRE-00221648$$uWuppertal U.
002255384 700__ $$aPater, Joleen$$iINSPIRE-00221668$$uManchester U.
002255384 700__ $$aPauly, Thilo$$iINSPIRE-00221680$$uCERN
002255384 700__ $$aPearce, James$$iINSPIRE-00333118$$uVictoria U.
002255384 700__ $$aPearson, Benjamin$$iINSPIRE-00368502$$uOklahoma U.
002255384 700__ $$aPedersen, Lars Egholm$$iINSPIRE-00379022$$uBohr Inst.
002255384 700__ $$aPedraza Lopez, Sebastian$$iINSPIRE-00288626$$uValencia U., IFIC
002255384 700__ $$aPedro, Rute$$iINSPIRE-00357018$$uLIP, Lisbon$$uLisbon U., CFNUL
002255384 700__ $$aPeleganchuk, Sergey$$iINSPIRE-00221714$$uNovosibirsk State U.$$uNovosibirsk, IYF
002255384 700__ $$aPenc, Ondrej$$iINSPIRE-00408388$$uPrague, Inst. Phys.
002255384 700__ $$aPeng, Cong$$iINSPIRE-00407696$$uBeijing, Inst. High Energy Phys.
002255384 700__ $$aPeng, Haiping$$iINSPIRE-00217635$$uHefei, CUST
002255384 700__ $$aPenwell, John$$iINSPIRE-00221730$$uIndiana U.
002255384 700__ $$aPeralva, Bernardo$$iINSPIRE-00517880$$uJuiz de Fora U.
002255384 700__ $$aPerego, Marta Maria$$iINSPIRE-00444101$$uIRFU, Saclay
002255384 700__ $$aPerepelitsa, Dennis$$iINSPIRE-00342739$$uBrookhaven
002255384 700__ $$aPerini, Laura$$iINSPIRE-00221789$$uINFN, Milan$$uMilan U.
002255384 700__ $$aPernegger, Heinz$$iINSPIRE-00115755$$uCERN
002255384 700__ $$aPerrella, Sabrina$$iINSPIRE-00377109$$uINFN, Naples$$uNaples U.
002255384 700__ $$aPeschke, Richard$$iINSPIRE-00356050$$uDESY
002255384 700__ $$aPeshekhonov, Vladimir$$iINSPIRE-00221820$$uDubna, JINR
002255384 700__ $$aPeters, Krisztian$$iINSPIRE-00055152$$uDESY
002255384 700__ $$aPeters, Yvonne$$iINSPIRE-00008252$$uManchester U.
002255384 700__ $$aPetersen, Brian$$iINSPIRE-00115959$$uCERN
002255384 700__ $$aPetersen, Troels$$iINSPIRE-00221831$$uBohr Inst.
002255384 700__ $$aPetit, Elisabeth$$iINSPIRE-00221840$$uLPSC, Grenoble
002255384 700__ $$aPetridis, Andreas$$iINSPIRE-00232124$$uAdelaide U., Sch. Chem. Phys.
002255384 700__ $$aPetridou, Chariclia$$iINSPIRE-00116033$$uAristotle U., Thessaloniki
002255384 700__ $$aPetroff, Pierre$$iINSPIRE-00116049$$uOrsay, LAL
002255384 700__ $$aPetrolo, Emilio$$iINSPIRE-00221866$$uINFN, Rome
002255384 700__ $$aPetrov, Mariyan$$iINSPIRE-00443150$$uOxford U.
002255384 700__ $$aPetrucci, Fabrizio$$iINSPIRE-00221875$$uINFN, Rome$$uRome III U.
002255384 700__ $$aPettersson, Nora Emilia$$iINSPIRE-00360876$$uMassachusetts U., Amherst
002255384 700__ $$aPeyaud, Alan$$iINSPIRE-00380396$$uIRFU, Saclay
002255384 700__ $$aPezoa, Raquel$$iINSPIRE-00221890$$uSanta Maria U., Valparaiso
002255384 700__ $$aPhillips, Peter William$$iINSPIRE-00116199$$uRutherford
002255384 700__ $$aPiacquadio, Giacinto$$iINSPIRE-00221917$$uSUNY, Stony Brook
002255384 700__ $$aPianori, Elisabetta$$iINSPIRE-00009958$$uWarwick U.
002255384 700__ $$aPicazio, Attilio$$iINSPIRE-00286993$$uMassachusetts U., Amherst
002255384 700__ $$aPiccaro, Elisa$$iINSPIRE-00221925$$uQueen Mary, U. of London
002255384 700__ $$aPickering, Mark Andrew$$iINSPIRE-00378953$$uOxford U.
002255384 700__ $$aPiegaia, Ricardo$$iINSPIRE-00152829$$uBuenos Aires U.
002255384 700__ $$aPilcher, James$$iINSPIRE-00116477$$uChicago U., EFI
002255384 700__ $$aPilkington, Andrew$$iINSPIRE-00221938$$uManchester U.
002255384 700__ $$aPin, Arnaud Willy J$$iINSPIRE-00191428$$uManchester U.
002255384 700__ $$aPinamonti, Michele$$iINSPIRE-00221947$$uINFN, Udine$$uUdine U.$$uSISSA, Trieste
002255384 700__ $$aPinfold, James$$iINSPIRE-00116512$$uAlberta U.
002255384 700__ $$aPirumov, Hayk$$iINSPIRE-00243807$$uDESY
002255384 700__ $$aPitt, Michael$$iINSPIRE-00354261$$uWeizmann Inst.
002255384 700__ $$aPlazak, Lukas$$iINSPIRE-00374596$$uComenius U.
002255384 700__ $$aPleier, Marc-Andre$$iINSPIRE-00046720$$uBrookhaven
002255384 700__ $$aPleskot, Vojtech$$iINSPIRE-00335597$$uMainz U.
002255384 700__ $$aPlotnikova, Elena$$iINSPIRE-00237193$$uDubna, JINR
002255384 700__ $$aPluth, Daniel$$iINSPIRE-00365906$$uIowa State U.
002255384 700__ $$aPodberezko, Pavel$$iINSPIRE-00537273$$uNovosibirsk State U.$$uNovosibirsk, IYF
002255384 700__ $$aPoettgen, Ruth$$iINSPIRE-00335606$$uStockholm U.$$uStockholm U., OKC
002255384 700__ $$aPoggioli, Luc$$iINSPIRE-00221996$$uOrsay, LAL
002255384 700__ $$aPohl, David-leon$$iINSPIRE-00288837$$uBonn U.
002255384 700__ $$aPolesello, Giacomo$$iINSPIRE-00117049$$uINFN, Pavia
002255384 700__ $$aPoley, Anne-luise$$iINSPIRE-00407830$$uDESY
002255384 700__ $$aPolicicchio, Antonio$$iINSPIRE-00020903$$uINFN, Cosenza$$uCalabria U.
002255384 700__ $$aPolifka, Richard$$iINSPIRE-00185642$$uCERN
002255384 700__ $$aPolini, Alessandro$$iINSPIRE-00172064$$uINFN, Bologna
002255384 700__ $$aPollard, Christopher Samuel$$iINSPIRE-00345073$$uGlasgow U.
002255384 700__ $$aPolychronakos, Venetios$$iINSPIRE-00177114$$uBrookhaven
002255384 700__ $$aPommès, Kathy$$iINSPIRE-00222020$$uCERN
002255384 700__ $$aPontecorvo, Ludovico$$iINSPIRE-00222031$$uINFN, Rome
002255384 700__ $$aPope, Bernard$$iINSPIRE-00117279$$uMichigan State U.
002255384 700__ $$aPopeneciu, Gabriel Alexandru$$iINSPIRE-00226844$$uINCDTIM, Cluj Napoca
002255384 700__ $$aPoppleton, Alan$$iINSPIRE-00222058$$uCERN
002255384 700__ $$aPospisil, Stanislav$$iINSPIRE-00222085$$uPrague, Tech. U.
002255384 700__ $$aPotamianos, Karolos$$iINSPIRE-00019188$$uLBL, Berkeley
002255384 700__ $$aPotrap, Igor$$iINSPIRE-00222100$$uDubna, JINR
002255384 700__ $$aPotter, Christina$$iINSPIRE-00222115$$uCambridge U.
002255384 700__ $$aPotter, Christopher$$iINSPIRE-00042218$$uOregon U.
002255384 700__ $$aPoulard, Gilbert$$iINSPIRE-00222120$$uCERN
002255384 700__ $$aPoveda, Joaquin$$iINSPIRE-00222132$$uCERN
002255384 700__ $$aPozo Astigarraga, Mikel Eukeni$$iINSPIRE-00390254$$uCERN
002255384 700__ $$aPralavorio, Pascal$$iINSPIRE-00117512$$uMarseille, CPPM
002255384 700__ $$aPranko, Aliaksandr$$iINSPIRE-00049000$$uLBL, Berkeley
002255384 700__ $$aPrell, Soeren$$iINSPIRE-00117610$$uIowa State U.
002255384 700__ $$aPrice, Darren$$iINSPIRE-00027472$$uManchester U.
002255384 700__ $$aPrice, Lawrence$$iINSPIRE-00117710$$uArgonne
002255384 700__ $$aPrimavera, Margherita$$iINSPIRE-00117740$$uINFN, Lecce
002255384 700__ $$aPrince, Sebastien$$iINSPIRE-00359694$$uMcGill U.
002255384 700__ $$aProkofiev, Kirill$$iINSPIRE-00002760$$uHong Kong U. Sci. Tech.
002255384 700__ $$aProkoshin, Fedor$$iINSPIRE-00030407$$uSanta Maria U., Valparaiso
002255384 700__ $$aProtopopescu, Serban$$iINSPIRE-00117905$$uBrookhaven
002255384 700__ $$aProudfoot, James$$iINSPIRE-00117915$$uArgonne
002255384 700__ $$aPrzybycien, Mariusz$$iINSPIRE-00117955$$uAGH-UST, Cracow
002255384 700__ $$aPuddu, Daniele$$iINSPIRE-00367527$$uINFN, Rome$$uRome III U.
002255384 700__ $$aPuri, Akshat$$iINSPIRE-00515564$$uIllinois U., Urbana
002255384 700__ $$aPuzo, Patrick$$iINSPIRE-00222199$$uOrsay, LAL
002255384 700__ $$aQian, Jianming$$iINSPIRE-00118167$$uMichigan U.
002255384 700__ $$aQin, Gang$$iINSPIRE-00273074$$uGlasgow U.
002255384 700__ $$aQin, Yang$$iINSPIRE-00367059$$uManchester U.
002255384 700__ $$aQuadt, Arnulf$$iINSPIRE-00118216$$uGottingen U., II. Phys. Inst.
002255384 700__ $$aQuayle, William$$iINSPIRE-00222250$$uINFN, Udine$$uICTP, Trieste
002255384 700__ $$aQueitsch-Maitland, Michaela$$iINSPIRE-00367060$$uDESY
002255384 700__ $$aQuilty, Donnchadha$$iINSPIRE-00014465$$uGlasgow U.
002255384 700__ $$aRaddum, Silje$$iINSPIRE-00380321$$uOslo U.
002255384 700__ $$aRadeka, Veljko$$iINSPIRE-00304240$$uBrookhaven
002255384 700__ $$aRadescu, Voica$$iINSPIRE-00028751$$uOxford U.
002255384 700__ $$aRadhakrishnan, Sooraj Krishnan$$iINSPIRE-00354278$$uSUNY, Stony Brook
002255384 700__ $$aRadloff, Peter$$iINSPIRE-00237221$$uOregon U.
002255384 700__ $$aRados, Pere$$iINSPIRE-00362130$$uMelbourne U.
002255384 700__ $$aRagusa, Francesco$$iINSPIRE-00194492$$uINFN, Milan$$uMilan U.
002255384 700__ $$aRahal, Ghita$$iINSPIRE-00301248$$uCC, Villeurbanne
002255384 700__ $$aRaine, John Andrew$$iINSPIRE-00452694$$uManchester U.
002255384 700__ $$aRajagopalan, Srinivasan$$iINSPIRE-00222308$$uBrookhaven
002255384 700__ $$aRangel-Smith, Camila$$iINSPIRE-00237235$$uUppsala U., Inst. Theor. Phys.
002255384 700__ $$aRatti, Maria Giulia$$iINSPIRE-00443282$$uINFN, Milan$$uMilan U.
002255384 700__ $$aRauch, Daniel$$iINSPIRE-00525066$$uDESY
002255384 700__ $$aRauscher, Felix$$iINSPIRE-00222332$$uMunich U.
002255384 700__ $$aRave, Stefan$$iINSPIRE-00386585$$uMainz U.
002255384 700__ $$aRavenscroft, Thomas$$iINSPIRE-00334506$$uGlasgow U.
002255384 700__ $$aRavinovich, Ilia$$iINSPIRE-00119200$$uWeizmann Inst.
002255384 700__ $$aRaymond, Michel$$iINSPIRE-00222353$$uCERN
002255384 700__ $$aRead, Alexander Lincoln$$iINSPIRE-00119327$$uOslo U.
002255384 700__ $$aReadioff, Nathan Peter$$iINSPIRE-00368514$$uLiverpool U.
002255384 700__ $$aReale, Marilea$$iINSPIRE-00445873$$uINFN, Lecce$$uSalento U.
002255384 700__ $$aRebuzzi, Daniela$$iINSPIRE-00222361$$uINFN, Pavia$$uPavia U.
002255384 700__ $$aRedelbach, Andreas$$iINSPIRE-00222375$$uWurzburg U.
002255384 700__ $$aRedlinger, George$$iINSPIRE-00119430$$uBrookhaven
002255384 700__ $$aReece, Ryan$$iINSPIRE-00016749$$uUC, Santa Cruz
002255384 700__ $$aReed, Robert$$iINSPIRE-00508435$$uWitwatersrand U.
002255384 700__ $$aReeves, Kendall$$iINSPIRE-00142245$$uTexas U., Dallas
002255384 700__ $$aRehnisch, Laura$$iINSPIRE-00354285$$uHumboldt U., Berlin
002255384 700__ $$aReichert, Joseph$$iINSPIRE-00423182$$uPennsylvania U.
002255384 700__ $$aReiss, Andreas$$iINSPIRE-00390339$$uMainz U.
002255384 700__ $$aRembser, Christoph$$iINSPIRE-00222420$$uCERN
002255384 700__ $$aRen, Huan$$iINSPIRE-00360700$$uBeijing, Inst. High Energy Phys.
002255384 700__ $$aRescigno, Marco$$iINSPIRE-00119727$$uINFN, Rome
002255384 700__ $$aResconi, Silvia$$iINSPIRE-00222441$$uINFN, Milan
002255384 700__ $$aResseguie, Elodie Deborah$$iINSPIRE-00540608$$uPennsylvania U.
002255384 700__ $$aRettie, Sebastien$$iINSPIRE-00436230$$uBritish Columbia U.
002255384 700__ $$aReynolds, Elliot$$iINSPIRE-00537820$$uBirmingham U.
002255384 700__ $$aRezanova, Olga$$iINSPIRE-00235827$$uNovosibirsk State U.$$uNovosibirsk, IYF
002255384 700__ $$aReznicek, Pavel$$iINSPIRE-00222462$$uCharles U.
002255384 700__ $$aRezvani, Reyhaneh$$iINSPIRE-00226862$$uMontreal U.
002255384 700__ $$aRichter, Robert$$iINSPIRE-00120026$$uMunich, Max Planck Inst.
002255384 700__ $$aRichter, Stefan$$iINSPIRE-00393156$$uUniversity Coll. London
002255384 700__ $$aRichter-Was, Elzbieta$$iINSPIRE-00222485$$uJagiellonian U.
002255384 700__ $$aRicken, Oliver$$iINSPIRE-00394440$$uBonn U.
002255384 700__ $$aRidel, Melissa$$iINSPIRE-00052999$$uParis U., VI-VII
002255384 700__ $$aRieck, Patrick$$iINSPIRE-00333614$$uMunich, Max Planck Inst.
002255384 700__ $$aRiegel, Christian Johann$$iINSPIRE-00390368$$uWuppertal U.
002255384 700__ $$aRieger, Julia$$iINSPIRE-00367854$$uGottingen U., II. Phys. Inst.
002255384 700__ $$aRifki, Othmane$$iINSPIRE-00421293$$uOklahoma U.
002255384 700__ $$aRijssenbeek, Michael$$iINSPIRE-00120164$$uSUNY, Stony Brook
002255384 700__ $$aRimoldi, Adele$$iINSPIRE-00120224$$uINFN, Pavia$$uPavia U.
002255384 700__ $$aRimoldi, Marco$$iINSPIRE-00511766$$uBern U., LHEP
002255384 700__ $$aRinaldi, Lorenzo$$iINSPIRE-00222509$$uINFN, Bologna
002255384 700__ $$aRistić, Branislav$$iINSPIRE-00442335$$uGeneva U.
002255384 700__ $$aRitsch, Elmar$$iINSPIRE-00334537$$uCERN
002255384 700__ $$aRiu, Imma$$iINSPIRE-00120419$$uBarcelona, IFAE
002255384 700__ $$aRizatdinova, Flera$$iINSPIRE-00048668$$uOklahoma State U.
002255384 700__ $$aRizvi, Eram$$iINSPIRE-00120467$$uQueen Mary, U. of London
002255384 700__ $$aRizzi, Chiara$$iINSPIRE-00403072$$uBarcelona, IFAE
002255384 700__ $$aRoberts, Rhys Thomas$$iINSPIRE-00534698$$uManchester U.
002255384 700__ $$aRobertson, Steven$$iINSPIRE-00120586$$uMcGill U.$$uIPP, Canada
002255384 700__ $$aRobichaud-Veronneau, Andree$$iINSPIRE-00220239$$uMcGill U.
002255384 700__ $$aRobinson, Dave$$iINSPIRE-00222525$$uCambridge U.
002255384 700__ $$aRobinson, James$$iINSPIRE-00222565$$uDESY
002255384 700__ $$aRobson, Aidan$$iINSPIRE-00052951$$uGlasgow U.
002255384 700__ $$aRoda, Chiara$$iINSPIRE-00222584$$uINFN, Pisa$$uPisa U.
002255384 700__ $$aRodina, Yulia$$iINSPIRE-00439858$$uMarseille, CPPM$$uBarcelona, IFAE
002255384 700__ $$aRodriguez Perez, Andrea$$iINSPIRE-00436939$$uBarcelona, IFAE
002255384 700__ $$aRodriguez Rodriguez, Daniel$$iINSPIRE-00442425$$uValencia U., IFIC
002255384 700__ $$aRoe, Shaun$$iINSPIRE-00222620$$uCERN
002255384 700__ $$aRogan, Christopher Sean$$iINSPIRE-00008339$$uHarvard U., Phys. Dept.
002255384 700__ $$aRøhne, Ole$$iINSPIRE-00120872$$uOslo U.
002255384 700__ $$aRoloff, Jennifer$$iINSPIRE-00283411$$uHarvard U., Phys. Dept.
002255384 700__ $$aRomaniouk, Anatoli$$iINSPIRE-00222643$$uMoscow Phys. Eng. Inst.
002255384 700__ $$aRomano, Marino$$iINSPIRE-00237277$$uINFN, Bologna$$uBologna U.
002255384 700__ $$aRomano Saez, Silvestre Marino$$iINSPIRE-00390473$$uClermont-Ferrand U.
002255384 700__ $$aRomero Adam, Elena$$iINSPIRE-00237280$$uValencia U., IFIC
002255384 700__ $$aRompotis, Nikolaos$$iINSPIRE-00311758$$uLiverpool U.
002255384 700__ $$aRonzani, Manfredi$$iINSPIRE-00265551$$uFreiburg U.
002255384 700__ $$aRoos, Lydia$$iINSPIRE-00121125$$uParis U., VI-VII
002255384 700__ $$aRosati, Stefano$$iINSPIRE-00226874$$uINFN, Rome
002255384 700__ $$aRosbach, Kilian$$iINSPIRE-00237292$$uFreiburg U.
002255384 700__ $$aRose, Peyton$$iINSPIRE-00376762$$uUC, Santa Cruz
002255384 700__ $$aRosien, Nils-Arne$$iINSPIRE-00451917$$uGottingen U., II. Phys. Inst.
002255384 700__ $$aRossetti, Valerio$$iINSPIRE-00222722$$uStockholm U.$$uStockholm U., OKC
002255384 700__ $$aRossi, Elvira$$iINSPIRE-00232312$$uINFN, Naples$$uNaples U.
002255384 700__ $$aRossi, Leonardo Paolo$$iINSPIRE-00222731$$uINFN, Genoa
002255384 700__ $$aRosten, Jonatan$$iINSPIRE-00396349$$uCambridge U.
002255384 700__ $$aRosten, Rachel$$iINSPIRE-00345760$$uWashington U., Seattle
002255384 700__ $$aRotaru, Marina$$iINSPIRE-00185709$$uBucharest, IFIN-HH
002255384 700__ $$aRoth, Itamar$$iINSPIRE-00232324$$uWeizmann Inst.
002255384 700__ $$aRothberg, Joseph$$iINSPIRE-00147103$$uWashington U., Seattle
002255384 700__ $$aRousseau, David$$iINSPIRE-00121457$$uOrsay, LAL
002255384 700__ $$aRozanov, Alexandre$$iINSPIRE-00121556$$uMarseille, CPPM
002255384 700__ $$aRozen, Yoram$$iINSPIRE-00222740$$uTechnion
002255384 700__ $$aRuan, Xifeng$$iINSPIRE-00227177$$uWitwatersrand U.
002255384 700__ $$aRubbo, Francesco$$iINSPIRE-00263547$$uSLAC
002255384 700__ $$aRühr, Frederik$$iINSPIRE-00222786$$uFreiburg U.
002255384 700__ $$aRuiz-Martinez, Aranzazu$$iINSPIRE-00222798$$uCarleton U.
002255384 700__ $$aRurikova, Zuzana$$iINSPIRE-00217990$$uFreiburg U.
002255384 700__ $$aRusakovich, Nikolai$$iINSPIRE-00301212$$uDubna, JINR
002255384 700__ $$aRuschke, Alexander$$iINSPIRE-00295921$$uMunich U.
002255384 700__ $$aRussell, Heather$$iINSPIRE-00381301$$uWashington U., Seattle
002255384 700__ $$aRutherfoord, John$$iINSPIRE-00122016$$uArizona U.
002255384 700__ $$aRuthmann, Nils$$iINSPIRE-00334543$$uCERN
002255384 700__ $$aRyabov, Yury$$iINSPIRE-00306193$$uSt. Petersburg, INP
002255384 700__ $$aRybar, Martin$$iINSPIRE-00287074$$uIllinois U., Urbana
002255384 700__ $$aRybkin, Grigori$$iINSPIRE-00222835$$uOrsay, LAL
002255384 700__ $$aRyu, Soo$$iINSPIRE-00370160$$uArgonne
002255384 700__ $$aRyzhov, Andrey$$iINSPIRE-00414625$$uSerpukhov, IHEP
002255384 700__ $$aRzehorz, Gerhard Ferdinand$$iINSPIRE-00396985$$uGottingen U., II. Phys. Inst.
002255384 700__ $$aSaavedra, Aldo$$iINSPIRE-00222859$$uSydney U.
002255384 700__ $$aSabato, Gabriele$$iINSPIRE-00375930$$uFOM, Amsterdam
002255384 700__ $$aSacerdoti, Sabrina$$iINSPIRE-00339152$$uBuenos Aires U.
002255384 700__ $$aSadrozinski, Hartmut$$iINSPIRE-00122290$$uUC, Santa Cruz
002255384 700__ $$aSadykov, Renat$$iINSPIRE-00222866$$uDubna, JINR
002255384 700__ $$aSafai Tehrani, Francesco$$iINSPIRE-00041870$$uINFN, Rome
002255384 700__ $$aSaha, Puja$$iINSPIRE-00418043$$uNorthern Illinois U.
002255384 700__ $$aSahinsoy, Merve$$iINSPIRE-00394595$$uKirchhoff Inst. Phys.
002255384 700__ $$aSaimpert, Matthias$$iINSPIRE-00387311$$uDESY
002255384 700__ $$aSaito, Tomoyuki$$iINSPIRE-00399900$$uTokyo U., ICEPP
002255384 700__ $$aSakamoto, Hiroshi$$iINSPIRE-00122550$$uTokyo U., ICEPP
002255384 700__ $$aSakurai, Yuki$$iINSPIRE-00263552$$uWaseda U.
002255384 700__ $$aSalamanna, Giuseppe$$iINSPIRE-00040818$$uINFN, Rome$$uRome III U.
002255384 700__ $$aSalazar Loyola, Javier Esteban$$iINSPIRE-00393200$$uSanta Maria U., Valparaiso
002255384 700__ $$aSalek, David$$iINSPIRE-00185720$$uFOM, Amsterdam
002255384 700__ $$aSales De Bruin, Pedro Henrique$$iINSPIRE-00354071$$uWashington U., Seattle
002255384 700__ $$aSalihagic, Denis$$iINSPIRE-00122755$$uMunich, Max Planck Inst.
002255384 700__ $$aSalnikov, Andrei$$iINSPIRE-00122791$$uSLAC
002255384 700__ $$aSalt, José$$iINSPIRE-00222878$$uValencia U., IFIC
002255384 700__ $$aSalvatore, Daniela$$iINSPIRE-00222890$$uINFN, Cosenza$$uCalabria U.
002255384 700__ $$aSalvatore, Pasquale Fabrizio$$iINSPIRE-00042310$$uSussex U.
002255384 700__ $$aSalvucci, Antonio$$iINSPIRE-00222904$$uHong Kong, Chinese U.$$uHong Kong U.$$uHong Kong U. Sci. Tech.
002255384 700__ $$aSalzburger, Andreas$$iINSPIRE-00222917$$uCERN
002255384 700__ $$aSammel, Dirk$$iINSPIRE-00394771$$uFreiburg U.
002255384 700__ $$aSampsonidis, Dimitrios$$iINSPIRE-00222923$$uAristotle U., Thessaloniki
002255384 700__ $$aSánchez, Javier$$iINSPIRE-00224147$$uValencia U., IFIC
002255384 700__ $$aSanchez Martinez, Victoria$$iINSPIRE-00237361$$uValencia U., IFIC
002255384 700__ $$aSanchez Pineda, Arturo Rodolfo$$iINSPIRE-00237353$$uINFN, Naples$$uNaples U.
002255384 700__ $$aSandaker, Heidi$$iINSPIRE-00222934$$uOslo U.
002255384 700__ $$aSandbach, Ruth Laura$$iINSPIRE-00358569$$uQueen Mary, U. of London
002255384 700__ $$aSander, Christian Oliver$$iINSPIRE-00315812$$uDESY
002255384 700__ $$aSandhoff, Marisa$$iINSPIRE-00008264$$uWuppertal U.
002255384 700__ $$aSandoval, Carlos$$iINSPIRE-00237372$$uAntonio Narino U.
002255384 700__ $$aSankey, Dave$$iINSPIRE-00123095$$uRutherford
002255384 700__ $$aSannino, Mario$$iINSPIRE-00123116$$uINFN, Genoa$$uGenoa U.
002255384 700__ $$aSansoni, Andrea$$iINSPIRE-00222964$$uFrascati
002255384 700__ $$aSantoni, Claudio$$iINSPIRE-00161887$$uClermont-Ferrand U.
002255384 700__ $$aSantonico, Rinaldo$$iINSPIRE-00222976$$uINFN, Rome$$uRome U., Tor Vergata
002255384 700__ $$aSantos, Helena$$iINSPIRE-00232412$$uLIP, Lisbon
002255384 700__ $$aSantoyo Castillo, Itzebelt$$iINSPIRE-00291958$$uSussex U.
002255384 700__ $$aSapp, Kevin$$iINSPIRE-00335926$$uPittsburgh U.
002255384 700__ $$aSapronov, Andrey$$iINSPIRE-00011775$$uDubna, JINR
002255384 700__ $$aSaraiva, João$$iINSPIRE-00306227$$uLIP, Lisbon$$uLisbon U., CFNUL
002255384 700__ $$aSarrazin, Bjorn$$iINSPIRE-00334550$$uBonn U.
002255384 700__ $$aSasaki, Osamu$$iINSPIRE-00123320$$uKEK, Tsukuba
002255384 700__ $$aSato, Koji$$iINSPIRE-00048967$$uTsukuba U.
002255384 700__ $$aSauvan, Emmanuel$$iINSPIRE-00185747$$uAnnecy, LAPP
002255384 700__ $$aSavage, Graham$$iINSPIRE-00375948$$uRoyal Holloway, U. of London
002255384 700__ $$aSavard, Pierre$$iINSPIRE-00123492$$uToronto U.$$uTRIUMF
002255384 700__ $$aSavic, Natascha$$iINSPIRE-00517212$$uMunich, Max Planck Inst.
002255384 700__ $$aSawyer, Craig$$iINSPIRE-00337679$$uRutherford
002255384 700__ $$aSawyer, Lee$$iINSPIRE-00123608$$uLouisiana Tech. U.
002255384 700__ $$aSaxon, James$$iINSPIRE-00332965$$uChicago U., EFI
002255384 700__ $$aSbarra, Carla$$iINSPIRE-00223003$$uINFN, Bologna
002255384 700__ $$aSbrizzi, Antonio$$iINSPIRE-00223019$$uINFN, Bologna$$uBologna U.
002255384 700__ $$aScanlon, Tim$$iINSPIRE-00038709$$uUniversity Coll. London
002255384 700__ $$aScannicchio, Diana$$iINSPIRE-00223137$$uUC, Irvine
002255384 700__ $$aScarcella, Mark$$iINSPIRE-00287125$$uSydney U.
002255384 700__ $$aScarfone, Valerio$$iINSPIRE-00356284$$uINFN, Cosenza$$uCalabria U.
002255384 700__ $$aSchaarschmidt, Jana$$iINSPIRE-00223142$$uWashington U., Seattle
002255384 700__ $$aSchacht, Peter$$iINSPIRE-00223156$$uMunich, Max Planck Inst.
002255384 700__ $$aSchachtner, Balthasar Maria$$iINSPIRE-00470481$$uMunich U.
002255384 700__ $$aSchaefer, Douglas$$iINSPIRE-00332120$$uCERN
002255384 700__ $$aSchaefer, Leigh$$iINSPIRE-00442510$$uPennsylvania U.
002255384 700__ $$aSchaefer, Ralph$$iINSPIRE-00362142$$uDESY
002255384 700__ $$aSchaeffer, Jan$$iINSPIRE-00354291$$uMainz U.
002255384 700__ $$aSchaepe, Steffen$$iINSPIRE-00237394$$uBonn U.
002255384 700__ $$aSchaetzel, Sebastian$$iINSPIRE-00217959$$uHeidelberg U.
002255384 700__ $$aSchäfer, Uli$$iINSPIRE-00146919$$uMainz U.
002255384 700__ $$aSchaffer, Arthur$$iINSPIRE-00223168$$uOrsay, LAL
002255384 700__ $$aSchaile, Dorothee$$iINSPIRE-00300542$$uMunich U.
002255384 700__ $$aSchamberger, R Dean$$iINSPIRE-00123848$$uSUNY, Stony Brook
002255384 700__ $$aScharf, Veit$$iINSPIRE-00223180$$uKirchhoff Inst. Phys.
002255384 700__ $$aSchegelsky, Valery$$iINSPIRE-00223190$$uSt. Petersburg, INP
002255384 700__ $$aScheirich, Daniel$$iINSPIRE-00223208$$uCharles U.
002255384 700__ $$aSchernau, Michael$$iINSPIRE-00123929$$uUC, Irvine
002255384 700__ $$aSchiavi, Carlo$$iINSPIRE-00223222$$uINFN, Genoa$$uGenoa U.
002255384 700__ $$aSchier, Sheena$$iINSPIRE-00507500$$uUC, Santa Cruz
002255384 700__ $$aSchillo, Christian$$iINSPIRE-00336635$$uFreiburg U.
002255384 700__ $$aSchioppa, Marco$$iINSPIRE-00172296$$uINFN, Cosenza$$uCalabria U.
002255384 700__ $$aSchlenker, Stefan$$iINSPIRE-00223244$$uCERN
002255384 700__ $$aSchmidt-Sommerfeld, Korbinian Ralf$$iINSPIRE-00470659$$uMunich, Max Planck Inst.
002255384 700__ $$aSchmieden, Kristof$$iINSPIRE-00260738$$uCERN
002255384 700__ $$aSchmitt, Christian$$iINSPIRE-00058231$$uMainz U.
002255384 700__ $$aSchmitt, Stefan$$iINSPIRE-00124271$$uDESY
002255384 700__ $$aSchmitz, Simon$$iINSPIRE-00424511$$uMainz U.
002255384 700__ $$aSchneider, Basil$$iINSPIRE-00287133$$uTRIUMF
002255384 700__ $$aSchnoor, Ulrike$$iINSPIRE-00287141$$uFreiburg U.
002255384 700__ $$aSchoeffel, Laurent$$iINSPIRE-00185759$$uIRFU, Saclay
002255384 700__ $$aSchoening, Andre$$iINSPIRE-00185763$$uHeidelberg U.
002255384 700__ $$aSchoenrock, Bradley Daniel$$iINSPIRE-00329529$$uMichigan State U.
002255384 700__ $$aSchopf, Elisabeth$$iINSPIRE-00396420$$uBonn U.
002255384 700__ $$aSchott, Matthias$$iINSPIRE-00223276$$uMainz U.
002255384 700__ $$aSchouwenberg, Jeroen$$iINSPIRE-00518610$$uNIKHEF, Amsterdam
002255384 700__ $$aSchovancova, Jaroslava$$iINSPIRE-00153378$$uTexas U., Arlington
002255384 700__ $$aSchramm, Steven$$iINSPIRE-00356617$$uGeneva U.
002255384 700__ $$aSchuh, Natascha$$iINSPIRE-00345099$$uMainz U.
002255384 700__ $$aSchulte, Alexandra$$iINSPIRE-00452850$$uMainz U.
002255384 700__ $$aSchultens, Martin Johannes$$iINSPIRE-00287155$$uBonn U.
002255384 700__ $$aSchultz-Coulon, Hans-Christian$$iINSPIRE-00124529$$uKirchhoff Inst. Phys.
002255384 700__ $$aSchulz, Holger$$iINSPIRE-00287163$$uHumboldt U., Berlin
002255384 700__ $$aSchumacher, Markus$$iINSPIRE-00223322$$uFreiburg U.
002255384 700__ $$aSchumm, Bruce$$iINSPIRE-00124566$$uUC, Santa Cruz
002255384 700__ $$aSchune, Philippe$$iINSPIRE-00124581$$uIRFU, Saclay
002255384 700__ $$aSchwartzman, Ariel$$iINSPIRE-00053381$$uSLAC
002255384 700__ $$aSchwarz, Thomas Andrew$$iINSPIRE-00025352$$uMichigan U.
002255384 700__ $$aSchweiger, Hansdieter$$iINSPIRE-00362154$$uManchester U.
002255384 700__ $$aSchwemling, Philippe$$iINSPIRE-00124725$$uIRFU, Saclay
002255384 700__ $$aSchwienhorst, Reinhard$$iINSPIRE-00050408$$uMichigan State U.
002255384 700__ $$aSchwindling, Jerome$$iINSPIRE-00223337$$uIRFU, Saclay
002255384 700__ $$aSchwindt, Thomas$$iINSPIRE-00237410$$uBonn U.
002255384 700__ $$aSciolla, Gabriella$$iINSPIRE-00124804$$uBrandeis U.
002255384 700__ $$aScuri, Fabrizio$$iINSPIRE-00124895$$uINFN, Pisa$$uPisa U.
002255384 700__ $$aScutti, Federico$$iINSPIRE-00339167$$uMelbourne U.
002255384 700__ $$aSearcy, Jacob$$iINSPIRE-00223354$$uMichigan U.
002255384 700__ $$aSeema, Pienpen$$iINSPIRE-00380584$$uBonn U.
002255384 700__ $$aSeidel, Sally$$iINSPIRE-00125002$$uNew Mexico U.
002255384 700__ $$aSeiden, Abraham$$iINSPIRE-00125018$$uUC, Santa Cruz
002255384 700__ $$aSeixas, José$$iINSPIRE-00306265$$uRio de Janeiro Federal U.
002255384 700__ $$aSekhniaidze, Givi$$iINSPIRE-00223392$$uINFN, Naples
002255384 700__ $$aSekhon, Karishma$$iINSPIRE-00405663$$uMichigan U.
002255384 700__ $$aSekula, Stephen$$iINSPIRE-00052448$$uSouthern Methodist U.
002255384 700__ $$aSemprini-Cesari, Nicola$$iINSPIRE-00223442$$uINFN, Bologna$$uBologna U.
002255384 700__ $$aSerfon, Cedric$$iINSPIRE-00223458$$uOslo U.
002255384 700__ $$aSerin, Laurent$$iINSPIRE-00223468$$uOrsay, LAL
002255384 700__ $$aSerkin, Leonid$$iINSPIRE-00246780$$uINFN, Udine$$uICTP, Trieste
002255384 700__ $$aSessa, Marco$$iINSPIRE-00404546$$uINFN, Rome$$uRome III U.
002255384 700__ $$aSeuster, Rolf$$iINSPIRE-00223473$$uVictoria U.
002255384 700__ $$aSeverini, Horst$$iINSPIRE-00125370$$uOklahoma U.
002255384 700__ $$aSfiligoj, Tina$$iINSPIRE-00371537$$uStefan Inst., Ljubljana
002255384 700__ $$aSforza, Federico$$iINSPIRE-00011580$$uCERN
002255384 700__ $$aSfyrla, Anna$$iINSPIRE-00030383$$uGeneva U.
002255384 700__ $$aShabalina, Elizaveta$$iINSPIRE-00038690$$uGottingen U., II. Phys. Inst.
002255384 700__ $$aShaikh, Nabila Wahab$$iINSPIRE-00440772$$uStockholm U.$$uStockholm U., OKC
002255384 700__ $$aShan, Lianyou$$iINSPIRE-00223489$$uBeijing, Inst. High Energy Phys.
002255384 700__ $$aShang, Ruo-yu$$iINSPIRE-00367695$$uIllinois U., Urbana
002255384 700__ $$aShank, James$$iINSPIRE-00125560$$uBoston U.
002255384 700__ $$aShapiro, Marjorie$$iINSPIRE-00125625$$uLBL, Berkeley
002255384 700__ $$aShatalov, Pavel$$iINSPIRE-00223506$$uMoscow, ITEP
002255384 700__ $$aShaw, Kate$$iINSPIRE-00223518$$uINFN, Udine$$uICTP, Trieste
002255384 700__ $$aShaw, Savanna Marie$$iINSPIRE-00347635$$uManchester U.
002255384 700__ $$aShcherbakova, Anna$$iINSPIRE-00386441$$uStockholm U.$$uStockholm U., OKC
002255384 700__ $$aShehu, Ciwake Yusufu$$iINSPIRE-00362166$$uSussex U.
002255384 700__ $$aShen, Yu-Ting$$iINSPIRE-00529728$$uOklahoma U.
002255384 700__ $$aSherwood, Peter$$iINSPIRE-00223529$$uUniversity Coll. London
002255384 700__ $$aShi, Liaoshan$$iINSPIRE-00367077$$uTaiwan, Inst. Phys.$$uZhongshan U.
002255384 700__ $$aShimizu, Shima$$iINSPIRE-00173951$$uKobe U.
002255384 700__ $$aShimmin, Chase Owen$$iINSPIRE-00364288$$uYale U.
002255384 700__ $$aShimojima, Makoto$$iINSPIRE-00050740$$uNagasaki Inst. Appl. Sci.
002255384 700__ $$aShirabe, Shohei$$iINSPIRE-00529735$$uKyushu U.
002255384 700__ $$aShiyakova, Mariya$$iINSPIRE-00237482$$uDubna, JINR$$uSofiya, Inst. Nucl. Res.
002255384 700__ $$aShlomi, Jonathan$$iINSPIRE-00541100$$uWeizmann Inst.
002255384 700__ $$aShmeleva, Alevtina$$iINSPIRE-00223548$$uLebedev Inst.
002255384 700__ $$aShoaleh Saadi, Diane$$iINSPIRE-00382063$$uMontreal U.
002255384 700__ $$aShochet, Mel$$iINSPIRE-00126064$$uChicago U., EFI
002255384 700__ $$aShojaii, Seyed Ruhollah$$iINSPIRE-00380893$$uINFN, Milan
002255384 700__ $$aShope, David Richard$$iINSPIRE-00529749$$uOklahoma U.
002255384 700__ $$aShrestha, Suyog$$iINSPIRE-00237498$$uOhio State U.
002255384 700__ $$aShulga, Evgeny$$iINSPIRE-00287239$$uMoscow Phys. Eng. Inst.
002255384 700__ $$aShupe, Michael$$iINSPIRE-00223552$$uArizona U.
002255384 700__ $$aSicho, Petr$$iINSPIRE-00223560$$uPrague, Inst. Phys.
002255384 700__ $$aSickles, Anne Marie$$iINSPIRE-00043440$$uIllinois U., Urbana
002255384 700__ $$aSidebo, Per Edvin$$iINSPIRE-00407780$$uRoyal Inst. Tech., Stockholm
002255384 700__ $$aSideras Haddad, Elias$$iINSPIRE-00508575$$uWitwatersrand U.
002255384 700__ $$aSidiropoulou, Ourania$$iINSPIRE-00377116$$uWurzburg U.
002255384 700__ $$aSidorov, Dmitri$$iINSPIRE-00007941$$uOklahoma State U.
002255384 700__ $$aSidoti, Antonio$$iINSPIRE-00040767$$uINFN, Bologna$$uBologna U.
002255384 700__ $$aSiegert, Frank$$iINSPIRE-00004088$$uDresden, Tech. U.
002255384 700__ $$aSijacki, Djordje$$iINSPIRE-00126317$$uBelgrade U.
002255384 700__ $$aSilva, José$$iINSPIRE-00227185$$uLIP, Lisbon$$uLisbon U., CFNUL
002255384 700__ $$aSilverstein, Samuel$$iINSPIRE-00223592$$uStockholm U.
002255384 700__ $$aSimak, Vladislav$$iINSPIRE-00126496$$uPrague, Tech. U.
002255384 700__ $$aSimic, Ljiljana$$iINSPIRE-00223604$$uBelgrade U.
002255384 700__ $$aSimion, Stefan$$iINSPIRE-00223610$$uOrsay, LAL
002255384 700__ $$aSimioni, Eduard$$iINSPIRE-00226165$$uMainz U.
002255384 700__ $$aSimmons, Brinick$$iINSPIRE-00223627$$uUniversity Coll. London
002255384 700__ $$aSimon, Manuel$$iINSPIRE-00396523$$uMainz U.
002255384 700__ $$aSinervo, Pekka$$iINSPIRE-00126695$$uToronto U.
002255384 700__ $$aSinev, Nikolai$$iINSPIRE-00042060$$uOregon U.
002255384 700__ $$aSioli, Maximiliano$$iINSPIRE-00126783$$uINFN, Bologna$$uBologna U.
002255384 700__ $$aSiragusa, Giovanni$$iINSPIRE-00020730$$uWurzburg U.
002255384 700__ $$aSiral, Ismet$$iINSPIRE-00529755$$uMichigan U.
002255384 700__ $$aSivoklokov, Serguei$$iINSPIRE-00223641$$uMoscow State U.
002255384 700__ $$aSjölin, Jörgen$$iINSPIRE-00180522$$uStockholm U.$$uStockholm U., OKC
002255384 700__ $$aSkinner, Malcolm Bruce$$iINSPIRE-00340295$$uLancaster U.
002255384 700__ $$aSkubic, Patrick$$iINSPIRE-00127003$$uOklahoma U.
002255384 700__ $$aSlater, Mark$$iINSPIRE-00223675$$uBirmingham U.
002255384 700__ $$aSlavicek, Tomas$$iINSPIRE-00223682$$uPrague, Tech. U.
002255384 700__ $$aSlawinska, Magdalena$$iINSPIRE-00379172$$uFOM, Amsterdam
002255384 700__ $$aSliwa, Krzysztof$$iINSPIRE-00127092$$uTufts U.
002255384 700__ $$aSlovak, Radim$$iINSPIRE-00443411$$uCharles U.
002255384 700__ $$aSmakhtin, Vladimir$$iINSPIRE-00223693$$uWeizmann Inst.
002255384 700__ $$aSmart, Ben$$iINSPIRE-00237541$$uAnnecy, LAPP
002255384 700__ $$aSmestad, Lillian$$iINSPIRE-00293064$$uBergen U.
002255384 700__ $$aSmiesko, Juraj$$iINSPIRE-00507669$$uComenius U.
002255384 700__ $$aSmirnov, Sergei$$iINSPIRE-00184110$$uMoscow Phys. Eng. Inst.
002255384 700__ $$aSmirnov, Yury$$iINSPIRE-00287508$$uMoscow Phys. Eng. Inst.
002255384 700__ $$aSmirnova, Lidia$$iINSPIRE-00223701$$uMoscow State U.$$uLomonosov Moscow State U.
002255384 700__ $$aSmirnova, Oxana$$iINSPIRE-00223710$$uLund U.
002255384 700__ $$aSmith, Joshua Wyatt$$iINSPIRE-00529764$$uGottingen U., II. Phys. Inst.
002255384 700__ $$aSmith, Matthew$$iINSPIRE-00382246$$uNevis Labs, Columbia U.
002255384 700__ $$aSmith, Russell$$iINSPIRE-00407872$$uNevis Labs, Columbia U.
002255384 700__ $$aSmizanska, Maria$$iINSPIRE-00127348$$uLancaster U.
002255384 700__ $$aSmolek, Karel$$iINSPIRE-00223725$$uPrague, Tech. U.
002255384 700__ $$aSnesarev, Andrei$$iINSPIRE-00223739$$uLebedev Inst.
002255384 700__ $$aSnyder, Ian Michael$$iINSPIRE-00529778$$uOregon U.
002255384 700__ $$aSnyder, Scott$$iINSPIRE-00300553$$uBrookhaven
002255384 700__ $$aSobie, Randall$$iINSPIRE-00127469$$uVictoria U.$$uIPP, Canada
002255384 700__ $$aSocher, Felix$$iINSPIRE-00355153$$uDresden, Tech. U.
002255384 700__ $$aSoffer, Abner$$iINSPIRE-00127510$$uTel Aviv U.
002255384 700__ $$aSoh, Dart-yin$$iINSPIRE-00227270$$uTaiwan, Inst. Phys.
002255384 700__ $$aSokhrannyi, Grygorii$$iINSPIRE-00418133$$uStefan Inst., Ljubljana
002255384 700__ $$aSolans Sanchez, Carlos$$iINSPIRE-00306293$$uCERN
002255384 700__ $$aSolar, Michael$$iINSPIRE-00223750$$uPrague, Tech. U.
002255384 700__ $$aSoldatov, Evgeny$$iINSPIRE-00237550$$uMoscow Phys. Eng. Inst.
002255384 700__ $$aSoldevila, Urmila$$iINSPIRE-00232570$$uValencia U., IFIC
002255384 700__ $$aSolodkov, Alexander$$iINSPIRE-00127668$$uSerpukhov, IHEP
002255384 700__ $$aSoloshenko, Alexei$$iINSPIRE-00368534$$uDubna, JINR
002255384 700__ $$aSolovyanov, Oleg$$iINSPIRE-00223789$$uSerpukhov, IHEP
002255384 700__ $$aSolovyev, Victor$$iINSPIRE-00287277$$uSt. Petersburg, INP
002255384 700__ $$aSommer, Philip$$iINSPIRE-00364294$$uFreiburg U.
002255384 700__ $$aSon, Hyungsuk$$iINSPIRE-00247667$$uTufts U.
002255384 700__ $$aSong, Hong Ye$$iINSPIRE-00363126$$uHefei, CUST$$uTaiwan, Inst. Phys.
002255384 700__ $$aSopczak, Andre$$iINSPIRE-00127812$$uPrague, Tech. U.
002255384 700__ $$aSorin, Veronica$$iINSPIRE-00049169$$uBarcelona, IFAE
002255384 700__ $$aSosa, David$$iINSPIRE-00365541$$uHeidelberg U.
002255384 700__ $$aSotiropoulou, Calliope Louisa$$iINSPIRE-00380743$$uINFN, Pisa$$uPisa U.
002255384 700__ $$aSoualah, Rachik$$iINSPIRE-00237567$$uINFN, Udine$$uUdine U.
002255384 700__ $$aSoukharev, Andrey$$iINSPIRE-00223813$$uNovosibirsk State U.$$uNovosibirsk, IYF
002255384 700__ $$aSouth, David$$iINSPIRE-00185821$$uDESY
002255384 700__ $$aSowden, Benjamin$$iINSPIRE-00403960$$uRoyal Holloway, U. of London
002255384 700__ $$aSpagnolo, Stefania$$iINSPIRE-00146499$$uINFN, Lecce$$uSalento U.
002255384 700__ $$aSpalla, Margherita$$iINSPIRE-00393248$$uINFN, Pisa$$uPisa U.
002255384 700__ $$aSpangenberg, Martin$$iINSPIRE-00396616$$uWarwick U.
002255384 700__ $$aSpanò, Francesco$$iINSPIRE-00051714$$uRoyal Holloway, U. of London
002255384 700__ $$aSperlich, Dennis$$iINSPIRE-00407979$$uHumboldt U., Berlin
002255384 700__ $$aSpettel, Fabian$$iINSPIRE-00366625$$uMunich, Max Planck Inst.
002255384 700__ $$aSpieker, Thomas Malte$$iINSPIRE-00535066$$uKirchhoff Inst. Phys.
002255384 700__ $$aSpighi, Roberto$$iINSPIRE-00223820$$uINFN, Bologna
002255384 700__ $$aSpigo, Giancarlo$$iINSPIRE-00223836$$uCERN
002255384 700__ $$aSpiller, Laurence Anthony$$iINSPIRE-00413161$$uMelbourne U.
002255384 700__ $$aSpousta, Martin$$iINSPIRE-00223860$$uCharles U.
002255384 700__ $$aSt Denis, Richard Dante$$iINSPIRE-00128281$$uGlasgow U.
002255384 700__ $$aStabile, Alberto$$iINSPIRE-00380950$$uINFN, Milan
002255384 700__ $$aStamen, Rainer$$iINSPIRE-00223881$$uKirchhoff Inst. Phys.
002255384 700__ $$aStamm, Soren$$iINSPIRE-00374679$$uHumboldt U., Berlin
002255384 700__ $$aStanecka, Ewa$$iINSPIRE-00223897$$uCracow, INP
002255384 700__ $$aStanek, Robert$$iINSPIRE-00128391$$uArgonne
002255384 700__ $$aStanescu, Cristian$$iINSPIRE-00128407$$uINFN, Rome
002255384 700__ $$aStanitzki, Marcel Michael$$iINSPIRE-00006638$$uDESY
002255384 700__ $$aStapnes, Steinar$$iINSPIRE-00223901$$uOslo U.
002255384 700__ $$aStarchenko, Evgeny$$iINSPIRE-00223911$$uSerpukhov, IHEP
002255384 700__ $$aStark, Giordon$$iINSPIRE-00434905$$uChicago U., EFI
002255384 700__ $$aStark, Jan$$iINSPIRE-00050567$$uLPSC, Grenoble
002255384 700__ $$aStark, Simon Holm$$iINSPIRE-00399764$$uBohr Inst.
002255384 700__ $$aStaroba, Pavel$$iINSPIRE-00223923$$uPrague, Inst. Phys.
002255384 700__ $$aStarovoitov, Pavel$$iINSPIRE-00223937$$uKirchhoff Inst. Phys.
002255384 700__ $$aStärz, Steffen$$iINSPIRE-00364781$$uCERN
002255384 700__ $$aStaszewski, Rafal$$iINSPIRE-00237571$$uCracow, INP
002255384 700__ $$aSteinberg, Peter$$iINSPIRE-00256449$$uBrookhaven
002255384 700__ $$aStelzer, Bernd$$iINSPIRE-00040738$$uSimon Fraser U.
002255384 700__ $$aStelzer, Harald Joerg$$iINSPIRE-00027247$$uCERN
002255384 700__ $$aStelzer-Chilton, Oliver$$iINSPIRE-00040726$$uTRIUMF
002255384 700__ $$aStenzel, Hasko$$iINSPIRE-00128831$$uGiessen U.
002255384 700__ $$aStewart, Graeme$$iINSPIRE-00226135$$uGlasgow U.
002255384 700__ $$aStillings, Jan Andre$$iINSPIRE-00237604$$uBonn U.
002255384 700__ $$aStockton, Mark$$iINSPIRE-00223972$$uMcGill U.
002255384 700__ $$aStoebe, Michael$$iINSPIRE-00329732$$uMcGill U.
002255384 700__ $$aStoicea, Gabriel$$iINSPIRE-00185869$$uBucharest, IFIN-HH
002255384 700__ $$aStolte, Philipp$$iINSPIRE-00362178$$uGottingen U., II. Phys. Inst.
002255384 700__ $$aStonjek, Stefan$$iINSPIRE-00027833$$uMunich, Max Planck Inst.
002255384 700__ $$aStradling, Alden$$iINSPIRE-00224005$$uTexas U., Arlington
002255384 700__ $$aStraessner, Arno$$iINSPIRE-00129196$$uDresden, Tech. U.
002255384 700__ $$aStramaglia, Maria Elena$$iINSPIRE-00372086$$uBern U., LHEP
002255384 700__ $$aStrandberg, Jonas$$iINSPIRE-00038640$$uRoyal Inst. Tech., Stockholm
002255384 700__ $$aStrandberg, Sara$$iINSPIRE-00024662$$uStockholm U.$$uStockholm U., OKC
002255384 700__ $$aStrandlie, Are$$iINSPIRE-00224010$$uOslo U.
002255384 700__ $$aStrauss, Michael$$iINSPIRE-00129297$$uOklahoma U.
002255384 700__ $$aStrizenec, Pavol$$iINSPIRE-00129337$$uKosice, IEF
002255384 700__ $$aStröhmer, Raimund$$iINSPIRE-00129353$$uWurzburg U.
002255384 700__ $$aStrom, David$$iINSPIRE-00129396$$uOregon U.
002255384 700__ $$aStroynowski, Ryszard$$iINSPIRE-00129434$$uSouthern Methodist U.
002255384 700__ $$aStrubig, Antonia$$iINSPIRE-00371025$$uNIKHEF, Amsterdam
002255384 700__ $$aStucci, Stefania Antonia$$iINSPIRE-00353969$$uBrookhaven
002255384 700__ $$aStugu, Bjarne$$iINSPIRE-00129469$$uBergen U.
002255384 700__ $$aStyles, Nicholas Adam$$iINSPIRE-00049529$$uDESY
002255384 700__ $$aSu, Dong$$iINSPIRE-00224038$$uSLAC
002255384 700__ $$aSu, Jun$$iINSPIRE-00354087$$uPittsburgh U.
002255384 700__ $$aSuchek, Stanislav$$iINSPIRE-00366364$$uKirchhoff Inst. Phys.
002255384 700__ $$aSugaya, Yorihito$$iINSPIRE-00224054$$uOsaka U.
002255384 700__ $$aSuk, Michal$$iINSPIRE-00224089$$uPrague, Tech. U.
002255384 700__ $$aSulin, Vladimir$$iINSPIRE-00224090$$uLebedev Inst.
002255384 700__ $$aSultansoy, Saleh$$iINSPIRE-00009070$$uTOBB ETU, Ankara
002255384 700__ $$aSumida, Toshi$$iINSPIRE-00129684$$uKyoto U.
002255384 700__ $$aSun, Siyuan$$iINSPIRE-00375257$$uHarvard U., Phys. Dept.
002255384 700__ $$aSun, Xiaohu$$iINSPIRE-00226957$$uAlberta U.
002255384 700__ $$aSuruliz, Kerim$$iINSPIRE-00224106$$uSussex U.
002255384 700__ $$aSuster, Carl$$iINSPIRE-00511778$$uSydney U.
002255384 700__ $$aSutton, Mark$$iINSPIRE-00129913$$uSussex U.
002255384 700__ $$aSuzuki, Shota$$iINSPIRE-00394929$$uKEK, Tsukuba
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002255384 700__ $$aSwiatlowski, Maximilian$$iINSPIRE-00333637$$uChicago U., EFI
002255384 700__ $$aSwift, Stewart Patrick$$iINSPIRE-00529784$$uSUNY, Albany
002255384 700__ $$aSykora, Ivan$$iINSPIRE-00224134$$uComenius U.
002255384 700__ $$aSykora, Tomas$$iINSPIRE-00185883$$uCharles U.
002255384 700__ $$aTa, Duc$$iINSPIRE-00224156$$uFreiburg U.
002255384 700__ $$aTackmann, Kerstin$$iINSPIRE-00024648$$uDESY
002255384 700__ $$aTaenzer, Joe$$iINSPIRE-00354235$$uTel Aviv U.
002255384 700__ $$aTaffard, Anyes$$iINSPIRE-00054866$$uUC, Irvine
002255384 700__ $$aTafirout, Reda$$iINSPIRE-00224168$$uTRIUMF
002255384 700__ $$aTaiblum, Nimrod$$iINSPIRE-00232703$$uTel Aviv U.
002255384 700__ $$aTakai, Helio$$iINSPIRE-99155656$$uBrookhaven
002255384 700__ $$aTakashima, Ryuichi$$iINSPIRE-00130375$$uKyoto U. of Education
002255384 700__ $$aTakeshita, Tohru$$iINSPIRE-00224192$$uShinshu U.
002255384 700__ $$aTakubo, Yosuke$$iINSPIRE-00237659$$uKEK, Tsukuba
002255384 700__ $$aTalby, Mossadek$$iINSPIRE-00224200$$uMarseille, CPPM
002255384 700__ $$aTalyshev, Alexey$$iINSPIRE-00224212$$uNovosibirsk State U.$$uNovosibirsk, IYF
002255384 700__ $$aTanaka, Junichi$$iINSPIRE-00224238$$uTokyo U., ICEPP
002255384 700__ $$aTanaka, Masahiro$$iINSPIRE-00514556$$uTokyo Inst. Tech.
002255384 700__ $$aTanaka, Reisaburo$$iINSPIRE-00130555$$uOrsay, LAL
002255384 700__ $$aTanaka, Shuji$$iINSPIRE-00224249$$uKEK, Tsukuba
002255384 700__ $$aTanioka, Ryo$$iINSPIRE-00529792$$uKobe U.
002255384 700__ $$aTannenwald, Benjamin Bordy$$iINSPIRE-00375951$$uOhio State U.
002255384 700__ $$aTapia Araya, Sebastian$$iINSPIRE-00424626$$uSanta Maria U., Valparaiso
002255384 700__ $$aTapprogge, Stefan$$iINSPIRE-00141544$$uMainz U.
002255384 700__ $$aTarem, Shlomit$$iINSPIRE-00130701$$uTechnion
002255384 700__ $$aTartarelli, Giuseppe Francesco$$iINSPIRE-00130743$$uINFN, Milan
002255384 700__ $$aTas, Petr$$iINSPIRE-00306326$$uCharles U.
002255384 700__ $$aTasevsky, Marek$$iINSPIRE-00224260$$uPrague, Inst. Phys.
002255384 700__ $$aTashiro, Takuya$$iINSPIRE-00340474$$uKyoto U.
002255384 700__ $$aTassi, Enrico$$iINSPIRE-00172313$$uINFN, Cosenza$$uCalabria U.
002255384 700__ $$aTavares Delgado, Ademar$$iINSPIRE-00342767$$uLIP, Lisbon$$uLisbon U., CFNUL
002255384 700__ $$aTayalati, Yahya$$iINSPIRE-00295930$$uMohammed V U., Agdal
002255384 700__ $$aTaylor, Aaron$$iINSPIRE-00388427$$uNew Mexico U.
002255384 700__ $$aTaylor, Geoffrey$$iINSPIRE-00130854$$uMelbourne U.
002255384 700__ $$aTaylor, Pierre Thor Elliot$$iINSPIRE-00418209$$uMelbourne U.
002255384 700__ $$aTaylor, Wendy$$iINSPIRE-00301147$$uYork U., Canada
002255384 700__ $$aTeixeira-Dias, Pedro$$iINSPIRE-00130949$$uRoyal Holloway, U. of London
002255384 700__ $$aTemple, Darren$$iINSPIRE-00431697$$uSimon Fraser U.
002255384 700__ $$aTen Kate, Herman$$iINSPIRE-00224330$$uCERN
002255384 700__ $$aTeng, Ping-Kun$$iINSPIRE-00040709$$uTaiwan, Inst. Phys.
002255384 700__ $$aTeoh, Jia Jian$$iINSPIRE-00371033$$uOsaka U.
002255384 700__ $$aTepel, Fabian-Phillipp$$iINSPIRE-00379384$$uWuppertal U.
002255384 700__ $$aTerada, Susumu$$iINSPIRE-00224350$$uKEK, Tsukuba
002255384 700__ $$aTerashi, Koji$$iINSPIRE-00131056$$uTokyo U., ICEPP
002255384 700__ $$aTerron, Juan$$iINSPIRE-00145489$$uMadrid, Autonoma U.
002255384 700__ $$aTerzo, Stefano$$iINSPIRE-00349918$$uBarcelona, IFAE
002255384 700__ $$aTesta, Marianna$$iINSPIRE-00224377$$uFrascati
002255384 700__ $$aTeuscher, Richard$$iINSPIRE-00131201$$uToronto U.$$uIPP, Canada
002255384 700__ $$aTheveneaux-Pelzer, Timothée$$iINSPIRE-00224394$$uMarseille, CPPM
002255384 700__ $$aThomas, Juergen$$iINSPIRE-00224412$$uBirmingham U.
002255384 700__ $$aThomas-Wilsker, Joshuha$$iINSPIRE-00357035$$uRoyal Holloway, U. of London
002255384 700__ $$aThompson, Paul$$iINSPIRE-00185894$$uBirmingham U.
002255384 700__ $$aThompson, Stan$$iINSPIRE-00131382$$uGlasgow U.
002255384 700__ $$aThomsen, Lotte Ansgaard$$iINSPIRE-00287293$$uYale U.
002255384 700__ $$aThomson, Evelyn$$iINSPIRE-00300284$$uPennsylvania U.
002255384 700__ $$aTibbetts, Mark James$$iINSPIRE-00025280$$uLBL, Berkeley
002255384 700__ $$aTicse Torres, Royer Edson$$iINSPIRE-00388508$$uMarseille, CPPM
002255384 700__ $$aTikhomirov, Vladimir$$iINSPIRE-00306337$$uLebedev Inst.$$uMoscow Phys. Eng. Inst.
002255384 700__ $$aTikhonov, Yury$$iINSPIRE-00198040$$uNovosibirsk State U.$$uNovosibirsk, IYF
002255384 700__ $$aTimoshenko, Sergey$$iINSPIRE-00183342$$uMoscow Phys. Eng. Inst.
002255384 700__ $$aTipton, Paul$$iINSPIRE-00131560$$uYale U.
002255384 700__ $$aTisserant, Sylvain$$iINSPIRE-00131587$$uMarseille, CPPM
002255384 700__ $$aTodome, Kazuki$$iINSPIRE-00410948$$uTokyo Inst. Tech.
002255384 700__ $$aTodorova-Nova, Sharka$$iINSPIRE-00224498$$uAnnecy, LAPP
002255384 700__ $$aTojo, Junji$$iINSPIRE-00243319$$uKyushu U.
002255384 700__ $$aTokár, Stanislav$$iINSPIRE-00131686$$uComenius U.
002255384 700__ $$aTokushuku, Katsuo$$iINSPIRE-00173305$$uKEK, Tsukuba
002255384 700__ $$aTolley, Emma$$iINSPIRE-00377126$$uHarvard U., Phys. Dept.
002255384 700__ $$aTomlinson, Lee$$iINSPIRE-00337682$$uManchester U.
002255384 700__ $$aTomoto, Makoto$$iINSPIRE-00131811$$uNagoya U.
002255384 700__ $$aTompkins, Lauren$$iINSPIRE-00059527$$uSLAC$$uStanford U., Phys. Dept.
002255384 700__ $$aToms, Konstantin$$iINSPIRE-00224527$$uNew Mexico U.
002255384 700__ $$aTong, Baojia(Tony)$$iINSPIRE-00436984$$uHarvard U., Phys. Dept.
002255384 700__ $$aTornambe, Peter$$iINSPIRE-00529818$$uFreiburg U.
002255384 700__ $$aTorrence, Eric$$iINSPIRE-00144881$$uOregon U.
002255384 700__ $$aTorres, Heberth$$iINSPIRE-00237687$$uSimon Fraser U.
002255384 700__ $$aTorró Pastor, Emma$$iINSPIRE-00224567$$uWashington U., Seattle
002255384 700__ $$aToth, Jozsef$$iINSPIRE-00226986$$uMarseille, CPPM$$uBudapest, RMKI
002255384 700__ $$aTouchard, Francois$$iINSPIRE-00224579$$uMarseille, CPPM
002255384 700__ $$aTovey, Daniel$$iINSPIRE-00224589$$uSheffield U.
002255384 700__ $$aTreado, Colleen Jennifer$$iINSPIRE-00534702$$uNew York U.
002255384 700__ $$aTrefzger, Thomas$$iINSPIRE-00224598$$uWurzburg U.
002255384 700__ $$aTricoli, Alessandro$$iINSPIRE-00224619$$uBrookhaven
002255384 700__ $$aTrigger, Isabel Marian$$iINSPIRE-00132228$$uTRIUMF
002255384 700__ $$aTrincaz-Duvoid, Sophie$$iINSPIRE-00132232$$uParis U., VI-VII
002255384 700__ $$aTripiana, Martin$$iINSPIRE-00224624$$uBarcelona, IFAE
002255384 700__ $$aTrischuk, William$$iINSPIRE-00132286$$uToronto U.
002255384 700__ $$aTrocmé, Benjamin$$iINSPIRE-00224658$$uLPSC, Grenoble
002255384 700__ $$aTrofymov, Artur$$iINSPIRE-00443508$$uDESY
002255384 700__ $$aTroncon, Clara$$iINSPIRE-00132324$$uINFN, Milan
002255384 700__ $$aTrottier-McDonald, Michel$$iINSPIRE-00300515$$uLBL, Berkeley
002255384 700__ $$aTrovatelli, Monica$$iINSPIRE-00335615$$uVictoria U.
002255384 700__ $$aTruong, Loan$$iINSPIRE-00444174$$uINFN, Udine$$uUdine U.
002255384 700__ $$aTrzebinski, Maciej$$iINSPIRE-00237700$$uCracow, INP
002255384 700__ $$aTrzupek, Adam$$iINSPIRE-00256459$$uCracow, INP
002255384 700__ $$aTsang, Ka Wa$$iINSPIRE-00534716$$uHong Kong, Chinese U.
002255384 700__ $$aTseng, Jeffrey$$iINSPIRE-00224674$$uOxford U.
002255384 700__ $$aTsiareshka, Pavel$$iINSPIRE-00224691$$uMinsk, Inst. Phys.
002255384 700__ $$aTsipolitis, Georgios$$iINSPIRE-00159427$$uNatl. Tech. U., Athens
002255384 700__ $$aTsirintanis, Nikolaos$$iINSPIRE-00346988$$uAthens U.
002255384 700__ $$aTsiskaridze, Shota$$iINSPIRE-00287516$$uBarcelona, IFAE
002255384 700__ $$aTsiskaridze, Vakhtang$$iINSPIRE-00224710$$uFreiburg U.
002255384 700__ $$aTskhadadze, Edisher$$iINSPIRE-00224724$$uTbilisi, Inst. Phys.
002255384 700__ $$aTsui, Ka Ming$$iINSPIRE-00437088$$uHong Kong, Chinese U.
002255384 700__ $$aTsukerman, Ilya$$iINSPIRE-00224734$$uMoscow, ITEP
002255384 700__ $$aTsulaia, Vakhtang$$iINSPIRE-00224746$$uLBL, Berkeley
002255384 700__ $$aTsuno, Soshi$$iINSPIRE-00040679$$uKEK, Tsukuba
002255384 700__ $$aTsybychev, Dmitri$$iINSPIRE-00132531$$uSUNY, Stony Brook
002255384 700__ $$aTu, Yanjun$$iINSPIRE-00024619$$uHong Kong U.
002255384 700__ $$aTudorache, Alexandra$$iINSPIRE-00237716$$uBucharest, IFIN-HH
002255384 700__ $$aTudorache, Valentina$$iINSPIRE-00237721$$uBucharest, IFIN-HH
002255384 700__ $$aTulbure, Traian Tiberiu$$iINSPIRE-00517222$$uTransilvania U., Brasov
002255384 700__ $$aTuna, Alexander Naip$$iINSPIRE-00337698$$uHarvard U., Phys. Dept.
002255384 700__ $$aTupputi, Salvatore$$iINSPIRE-00313600$$uINFN, Bologna$$uBologna U.
002255384 700__ $$aTurchikhin, Semen$$iINSPIRE-00342946$$uDubna, JINR
002255384 700__ $$aTurgeman, Daniel$$iINSPIRE-00437130$$uWeizmann Inst.
002255384 700__ $$aTurk Cakir, Ilkay$$iINSPIRE-00224776$$uIstanbul Aydin U.$$uGiresun U.
002255384 700__ $$aTurra, Ruggero$$iINSPIRE-00237738$$uINFN, Milan$$uMilan U.
002255384 700__ $$aTuts, Michael$$iINSPIRE-00132751$$uNevis Labs, Columbia U.
002255384 700__ $$aUcchielli, Giulia$$iINSPIRE-00444244$$uINFN, Bologna$$uBologna U.
002255384 700__ $$aUeda, Ikuo$$iINSPIRE-00224805$$uKEK, Tsukuba
002255384 700__ $$aUghetto, Michael$$iINSPIRE-00334596$$uStockholm U.$$uStockholm U., OKC
002255384 700__ $$aUkegawa, Fumihiko$$iINSPIRE-00132910$$uTsukuba U.
002255384 700__ $$aUnal, Guillaume$$iINSPIRE-00132979$$uCERN
002255384 700__ $$aUndrus, Alexander$$iINSPIRE-00132984$$uBrookhaven
002255384 700__ $$aUnel, Gokhan$$iINSPIRE-00132990$$uUC, Irvine
002255384 700__ $$aUngaro, Francesca$$iINSPIRE-00334608$$uMelbourne U.
002255384 700__ $$aUnno, Yoshinobu$$iINSPIRE-00133014$$uKEK, Tsukuba
002255384 700__ $$aUnverdorben, Christopher$$iINSPIRE-00530015$$uMunich U.
002255384 700__ $$aUrban, Jozef$$iINSPIRE-00244950$$uKosice, IEF
002255384 700__ $$aUrquijo, Phillip$$iINSPIRE-00227284$$uMelbourne U.
002255384 700__ $$aUrrejola, Pedro$$iINSPIRE-00226996$$uMainz U.
002255384 700__ $$aUsai, Giulio$$iINSPIRE-00224879$$uTexas U., Arlington
002255384 700__ $$aUsui, Junya$$iINSPIRE-00529820$$uKEK, Tsukuba
002255384 700__ $$aVacavant, Laurent$$iINSPIRE-00179395$$uMarseille, CPPM
002255384 700__ $$aVacek, Vaclav$$iINSPIRE-00227000$$uPrague, Tech. U.
002255384 700__ $$aVachon, Brigitte$$iINSPIRE-00056509$$uMcGill U.
002255384 700__ $$aValderanis, Chrysostomos$$iINSPIRE-00232811$$uMunich U.
002255384 700__ $$aValdes Santurio, Eduardo$$iINSPIRE-00441276$$uStockholm U.$$uStockholm U., OKC
002255384 700__ $$aValencic, Nika$$iINSPIRE-00335628$$uFOM, Amsterdam
002255384 700__ $$aValentinetti, Sara$$iINSPIRE-00224911$$uINFN, Bologna$$uBologna U.
002255384 700__ $$aValero, Alberto$$iINSPIRE-00306349$$uValencia U., IFIC
002255384 700__ $$aValéry, Loic$$iINSPIRE-00334610$$uBarcelona, IFAE
002255384 700__ $$aValkar, Stefan$$iINSPIRE-00224924$$uCharles U.
002255384 700__ $$aVallier, Alexis$$iINSPIRE-00392294$$uAnnecy, LAPP
002255384 700__ $$aValls Ferrer, Juan Antonio$$iINSPIRE-00224946$$uValencia U., IFIC
002255384 700__ $$aVan Den Wollenberg, Wouter$$iINSPIRE-00374702$$uFOM, Amsterdam
002255384 700__ $$avan der Graaf, Harry$$iINSPIRE-00224951$$uFOM, Amsterdam
002255384 700__ $$avan Eldik, Niels$$iINSPIRE-00224996$$uTechnion
002255384 700__ $$avan Gemmeren, Peter$$iINSPIRE-00084279$$uArgonne
002255384 700__ $$aVan Nieuwkoop, Jacobus$$iINSPIRE-00354211$$uSimon Fraser U.
002255384 700__ $$avan Vulpen, Ivo$$iINSPIRE-00225014$$uFOM, Amsterdam
002255384 700__ $$avan Woerden, Marius Cornelis$$iINSPIRE-00352208$$uFOM, Amsterdam
002255384 700__ $$aVanadia, Marco$$iINSPIRE-00237763$$uINFN, Rome$$uRome U.
002255384 700__ $$aVandelli, Wainer$$iINSPIRE-00306351$$uCERN
002255384 700__ $$aVanguri, Rami$$iINSPIRE-00025259$$uPennsylvania U.
002255384 700__ $$aVaniachine, Alexandre$$iINSPIRE-00133440$$uTomsk State U.
002255384 700__ $$aVankov, Peter$$iINSPIRE-00225024$$uFOM, Amsterdam
002255384 700__ $$aVardanyan, Gagik$$iINSPIRE-00354109$$uYerevan Phys. Inst.
002255384 700__ $$aVari, Riccardo$$iINSPIRE-00225039$$uINFN, Rome
002255384 700__ $$aVarnes, Erich$$iINSPIRE-00133542$$uArizona U.
002255384 700__ $$aVarni, Carlo$$iINSPIRE-00534739$$uINFN, Genoa$$uGenoa U.
002255384 700__ $$aVarol, Tulin$$iINSPIRE-00287318$$uSouthern Methodist U.
002255384 700__ $$aVarouchas, Dimitris$$iINSPIRE-00225042$$uParis U., VI-VII
002255384 700__ $$aVartapetian, Armen$$iINSPIRE-00225055$$uTexas U., Arlington
002255384 700__ $$aVarvell, Kevin$$iINSPIRE-00225063$$uSydney U.
002255384 700__ $$aVasquez, Jared Gregory$$iINSPIRE-00265075$$uYale U.
002255384 700__ $$aVasquez, Gerardo$$iINSPIRE-00529830$$uSanta Maria U., Valparaiso
002255384 700__ $$aVazeille, Francois$$iINSPIRE-00225072$$uClermont-Ferrand U.
002255384 700__ $$aVazquez Schroeder, Tamara$$iINSPIRE-00237778$$uMcGill U.
002255384 700__ $$aVeatch, Jason$$iINSPIRE-00354304$$uGottingen U., II. Phys. Inst.
002255384 700__ $$aVeeraraghavan, Venkatesh$$iINSPIRE-00192035$$uArizona U.
002255384 700__ $$aVeloce, Laurelle Maria$$iINSPIRE-00406224$$uToronto U.
002255384 700__ $$aVeloso, Filipe$$iINSPIRE-00034280$$uLIP, Lisbon$$uCoimbra U.
002255384 700__ $$aVeneziano, Stefano$$iINSPIRE-00225080$$uINFN, Rome
002255384 700__ $$aVentura, Andrea$$iINSPIRE-00058029$$uINFN, Lecce$$uSalento U.
002255384 700__ $$aVenturi, Manuela$$iINSPIRE-00225109$$uVictoria U.
002255384 700__ $$aVenturi, Nicola$$iINSPIRE-00225111$$uToronto U.
002255384 700__ $$aVenturini, Alessio$$iINSPIRE-00354311$$uBrandeis U.
002255384 700__ $$aVercesi, Valerio$$iINSPIRE-00140154$$uINFN, Pavia
002255384 700__ $$aVerducci, Monica$$iINSPIRE-00225123$$uINFN, Rome$$uRome III U.
002255384 700__ $$aVerkerke, Wouter$$iINSPIRE-00029133$$uFOM, Amsterdam
002255384 700__ $$aVermeulen, Jos$$iINSPIRE-00140176$$uFOM, Amsterdam
002255384 700__ $$aVetterli, Michel$$iINSPIRE-00133870$$uSimon Fraser U.$$uTRIUMF
002255384 700__ $$aViaux Maira, Nicolas$$iINSPIRE-00384010$$uChile U., Catolica
002255384 700__ $$aViazlo, Oleksandr$$iINSPIRE-00184482$$uLund U.
002255384 700__ $$aVichou, Irene$$iINSPIRE-00161358$$uIllinois U., Urbana
002255384 700__ $$aVickey, Trevor$$iINSPIRE-00052371$$uSheffield U.
002255384 700__ $$aVickey Boeriu, Oana Elena$$iINSPIRE-00237790$$uSheffield U.
002255384 700__ $$aViehhauser, Georg$$iINSPIRE-00225132$$uOxford U.
002255384 700__ $$aViel, Simon$$iINSPIRE-00232885$$uLBL, Berkeley
002255384 700__ $$aVigani, Luigi$$iINSPIRE-00427277$$uOxford U.
002255384 700__ $$aVilla, Mauro$$iINSPIRE-00225145$$uINFN, Bologna$$uBologna U.
002255384 700__ $$aVillaplana Perez, Miguel$$iINSPIRE-00225163$$uINFN, Milan$$uMilan U.
002255384 700__ $$aVilucchi, Elisabetta$$iINSPIRE-00225177$$uFrascati
002255384 700__ $$aVincter, Manuella$$iINSPIRE-00133971$$uCarleton U.
002255384 700__ $$aVinogradov, Vladimir$$iINSPIRE-00227012$$uDubna, JINR
002255384 700__ $$aVishwakarma, Akanksha$$iINSPIRE-00529840$$uDESY
002255384 700__ $$aVittori, Camilla$$iINSPIRE-00453010$$uINFN, Bologna$$uBologna U.
002255384 700__ $$aVivarelli, Iacopo$$iINSPIRE-00016420$$uSussex U.
002255384 700__ $$aVlachos, Sotirios$$iINSPIRE-00134107$$uNatl. Tech. U., Athens
002255384 700__ $$aVlasak, Michal$$iINSPIRE-00225228$$uPrague, Tech. U.
002255384 700__ $$aVogel, Marcelo$$iINSPIRE-00009675$$uWuppertal U.
002255384 700__ $$aVokac, Petr$$iINSPIRE-00007099$$uPrague, Tech. U.
002255384 700__ $$aVolpi, Guido$$iINSPIRE-00040623$$uINFN, Pisa$$uPisa U.
002255384 700__ $$aVolpi, Matteo$$iINSPIRE-00306360$$uMelbourne U.
002255384 700__ $$avon der Schmitt, Hans$$iINSPIRE-00225242$$uMunich, Max Planck Inst.
002255384 700__ $$avon Toerne, Eckhard$$iINSPIRE-00058359$$uBonn U.
002255384 700__ $$aVorobel, Vit$$iINSPIRE-00188264$$uCharles U.
002255384 700__ $$aVorobev, Konstantin$$iINSPIRE-00364793$$uMoscow Phys. Eng. Inst.
002255384 700__ $$aVos, Marcel$$iINSPIRE-00240580$$uValencia U., IFIC
002255384 700__ $$aVoss, Rudiger$$iINSPIRE-00134334$$uCERN
002255384 700__ $$aVossebeld, Joost$$iINSPIRE-00134340$$uLiverpool U.
002255384 700__ $$aVranjes, Nenad$$iINSPIRE-00225275$$uBelgrade U.
002255384 700__ $$aVranjes Milosavljevic, Marija$$iINSPIRE-00225280$$uBelgrade U.
002255384 700__ $$aVrba, Vaclav$$iINSPIRE-00134373$$uPrague, Tech. U.
002255384 700__ $$aVreeswijk, Marcel$$iINSPIRE-00225293$$uFOM, Amsterdam
002255384 700__ $$aVuillermet, Raphael$$iINSPIRE-00225322$$uCERN
002255384 700__ $$aVukotic, Ilija$$iINSPIRE-00225336$$uChicago U., EFI
002255384 700__ $$aWagner, Peter$$iINSPIRE-00052760$$uBonn U.
002255384 700__ $$aWagner, Wolfgang$$iINSPIRE-00051400$$uWuppertal U.
002255384 700__ $$aWahlberg, Hernan$$iINSPIRE-00153915$$uLa Plata U.
002255384 700__ $$aWahrmund, Sebastian$$iINSPIRE-00233070$$uDresden, Tech. U.
002255384 700__ $$aWakabayashi, Jun$$iINSPIRE-00233085$$uNagoya U.
002255384 700__ $$aWalder, James$$iINSPIRE-00007572$$uLancaster U.
002255384 700__ $$aWalker, Rodney$$iINSPIRE-00225350$$uMunich U.
002255384 700__ $$aWalkowiak, Wolfgang$$iINSPIRE-00134689$$uSiegen U.
002255384 700__ $$aWallangen, Veronica$$iINSPIRE-00441545$$uStockholm U.$$uStockholm U., OKC
002255384 700__ $$aWang, Chao$$iINSPIRE-00356629$$uNanjing U.
002255384 700__ $$aWang, Chao$$iINSPIRE-00439918$$uShandong U.$$uMarseille, CPPM
002255384 700__ $$aWang, Fuquan$$iINSPIRE-00357049$$uWisconsin U., Madison
002255384 700__ $$aWang, Haichen$$iINSPIRE-00225389$$uLBL, Berkeley
002255384 700__ $$aWang, Hulin$$iINSPIRE-00237831$$uAlberta U.
002255384 700__ $$aWang, Jike$$iINSPIRE-00287547$$uDESY
002255384 700__ $$aWang, Jin$$iINSPIRE-00225390$$uSydney U.
002255384 700__ $$aWang, Qing$$iINSPIRE-00507962$$uOklahoma U.
002255384 700__ $$aWang, Rui$$iINSPIRE-00237848$$uArgonne
002255384 700__ $$aWang, Song-Ming$$iINSPIRE-00134900$$uTaiwan, Inst. Phys.
002255384 700__ $$aWang, Tingting$$iINSPIRE-00408529$$uNevis Labs, Columbia U.
002255384 700__ $$aWang, Wei$$iINSPIRE-00533069$$uTaiwan, Inst. Phys.$$uNanjing U.
002255384 700__ $$aWang, Wenxiao$$iINSPIRE-00449272$$uHefei, CUST
002255384 700__ $$aWanotayaroj, Chaowaroj$$iINSPIRE-00366124$$uOregon U.
002255384 700__ $$aWarburton, Andreas$$iINSPIRE-00134957$$uMcGill U.
002255384 700__ $$aWard, Patricia$$iINSPIRE-00034528$$uCambridge U.
002255384 700__ $$aWardrope, David Robert$$iINSPIRE-00305495$$uUniversity Coll. London
002255384 700__ $$aWashbrook, Andrew$$iINSPIRE-00287555$$uEdinburgh U.
002255384 700__ $$aWatkins, Peter$$iINSPIRE-00225418$$uBirmingham U.
002255384 700__ $$aWatson, Alan$$iINSPIRE-00135097$$uBirmingham U.
002255384 700__ $$aWatson, Miriam$$iINSPIRE-00225428$$uBirmingham U.
002255384 700__ $$aWatts, Gordon$$iINSPIRE-00135120$$uWashington U., Seattle
002255384 700__ $$aWatts, Stephen$$iINSPIRE-00003412$$uManchester U.
002255384 700__ $$aWaugh, Ben$$iINSPIRE-00145415$$uUniversity Coll. London
002255384 700__ $$aWebb, Aaron Foley$$iINSPIRE-00536691$$uTexas U.
002255384 700__ $$aWebb, Samuel$$iINSPIRE-00345617$$uMainz U.
002255384 700__ $$aWeber, Michele$$iINSPIRE-00135206$$uBern U., LHEP
002255384 700__ $$aWeber, Stefan Wolf$$iINSPIRE-00349929$$uWurzburg U.
002255384 700__ $$aWeber, Stephen$$iINSPIRE-00529858$$uCarleton U.
002255384 700__ $$aWebster, Jordan S$$iINSPIRE-00291974$$uArgonne
002255384 700__ $$aWeidberg, Anthony$$iINSPIRE-00148085$$uOxford U.
002255384 700__ $$aWeinert, Benjamin$$iINSPIRE-00359706$$uIndiana U.
002255384 700__ $$aWeingarten, Jens$$iINSPIRE-00225459$$uGottingen U., II. Phys. Inst.
002255384 700__ $$aWeiser, Christian$$iINSPIRE-00225468$$uFreiburg U.
002255384 700__ $$aWeits, Hartger$$iINSPIRE-00342786$$uFOM, Amsterdam
002255384 700__ $$aWells, Phillippa$$iINSPIRE-00225479$$uCERN
002255384 700__ $$aWenaus, Torre$$iINSPIRE-00135450$$uBrookhaven
002255384 700__ $$aWengler, Thorsten$$iINSPIRE-00145320$$uCERN
002255384 700__ $$aWenig, Siegfried$$iINSPIRE-00145513$$uCERN
002255384 700__ $$aWermes, Norbert$$iINSPIRE-00135524$$uBonn U.
002255384 700__ $$aWerner, Michael David$$iINSPIRE-00433265$$uIowa State U.
002255384 700__ $$aWerner, Per$$iINSPIRE-00225665$$uCERN
002255384 700__ $$aWessels, Martin$$iINSPIRE-00217771$$uKirchhoff Inst. Phys.
002255384 700__ $$aWhalen, Kathleen$$iINSPIRE-00225692$$uOregon U.
002255384 700__ $$aWhallon, Nikola Lazar$$iINSPIRE-00444316$$uWashington U., Seattle
002255384 700__ $$aWharton, Andrew Mark$$iINSPIRE-00390886$$uLancaster U.
002255384 700__ $$aWhite, Andrew$$iINSPIRE-00013505$$uTexas U., Arlington
002255384 700__ $$aWhite, Martin$$iINSPIRE-00162417$$uAdelaide U., Sch. Chem. Phys.
002255384 700__ $$aWhite, Ryan$$iINSPIRE-00003676$$uSanta Maria U., Valparaiso
002255384 700__ $$aWhiteson, Daniel$$iINSPIRE-00054720$$uUC, Irvine
002255384 700__ $$aWickens, Fred$$iINSPIRE-00135820$$uRutherford
002255384 700__ $$aWiedenmann, Werner$$iINSPIRE-00225736$$uWisconsin U., Madison
002255384 700__ $$aWielers, Monika$$iINSPIRE-00225743$$uRutherford
002255384 700__ $$aWiglesworth, Craig$$iINSPIRE-00225769$$uBohr Inst.
002255384 700__ $$aWiik-Fuchs, Liv Antje Mari$$iINSPIRE-00225778$$uBonn U.
002255384 700__ $$aWildauer, Andreas$$iINSPIRE-00225788$$uMunich, Max Planck Inst.
002255384 700__ $$aWilk, Fabian$$iINSPIRE-00401313$$uManchester U.
002255384 700__ $$aWilkens, Henric George$$iINSPIRE-00225806$$uCERN
002255384 700__ $$aWilliams, Hugh$$iINSPIRE-00136066$$uPennsylvania U.
002255384 700__ $$aWilliams, Sarah$$iINSPIRE-00287350$$uFOM, Amsterdam
002255384 700__ $$aWillis, Christopher$$iINSPIRE-00358369$$uMichigan State U.
002255384 700__ $$aWillocq, Stephane$$iINSPIRE-00136116$$uMassachusetts U., Amherst
002255384 700__ $$aWilson, John$$iINSPIRE-00154108$$uBirmingham U.
002255384 700__ $$aWingerter-Seez, Isabelle$$iINSPIRE-00136245$$uAnnecy, LAPP
002255384 700__ $$aWinklmeier, Frank$$iINSPIRE-00042764$$uOregon U.
002255384 700__ $$aWinston, Oliver James$$iINSPIRE-00443634$$uSussex U.
002255384 700__ $$aWinter, Benedict Tobias$$iINSPIRE-00371046$$uBonn U.
002255384 700__ $$aWittgen, Matthias$$iINSPIRE-00041794$$uSLAC
002255384 700__ $$aWobisch, Markus$$iINSPIRE-00136413$$uLouisiana Tech. U.
002255384 700__ $$aWolf, Tim Michael Heinz$$iINSPIRE-00439983$$uFOM, Amsterdam
002255384 700__ $$aWolff, Robert$$iINSPIRE-00533076$$uMarseille, CPPM
002255384 700__ $$aWolter, Marcin Wladyslaw$$iINSPIRE-00136528$$uCracow, INP
002255384 700__ $$aWolters, Helmut$$iINSPIRE-00225832$$uLIP, Lisbon$$uCoimbra U.
002255384 700__ $$aWorm, Steven$$iINSPIRE-00145331$$uBirmingham U.
002255384 700__ $$aWosiek, Barbara$$iINSPIRE-00256470$$uCracow, INP
002255384 700__ $$aWotschack, Jorg$$iINSPIRE-00136696$$uCERN
002255384 700__ $$aWoudstra, Martin$$iINSPIRE-00136715$$uManchester U.
002255384 700__ $$aWozniak, Krzysztof$$iINSPIRE-00256486$$uCracow, INP
002255384 700__ $$aWu, Miles$$iINSPIRE-00390966$$uChicago U., EFI
002255384 700__ $$aWu, Sau Lan$$iINSPIRE-00136809$$uWisconsin U., Madison
002255384 700__ $$aWu, Xin$$iINSPIRE-00306899$$uGeneva U.
002255384 700__ $$aWu, Yusheng$$iINSPIRE-00237882$$uMichigan U.
002255384 700__ $$aWyatt, Terry Richard$$iINSPIRE-00136898$$uManchester U.
002255384 700__ $$aWynne, Benjamin$$iINSPIRE-00225867$$uEdinburgh U.
002255384 700__ $$aXella, Stefania$$iINSPIRE-00027688$$uBohr Inst.
002255384 700__ $$aXi, Zhaoxu$$iINSPIRE-00508949$$uMichigan U.
002255384 700__ $$aXia, Ligang$$iINSPIRE-00446504$$uTsinghua U., Beijing
002255384 700__ $$aXu, Da$$iINSPIRE-00225894$$uBeijing, Inst. High Energy Phys.
002255384 700__ $$aXu, Lailin$$iINSPIRE-00329742$$uBrookhaven
002255384 700__ $$aYabsley, Bruce$$iINSPIRE-00137014$$uSydney U.
002255384 700__ $$aYacoob, Sahal$$iINSPIRE-00038563$$uCape Town U.
002255384 700__ $$aYamaguchi, Daiki$$iINSPIRE-00413207$$uTokyo Inst. Tech.
002255384 700__ $$aYamaguchi, Yohei$$iINSPIRE-00336655$$uOsaka U.
002255384 700__ $$aYamamoto, Akira$$iINSPIRE-00225925$$uKEK, Tsukuba
002255384 700__ $$aYamamoto, Shimpei$$iINSPIRE-00227035$$uTokyo U., ICEPP
002255384 700__ $$aYamanaka, Takashi$$iINSPIRE-00237916$$uTokyo U., ICEPP
002255384 700__ $$aYamauchi, Katsuya$$iINSPIRE-00332132$$uNagoya U.
002255384 700__ $$aYamazaki, Yuji$$iINSPIRE-00173319$$uKobe U.
002255384 700__ $$aYan, Zhen$$iINSPIRE-00225940$$uBoston U.
002255384 700__ $$aYang, Haijun$$iINSPIRE-00059882$$uShanghai Jiao Tong U.
002255384 700__ $$aYang, Hongtao$$iINSPIRE-00336678$$uLBL, Berkeley
002255384 700__ $$aYang, Yi$$iINSPIRE-00227069$$uTaiwan, Inst. Phys.
002255384 700__ $$aYang, Zongchang$$iINSPIRE-00313020$$uBergen U.
002255384 700__ $$aYao, Weiming$$iINSPIRE-00137324$$uLBL, Berkeley
002255384 700__ $$aYap, Yee Chinn$$iINSPIRE-00441752$$uParis U., VI-VII
002255384 700__ $$aYasu, Yoshiji$$iINSPIRE-00225960$$uKEK, Tsukuba
002255384 700__ $$aYatsenko, Elena$$iINSPIRE-00333129$$uAnnecy, LAPP
002255384 700__ $$aYau Wong, Kaven Henry$$iINSPIRE-00339178$$uBonn U.
002255384 700__ $$aYe, Jingbo$$iINSPIRE-00226177$$uSouthern Methodist U.
002255384 700__ $$aYe, Shuwei$$iINSPIRE-00139045$$uBrookhaven
002255384 700__ $$aYeletskikh, Ivan$$iINSPIRE-00375274$$uDubna, JINR
002255384 700__ $$aYildirim, Eda$$iINSPIRE-00194534$$uMainz U.
002255384 700__ $$aYorita, Kohei$$iINSPIRE-00048979$$uWaseda U.
002255384 700__ $$aYoshihara, Keisuke$$iINSPIRE-00288002$$uPennsylvania U.
002255384 700__ $$aYoung, Charles$$iINSPIRE-00137680$$uSLAC
002255384 700__ $$aYoung, Christopher John$$iINSPIRE-00237930$$uCERN
002255384 700__ $$aYoussef, Saul$$iINSPIRE-00137710$$uBoston U.
002255384 700__ $$aYu, David Ren-Hwa$$iINSPIRE-00329256$$uLBL, Berkeley
002255384 700__ $$aYu, Jaehoon$$iINSPIRE-00137749$$uTexas U., Arlington
002255384 700__ $$aYu, Jie$$iINSPIRE-00226216$$uIowa State U.
002255384 700__ $$aYuan, Li$$iINSPIRE-00226222$$uKobe U.
002255384 700__ $$aYuen, Stephanie P$$iINSPIRE-00418328$$uBonn U.
002255384 700__ $$aYusuff, Imran$$iINSPIRE-00367518$$uCambridge U.$$uMalaya U.
002255384 700__ $$aZabinski, Bartlomiej$$iINSPIRE-00237959$$uCracow, INP
002255384 700__ $$aZacharis, Georgios$$iINSPIRE-00529860$$uNatl. Tech. U., Athens
002255384 700__ $$aZaidan, Remi$$iINSPIRE-00226234$$uBarcelona, IFAE
002255384 700__ $$aZaitsev, Alexander$$iINSPIRE-00170475$$uSerpukhov, IHEP$$uMoscow, MIPT
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002255384 700__ $$aZeng, Qi$$iINSPIRE-00387563$$uSLAC
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002255384 700__ $$aZhang, Ruiqi$$iINSPIRE-00381776$$uHefei, CUST$$uMarseille, CPPM
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002255384 700__ $$aZhao, Yongke$$iINSPIRE-00382184$$uShandong U.$$uOrsay, LAL
002255384 700__ $$aZhao, Zhengguo$$iINSPIRE-00226382$$uHefei, CUST
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002255384 700__ $$aZhou, Chen$$iINSPIRE-00264959$$uWisconsin U., Madison
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002255384 700__ $$aZhou, Mingliang$$iINSPIRE-00414784$$uSUNY, Stony Brook
002255384 700__ $$aZhou, Ning$$iINSPIRE-00301363$$uTsinghua U., Beijing
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002255384 700__ $$aZhu, Yingchun$$iINSPIRE-00218063$$uHefei, CUST
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002255384 700__ $$aZieminska, Daria$$iINSPIRE-00138550$$uIndiana U.
002255384 700__ $$aZimine, Nikolai$$iINSPIRE-00342797$$uDubna, JINR
002255384 700__ $$aZimmermann, Christoph$$iINSPIRE-00339183$$uMainz U.
002255384 700__ $$aZimmermann, Stephanie$$iINSPIRE-00226472$$uFreiburg U.
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002255384 700__ $$aZiolkowski, Michael$$iINSPIRE-00154081$$uSiegen U.
002255384 700__ $$aŽivković, Lidija$$iINSPIRE-00057284$$uBelgrade U.
002255384 700__ $$aZobernig, Georg$$iINSPIRE-00226497$$uWisconsin U., Madison
002255384 700__ $$aZoccoli, Antonio$$iINSPIRE-00138667$$uINFN, Bologna$$uBologna U.
002255384 700__ $$aZou, Rui$$iINSPIRE-00535690$$uChicago U., EFI
002255384 700__ $$azur Nedden, Martin$$iINSPIRE-00226500$$uHumboldt U., Berlin
002255384 700__ $$aZwalinski, Lukasz$$iINSPIRE-00233300$$uCERN
002255384 710__ $$gATLAS Collaboration
002255384 710__ $$5PH-EP
002255384 773__ $$c474$$n7$$pEur. Phys. J. C$$v77$$y2017
002255384 859__ [email protected]
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tables and other information$$yRivet analyses reference$$yFulltext$$y00136 Unfolded absolute differential \wjets production cross sections as a function of leading-jet $\pt$ for the forward-lepton control region (top left), forward-lepton/central-jet fiducial region (top right), the signal regions with $\mjj>0.5$~TeV (middle left) and 1.0~\TeV (middle right), and the central-jet validation region (bottom). The absolute (left) and normalized (right) distributions are shown in the central-jet region. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00057 Unfolded normalized differential QCD+EW \wjets production cross sections as a function of jet centrality for the inclusive fiducial region with $\mjj > 0.5$~\TeV~(left) and 1.0~\TeV~(right). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00115 Unfolded normalized differential \wjets production cross sections as a function of jet centrality (top) and lepton centrality (bottom) for the inclusive fiducial region with $\mjj > 1.5$~\TeV~(left) and 2.0~\TeV~(right). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00163 Differential \wjets production cross sections as a function of $\Delta\phi(j_1,j_2)$ in the signal, high-mass signal, forward-lepton/central-jet, forward-lepton, and central-jet fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00004 Examples of leading-order diagrams for strong $Wjj$ production at the LHC. The left-hand diagram interferes with the electroweak diagrams of Figure~\ref{intro:Fig:EWK2Jets} when the final-state quarks have the same colours as the initial-state quarks.$$y00082 The observed (solid blue) and expected (open dashed) 95\% C.L. allowed regions in two-parameter planes for $\Lambda = 4$~\TeV. The regions are derived using a single measured yield and therefore reduce to the corresponding one-parameter interval when the other parameter is set to zero. Constraints on $\tilde{\lambda}_V$ are similar to those on $\lambda_V$.$$y00167 Differential \wjets production cross sections as a function of $\Delta\phi(j_1,j_2)$ in the inclusive fiducial region with four thresholds on the dijet invariant mass (0.5~\TeV, 1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00161 Unfolded normalized differential \wjets production cross sections as a function of $\Delta\phi(j_1,j_2)$ in the signal, high-mass signal, forward-lepton/central-jet, forward-lepton, and central-jet fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00042 Unfolded normalized differential \wjets production cross sections as a function of $\dyjj$ in the inclusive, forward-lepton/central-jet, forward-lepton, and central-jet fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).Unfolded normalized differential \wjets production cross sections as a function of $\dyjj$ in the inclusive fiducial region with four thresholds on the dijet invariant mass (0.5~\TeV, 1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00045 Unfolded normalized differential \wjets production cross sections as a function of $\dyjj$ in the inclusive, forward-lepton/central-jet, forward-lepton, and central-jet fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00011 Predicted and observed distributions of the dijet invariant mass (top) and $\dyjj$ (bottom) for events in the signal region in 7~\TeV~(left) and 8~\TeV~(right) data. The bottom panel in each distribution shows the ratio of data to the prediction. The shaded band represents the statistical and experimental uncertainties summed in quadrature.$$y00159 Unfolded normalized differential \wjets production cross sections as a function of $\Delta\phi(j_1,j_2)$ in the inclusive fiducial region with four thresholds on the dijet invariant mass (0.5~\TeV, 1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00037 Top: Unfolded absolute (left) and normalized (right) differential \wjets production cross sections as a function of dijet mass for the signal fiducial region. Bottom: Unfolded normalized production cross sections as a function of $\dyjj$ for the signal regions with $\mjj > 0.5$~\TeV~(left) and $\mjj > 1.0$~\TeV~(right). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00002 Caption not extracted$$y00162 Differential \wjets production cross sections as a function of $\Delta\phi(j_1,j_2)$ in the signal, high-mass signal, forward-lepton/central-jet, forward-lepton, and central-jet fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00122 Unfolded differential \wjets production cross sections as a function of lepton centrality in the inclusive fiducial region with four thresholds on the dijet invariant mass (0.5~\TeV, 1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). The bottom plot shows the normalized distribution for $\mjj> 2.0$~\TeV. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00157 Unfolded normalized differential \wjets production cross sections as a function of $\Delta\phi(j_1,j_2)$ in the inclusive fiducial region with four thresholds on the dijet invariant mass (0.5~\TeV, 1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00023 Relative uncertainties in example unfolded differential cross sections for the combined QCD+EW~\wjets processes. The examples are: the number of jets in the rapidity gap between the two highest-$\pt$ jets in the inclusive region (top left); the lepton centrality distribution in the inclusive $\mjj>1$~TeV region (top right); $\mjj$ in the inclusive region (bottom left); and the dijet $\pt$ in the signal region (bottom right). Dominant contributions to the total systematic uncertainty are highlighted separately.$$y00110 Differential electroweak \wjets production cross sections as a function of the number of hard jets in the rapidity gap between the two leading jets in the inclusive fiducial region with $\mjj >1.0$~\TeV~(top left), 1.5~\TeV~(top right and bottom left), and 2.0~\TeV (bottom right). The region with $\mjj > 1.5$~\TeV, includes both absolute (top right) and normalized (bottom left) distributions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00149 Differential \wjets production cross sections as a function of dijet $\pt$ in the signal, high-mass signal, forward-lepton/central-jet, forward-lepton, and central-jet fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00160 Unfolded normalized differential \wjets production cross sections as a function of $\Delta\phi(j_1,j_2)$ in the signal, high-mass signal, forward-lepton/central-jet, forward-lepton, and central-jet fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00068 Unfolded normalized differential EW~\wjets production cross sections as a function of the leading-jet $\pt$ for the inclusive fiducial region with three thresholds on the dijet invariant mass (1.0~\TeV, 1.5~\TeV, and 2.0~\TeV), and for the signal-enriched fiducial region with a minimum dijet invariant mass of 1.0~\TeV. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00095 Differential \wjets production cross sections as a function of $\dyjj$ in the signal and high-mass signal fiducial regions, and in the forward-lepton, central-jet validation, and forward-lepton/central-jet fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00017 Comparison of the corrected QCD \wjets background dijet mass distribution to data with background processes subtracted, for events in the central-jet validation region in 7~\TeV~(left) and 8~\TeV~(right) data. The bottom panel in each subfigure shows the ratio of data to prediction, and the result of a linear fit to the ratio (solid line). The error bars represent statistical and experimental uncertainties summed in quadrature. The dotted lines show the fit with slope adjusted up and down by statistical and experimental uncertainties.$$y00114 Differential \wjets production cross sections as a function of jet centrality in the inclusive fiducial region with four thresholds on the dijet invariant mass (0.5~\TeV, 1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00170 Differential \wjets production cross sections as a function of $\Delta\phi(j_1,j_2)$ in the inclusive fiducial region with four thresholds on the dijet invariant mass (0.5~\TeV, 1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00164 Differential \wjets production cross sections as a function of $\Delta\phi(j_1,j_2)$ in the signal, high-mass signal, forward-lepton/central-jet, forward-lepton, and central-jet fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00144 Unfolded normalized differential \wjets production cross sections as a function of dijet $\pt$ in the inclusive (top), forward-lepton/central-jet (middle left), forward-lepton (middle right), central-jet (bottom left), and high-mass signal (bottom right) fiducial regions. The inclusive regions show the distributions for \mjj thresholds of 1.5~\TeV~(left) and 2.0~\TeV~(right). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00073 Unfolded normalized differential \wjets production cross sections as a function of dijet $\pt$ for the inclusive (top) and signal (bottom) regions with $\mjj>0.5$~\TeV~(left) and $\mjj > 1.0$~\TeV~(right). The bottom right distribution shows EW~\wjets production and the other distributions show QCD+EW~\wjets production. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00061 Unfolded normalized differential QCD+EW \wjets (top) and EW (bottom) production cross sections as a function of lepton centrality for the inclusive fiducial region with $\mjj > 0.5$~\TeV~(top left), 1.0~\TeV~(top right and bottom left), and 1.5~\TeV~(bottom right). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00060 Unfolded normalized differential QCD+EW \wjets (top) and EW (bottom) production cross sections as a function of lepton centrality for the inclusive fiducial region with $\mjj > 0.5$~\TeV~(top left), 1.0~\TeV~(top right and bottom left), and 1.5~\TeV~(bottom right). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00075 Unfolded normalized differential \wjets production cross sections as a function of $\Delta\phi(j_1,j_2)$ for the inclusive, forward-lepton control, central-jet validation, and signal fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).Unfolded normalized differential production cross sections as a function of $\Delta\phi(j_1,j_2)$ for the inclusive, forward-lepton control, central-jet validation, and signal fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).Unfolded normalized differential \wjets production cross sections as a function of $\Delta\phi(j_1,j_2)$ in the signal, high-mass signal, forward-lepton/central-jet, forward-lepton, and central-jet fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00003 Examples of leading-order diagrams for strong $Wjj$ production at the LHC. The left-hand diagram interferes with the electroweak diagrams of Figure~\ref{intro:Fig:EWK2Jets} when the final-state quarks have the same colours as the initial-state quarks.$$y00096 Differential \wjets production cross sections as a function of $\dyjj$ in the signal and high-mass signal fiducial regions, and in the forward-lepton, central-jet validation, and forward-lepton/central-jet fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00153 Differential \wjets production cross sections as a function of dijet $\pt$ in the inclusive fiducial region with four thresholds on the dijet invariant mass (0.5~\TeV, 1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00089 Unfolded normalized differential \wjets production cross sections as a function of $\dyjj$ in the inclusive fiducial region with four thresholds on the dijet invariant mass (0.5~\TeV, 1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00139 Differential electroweak \wjets production cross sections as a function of the leading-jet $\pt$ in the high-mass signal region and the inclusive fiducial region with three thresholds on the dijet invariant mass (1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00140 Differential electroweak \wjets production cross sections as a function of the leading-jet $\pt$ in the high-mass signal region and the inclusive fiducial region with three thresholds on the dijet invariant mass (1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00001 Non-resonantRepresentative leading-order diagrams for electroweak $Wjj$ production at the LHC. In addition to (a) the vector boson fusion process, there are four (b) $W$~bremsstrahlung diagrams, corresponding to $W^\pm$ boson radiation by any incoming or outgoing quark, and two (c) non-resonant diagrams, corresponding to $W^\pm$ boson radiation by either incoming quark.$$y00107 Differential electroweak \wjets production cross sections as a function of the number of hard jets in the rapidity gap between the two leading jets in the inclusive fiducial region with $\mjj >1.0$~\TeV~(top left), 1.5~\TeV~(top right and bottom left), and 2.0~\TeV (bottom right). The region with $\mjj > 1.5$~\TeV, includes both absolute (top right) and normalized (bottom left) distributions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00067 Unfolded normalized differential EW~\wjets production cross sections as a function of the leading-jet $\pt$ for the inclusive fiducial region with three thresholds on the dijet invariant mass (1.0~\TeV, 1.5~\TeV, and 2.0~\TeV), and for the signal-enriched fiducial region with a minimum dijet invariant mass of 1.0~\TeV. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00108 Differential electroweak \wjets production cross sections as a function of the number of hard jets in the rapidity gap between the two leading jets in the inclusive fiducial region with $\mjj >1.0$~\TeV~(top left), 1.5~\TeV~(top right and bottom left), and 2.0~\TeV (bottom right). The region with $\mjj > 1.5$~\TeV, includes both absolute (top right) and normalized (bottom left) distributions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00036 Top: Unfolded absolute (left) and normalized (right) differential \wjets production cross sections as a function of dijet mass for the signal fiducial region. Bottom: Unfolded normalized production cross sections as a function of $\dyjj$ for the signal regions with $\mjj > 0.5$~\TeV~(left) and $\mjj > 1.0$~\TeV~(right). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00101 Differential electroweak \wjets production cross sections as a function of $\dyjj$ in the high-mass signal region and the inclusive fiducial region with three thresholds on the dijet invariant mass (1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00031 Measurements of the cross sections times branching fractions of electroweak production of a single $W$, $Z$, or Higgs boson with two jets at high dijet invariant mass and in fiducial measurement regions. For each measurement the error bar represents the statistical and systematic uncertainties summed in quadrature. Shaded bands represent the theory predictions. The \mjj threshold defining the fiducial $Zjj$ region differs between ATLAS and CMS, leading to different inclusive cross sections.$$y00100 Differential electroweak \wjets production cross sections as a function of $\dyjj$ in the high-mass signal region and the inclusive fiducial region with three thresholds on the dijet invariant mass (1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00155 Differential \wjets production cross sections as a function of dijet $\pt$ in the inclusive fiducial region with four thresholds on the dijet invariant mass (0.5~\TeV, 1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00047 Unfolded normalized differential EW~\wjets production cross sections as a function of the dijet invariant mass (top) and $\dyjj$ (bottom) for the inclusive (left) and signal (right) fiducial regions with $\mjj > 1.0$~\TeV. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00166 Differential \wjets production cross sections as a function of $\Delta\phi(j_1,j_2)$ in the signal, high-mass signal, forward-lepton/central-jet, forward-lepton, and central-jet fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00065 Unfolded normalized differential \wjets production cross sections as a function of the leading-jet \pt in the signal, high-mass signal, forward-lepton/central-jet, and forward-lepton fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00034 Top: Unfolded absolute (left) and normalized (right) differential \wjets production cross sections as a function of dijet mass for the signal fiducial region. Bottom: Unfolded normalized production cross sections as a function of $\dyjj$ for the signal regions with $\mjj > 0.5$~\TeV~(left) and $\mjj > 1.0$~\TeV~(right). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00142 Unfolded normalized differential \wjets production cross sections as a function of dijet $\pt$ in the inclusive (top), forward-lepton/central-jet (middle left), forward-lepton (middle right), central-jet (bottom left), and high-mass signal (bottom right) fiducial regions. The inclusive regions show the distributions for \mjj thresholds of 1.5~\TeV~(left) and 2.0~\TeV~(right). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00044 Unfolded normalized differential \wjets production cross sections as a function of $\dyjj$ in the inclusive, forward-lepton/central-jet, forward-lepton, and central-jet fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00148 Differential \wjets production cross sections as a function of dijet $\pt$ in the signal, high-mass signal, forward-lepton/central-jet, forward-lepton, and central-jet fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00077 Unfolded normalized differential \wjets production cross sections as a function of $\Delta\phi(j_1,j_2)$ for the inclusive, forward-lepton control, central-jet validation, and signal fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).Unfolded normalized differential production cross sections as a function of $\Delta\phi(j_1,j_2)$ for the inclusive, forward-lepton control, central-jet validation, and signal fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).Unfolded normalized differential \wjets production cross sections as a function of $\Delta\phi(j_1,j_2)$ in the signal, high-mass signal, forward-lepton/central-jet, forward-lepton, and central-jet fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00026 Relative uncertainties in example unfolded differential cross sections for the EW \wjets processes. The examples are $\mjj$ (top left) and $\dyjj$ (top right) in the high-mass signal region; $\mjj$ in the $\mjj>1$~TeV inclusive region (bottom left); and leading-jet $\pt$ in the high-mass signal region (bottom right). Dominant contributions to the total systematic uncertainty are highlighted separately.$$y00032 Fraction of EW~\wjets signal relative to the combined QCD+EW~\wjets production, predicted by \powheg + \pythia and \sherpa simulations for observables in the signal (left) and inclusive (right) fiducial regions.$$y00105 Differential \wjets production cross sections as a function of the number of hard jets in the rapidity interval between the two leading jets in the inclusive fiducial region with four thresholds on the dijet invariant mass (0.5~\TeV, 1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00130 Unfolded normalized differential \wjets production cross sections as a function of the leading-jet \pt in the inclusive fiducial region with four thresholds on the dijet invariant mass (0.5~\TeV, 1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00079 Unfolded normalized differential EW~\wjets production cross sections as a function of the azimuthal angle between the two leading jets, for the inclusive and signal fiducial regions with $\mjj > 1.0$~\TeV. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00104 Differential \wjets production cross sections as a function of the number of hard jets in the rapidity interval between the two leading jets in the inclusive fiducial region with four thresholds on the dijet invariant mass (0.5~\TeV, 1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00152 Differential \wjets production cross sections as a function of dijet $\pt$ in the signal, high-mass signal, forward-lepton/central-jet, forward-lepton, and central-jet fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00103 Differential \wjets production cross sections as a function of the number of hard jets in the rapidity interval between the two leading jets in the inclusive fiducial region with four thresholds on the dijet invariant mass (0.5~\TeV, 1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00118 Unfolded normalized differential \wjets production cross sections as a function of jet centrality (top) and lepton centrality (bottom) for the inclusive fiducial region with $\mjj > 1.5$~\TeV~(left) and 2.0~\TeV~(right). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00009 Predicted and observed distributions of the lepton centrality (top) and the minimum centrality of additional jets (bottom) for events in the inclusive fiducial region (i.e. after preselection) in 7~\TeV~(left) and 8~\TeV~(right) data. The arrows in the lepton-centrality distributions separate the signal-region selection (to the left) from the control-region selection (to the right). The arrows in the jet-centrality distributions separate the signal-region selection (to the right) from the validation-region selection (to the left). The bottom panel in each distribution shows the ratio of data to the prediction. The shaded band represents the statistical and experimental uncertainties summed in quadrature.$$y00086 Unfolded differential \wjets production cross sections as a function of dijet mass for the inclusive (top left), forward-lepton (top right), central-jet (bottom left), and forward-lepton/central-jet (bottom right) fiducial regions, which are enriched in strong \wjets production. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00074 Unfolded normalized differential \wjets production cross sections as a function of $\Delta\phi(j_1,j_2)$ for the inclusive, forward-lepton control, central-jet validation, and signal fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).Unfolded normalized differential production cross sections as a function of $\Delta\phi(j_1,j_2)$ for the inclusive, forward-lepton control, central-jet validation, and signal fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).Unfolded normalized differential \wjets production cross sections as a function of $\Delta\phi(j_1,j_2)$ in the inclusive fiducial region with four thresholds on the dijet invariant mass (0.5~\TeV, 1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00143 Unfolded normalized differential \wjets production cross sections as a function of dijet $\pt$ in the inclusive (top), forward-lepton/central-jet (middle left), forward-lepton (middle right), central-jet (bottom left), and high-mass signal (bottom right) fiducial regions. The inclusive regions show the distributions for \mjj thresholds of 1.5~\TeV~(left) and 2.0~\TeV~(right). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00158 Unfolded normalized differential \wjets production cross sections as a function of $\Delta\phi(j_1,j_2)$ in the inclusive fiducial region with four thresholds on the dijet invariant mass (0.5~\TeV, 1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00054 Unfolded normalized differential EW~\wjets production cross sections as a function of the number of jets with $\pt>30$~\GeV~in the rapidity interval bounded by the two highest-$\pt$ jets in the inclusive fiducial region, with $\mjj> 1.0$~\TeV~(left) and $\mjj > 2.0$~\TeV~(right). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00099 Differential electroweak \wjets production cross sections as a function of $\dyjj$ in the high-mass signal region and the inclusive fiducial region with three thresholds on the dijet invariant mass (1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00109 Differential electroweak \wjets production cross sections as a function of the number of hard jets in the rapidity gap between the two leading jets in the inclusive fiducial region with $\mjj >1.0$~\TeV~(top left), 1.5~\TeV~(top right and bottom left), and 2.0~\TeV (bottom right). The region with $\mjj > 1.5$~\TeV, includes both absolute (top right) and normalized (bottom left) distributions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00094 Differential \wjets production cross sections as a function of $\dyjj$ in the signal and high-mass signal fiducial regions, and in the forward-lepton, central-jet validation, and forward-lepton/central-jet fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00056 Unfolded normalized differential QCD+EW \wjets production cross sections as a function of jet centrality for the inclusive fiducial region with $\mjj > 0.5$~\TeV~(left) and 1.0~\TeV~(right). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00040 Unfolded normalized differential \wjets production cross sections as a function of dijet invariant mass in the inclusive, forward-lepton/central-jet, forward-lepton, and central-jet fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00028 Relative uncertainties in example unfolded differential cross sections for the EW \wjets processes. The examples are $\mjj$ (top left) and $\dyjj$ (top right) in the high-mass signal region; $\mjj$ in the $\mjj>1$~TeV inclusive region (bottom left); and leading-jet $\pt$ in the high-mass signal region (bottom right). Dominant contributions to the total systematic uncertainty are highlighted separately.$$y00169 Differential \wjets production cross sections as a function of $\Delta\phi(j_1,j_2)$ in the inclusive fiducial region with four thresholds on the dijet invariant mass (0.5~\TeV, 1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00050 Unfolded normalized distribution of the number of jets with $\pt>30$~\GeV~in the rapidity interval bounded by the two highest-$\pt$ jets in the inclusive fiducial region with $\mjj$ thresholds of 0.5~\TeV~(top left),~1.0~\TeV~(top right),~1.5~\TeV~(bottom left), and 2.0~\TeV~(bottom right). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00097 Differential \wjets production cross sections as a function of $\dyjj$ in the signal and high-mass signal fiducial regions, and in the forward-lepton, central-jet validation, and forward-lepton/central-jet fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00135 Unfolded absolute differential \wjets production cross sections as a function of leading-jet $\pt$ for the forward-lepton control region (top left), forward-lepton/central-jet fiducial region (top right), the signal regions with $\mjj>0.5$~TeV (middle left) and 1.0~\TeV (middle right), and the central-jet validation region (bottom). The absolute (left) and normalized (right) distributions are shown in the central-jet region. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00063 Unfolded normalized differential \wjets production cross sections as a function of the leading-jet \pt in the signal, high-mass signal, forward-lepton/central-jet, and forward-lepton fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00022 Relative uncertainties in example unfolded differential cross sections for the combined QCD+EW~\wjets processes. The examples are: the number of jets in the rapidity gap between the two highest-$\pt$ jets in the inclusive region (top left); the lepton centrality distribution in the inclusive $\mjj>1$~TeV region (top right); $\mjj$ in the inclusive region (bottom left); and the dijet $\pt$ in the signal region (bottom right). Dominant contributions to the total systematic uncertainty are highlighted separately.$$y00134 Unfolded absolute differential \wjets production cross sections as a function of leading-jet $\pt$ for the forward-lepton control region (top left), forward-lepton/central-jet fiducial region (top right), the signal regions with $\mjj>0.5$~TeV (middle left) and 1.0~\TeV (middle right), and the central-jet validation region (bottom). The absolute (left) and normalized (right) distributions are shown in the central-jet region. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00117 Unfolded normalized differential \wjets production cross sections as a function of jet centrality (top) and lepton centrality (bottom) for the inclusive fiducial region with $\mjj > 1.5$~\TeV~(left) and 2.0~\TeV~(right). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00059 Unfolded normalized differential QCD+EW \wjets (top) and EW (bottom) production cross sections as a function of lepton centrality for the inclusive fiducial region with $\mjj > 0.5$~\TeV~(top left), 1.0~\TeV~(top right and bottom left), and 1.5~\TeV~(bottom right). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00035 Top: Unfolded absolute (left) and normalized (right) differential \wjets production cross sections as a function of dijet mass for the signal fiducial region. Bottom: Unfolded normalized production cross sections as a function of $\dyjj$ for the signal regions with $\mjj > 0.5$~\TeV~(left) and $\mjj > 1.0$~\TeV~(right). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00173 Differential electroweak \wjets production cross sections as a function of $\Delta\phi(j_1,j_2)$ in the high-mass signal region and the inclusive fiducial region with three thresholds on the dijet invariant mass (1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). The bottom two distributions are normalized, the rest are absolute. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00012 Predicted and observed distributions of the dijet invariant mass (top) and $\dyjj$ (bottom) for events in the signal region in 7~\TeV~(left) and 8~\TeV~(right) data. The bottom panel in each distribution shows the ratio of data to the prediction. The shaded band represents the statistical and experimental uncertainties summed in quadrature.$$y00126 Unfolded absolute differential \wjets production cross sections as a function of leading-jet $\pt$ for the inclusive fiducial region when the dijet invariant mass threshold is progressively raised in 500~\GeV~increments from 0.5~\TeV~(top left) to 2.0~\TeV~(bottom right). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00172 Differential electroweak \wjets production cross sections as a function of $\Delta\phi(j_1,j_2)$ in the high-mass signal region and the inclusive fiducial region with three thresholds on the dijet invariant mass (1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). The bottom two distributions are normalized, the rest are absolute. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00018 Comparison of the corrected QCD \wjets background dijet mass distribution to data with background processes subtracted, for events in the central-jet validation region in 7~\TeV~(left) and 8~\TeV~(right) data. The bottom panel in each subfigure shows the ratio of data to prediction, and the result of a linear fit to the ratio (solid line). The error bars represent statistical and experimental uncertainties summed in quadrature. The dotted lines show the fit with slope adjusted up and down by statistical and experimental uncertainties.$$y00064 Unfolded normalized differential \wjets production cross sections as a function of the leading-jet \pt in the signal, high-mass signal, forward-lepton/central-jet, and forward-lepton fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00058 Unfolded normalized differential QCD+EW \wjets (top) and EW (bottom) production cross sections as a function of lepton centrality for the inclusive fiducial region with $\mjj > 0.5$~\TeV~(top left), 1.0~\TeV~(top right and bottom left), and 1.5~\TeV~(bottom right). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00073 Unfolded normalized differential EW~\wjets production cross sections as a function of $\dyjj$ for the inclusive fiducial region with three thresholds on the dijet invariant mass, 1.0~\TeV~(top left), 1.5~\TeV~(bottom left), and 2.0~\TeV~(bottom right), and for the signal-enriched fiducial region with a minimum dijet invariant mass of 1.0~\TeV~(top right). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00008 Predicted and observed distributions of the lepton centrality (top) and the minimum centrality of additional jets (bottom) for events in the inclusive fiducial region (i.e. after preselection) in 7~\TeV~(left) and 8~\TeV~(right) data. The arrows in the lepton-centrality distributions separate the signal-region selection (to the left) from the control-region selection (to the right). The arrows in the jet-centrality distributions separate the signal-region selection (to the right) from the validation-region selection (to the left). The bottom panel in each distribution shows the ratio of data to the prediction. The shaded band represents the statistical and experimental uncertainties summed in quadrature.$$y00019 Distributions of the dijet invariant mass for events in the signal region in 7~\TeV~(left) and 8~\TeV~(right) data, after fitting for the yields of the individual \wjets processes. The bottom panel in each distribution shows the ratio of data to predicted signal-plus-background yields. The shaded band centred at unity represents the statistical and experimental uncertainties summed in quadrature.$$y00146 Unfolded normalized differential \wjets production cross sections as a function of dijet $\pt$ in the inclusive (top), forward-lepton/central-jet (middle left), forward-lepton (middle right), central-jet (bottom left), and high-mass signal (bottom right) fiducial regions. The inclusive regions show the distributions for \mjj thresholds of 1.5~\TeV~(left) and 2.0~\TeV~(right). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00006 Illustration of the relationship between the signal, control, and validation fiducial regions. The signal region is defined by both a veto on additional jets (beyond the two highest-$\pt$ jets) and the presence of a lepton in the rapidity region defined in Eq.~(\ref{evtsel:rapinterval}). The signal region is studied with either $\mjj>0.5$~\TeV~or $1$~\TeV. A forward-lepton/central-jet fiducial region is also defined, for which the centrality requirements on the jets and the lepton are inverted with respect to the signal region. The inclusive region corresponds to the union of all four regions, and is studied with $\mjj>0.5,~1.0,~1.5,$ or 2.0~TeV. The quantities $\ncenjet$ and $\ncenlep$ refer to the number of reconstructed leptons and additional jets reconstructed in the rapidity interval defined by Eq.~(\ref{evtsel:rapinterval}) and illustrated in Figure~\ref{evtsel:vetoIllustration}, with $C_{\textrm{max}} = 0.4$.$$y00043 Unfolded normalized differential \wjets production cross sections as a function of $\dyjj$ in the inclusive, forward-lepton/central-jet, forward-lepton, and central-jet fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00024 Relative uncertainties in example unfolded differential cross sections for the combined QCD+EW~\wjets processes. The examples are: the number of jets in the rapidity gap between the two highest-$\pt$ jets in the inclusive region (top left); the lepton centrality distribution in the inclusive $\mjj>1$~TeV region (top right); $\mjj$ in the inclusive region (bottom left); and the dijet $\pt$ in the signal region (bottom right). Dominant contributions to the total systematic uncertainty are highlighted separately.$$y00055 Unfolded normalized differential EW~\wjets production cross sections as a function of the number of jets with $\pt>30$~\GeV~in the rapidity interval bounded by the two highest-$\pt$ jets in the inclusive fiducial region, with $\mjj> 1.0$~\TeV~(left) and $\mjj > 2.0$~\TeV~(right). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00027 Relative uncertainties in example unfolded differential cross sections for the EW \wjets processes. The examples are $\mjj$ (top left) and $\dyjj$ (top right) in the high-mass signal region; $\mjj$ in the $\mjj>1$~TeV inclusive region (bottom left); and leading-jet $\pt$ in the high-mass signal region (bottom right). Dominant contributions to the total systematic uncertainty are highlighted separately.$$y00150 Differential \wjets production cross sections as a function of dijet $\pt$ in the signal, high-mass signal, forward-lepton/central-jet, forward-lepton, and central-jet fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00090 Unfolded absolute differential \wjets production cross sections as a function of $\dyjj$ for the inclusive fiducial region with progressively increasing dijet mass thresholds. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00151 Differential \wjets production cross sections as a function of dijet $\pt$ in the signal, high-mass signal, forward-lepton/central-jet, forward-lepton, and central-jet fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00083 Unfolded differential \wjets production cross sections as a function of dijet mass for the inclusive (top left), forward-lepton (top right), central-jet (bottom left), and forward-lepton/central-jet (bottom right) fiducial regions, which are enriched in strong \wjets production. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00020 Distributions of the dijet invariant mass for events in the signal region in 7~\TeV~(left) and 8~\TeV~(right) data, after fitting for the yields of the individual \wjets processes. The bottom panel in each distribution shows the ratio of data to predicted signal-plus-background yields. The shaded band centred at unity represents the statistical and experimental uncertainties summed in quadrature.$$y00171 Differential electroweak \wjets production cross sections as a function of $\Delta\phi(j_1,j_2)$ in the high-mass signal region and the inclusive fiducial region with three thresholds on the dijet invariant mass (1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). The bottom two distributions are normalized, the rest are absolute. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00087 Unfolded normalized differential \wjets production cross sections as a function of $\dyjj$ in the inclusive fiducial region with four thresholds on the dijet invariant mass (0.5~\TeV, 1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00102 Differential electroweak \wjets production cross sections as a function of $\dyjj$ in the high-mass signal region and the inclusive fiducial region with three thresholds on the dijet invariant mass (1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00088 Unfolded normalized differential \wjets production cross sections as a function of $\dyjj$ in the inclusive fiducial region with four thresholds on the dijet invariant mass (0.5~\TeV, 1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00176 Differential electroweak \wjets production cross sections as a function of $\Delta\phi(j_1,j_2)$ in the high-mass signal region and the inclusive fiducial region with three thresholds on the dijet invariant mass (1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). The bottom two distributions are normalized, the rest are absolute. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00085 Unfolded differential \wjets production cross sections as a function of dijet mass for the inclusive (top left), forward-lepton (top right), central-jet (bottom left), and forward-lepton/central-jet (bottom right) fiducial regions, which are enriched in strong \wjets production. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00091 Unfolded absolute differential \wjets production cross sections as a function of $\dyjj$ for the inclusive fiducial region with progressively increasing dijet mass thresholds. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00092 Unfolded absolute differential \wjets production cross sections as a function of $\dyjj$ for the inclusive fiducial region with progressively increasing dijet mass thresholds. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00080 The observed (solid blue) and expected (open dashed) 95\% C.L. allowed regions in two-parameter planes for $\Lambda = 4$~\TeV. The regions are derived using a single measured yield and therefore reduce to the corresponding one-parameter interval when the other parameter is set to zero. Constraints on $\tilde{\lambda}_V$ are similar to those on $\lambda_V$.$$y00062 Unfolded normalized differential \wjets production cross sections as a function of the leading-jet \pt in the signal, high-mass signal, forward-lepton/central-jet, and forward-lepton fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00041 Unfolded normalized differential \wjets production cross sections as a function of dijet invariant mass in the inclusive, forward-lepton/central-jet, forward-lepton, and central-jet fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00010 Predicted and observed distributions of the lepton centrality (top) and the minimum centrality of additional jets (bottom) for events in the inclusive fiducial region (i.e. after preselection) in 7~\TeV~(left) and 8~\TeV~(right) data. The arrows in the lepton-centrality distributions separate the signal-region selection (to the left) from the control-region selection (to the right). The arrows in the jet-centrality distributions separate the signal-region selection (to the right) from the validation-region selection (to the left). The bottom panel in each distribution shows the ratio of data to the prediction. The shaded band represents the statistical and experimental uncertainties summed in quadrature.$$y00123 Unfolded differential \wjets production cross sections as a function of lepton centrality in the inclusive fiducial region with four thresholds on the dijet invariant mass (0.5~\TeV, 1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). The bottom plot shows the normalized distribution for $\mjj> 2.0$~\TeV. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00147 Unfolded normalized differential \wjets production cross sections as a function of dijet $\pt$ in the inclusive (top), forward-lepton/central-jet (middle left), forward-lepton (middle right), central-jet (bottom left), and high-mass signal (bottom right) fiducial regions. The inclusive regions show the distributions for \mjj thresholds of 1.5~\TeV~(left) and 2.0~\TeV~(right). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00033 Fraction of EW~\wjets signal relative to the combined QCD+EW~\wjets production, predicted by \powheg + \pythia and \sherpa simulations for observables in the signal (left) and inclusive (right) fiducial regions.$$y00098 Differential \wjets production cross sections as a function of $\dyjj$ in the signal and high-mass signal fiducial regions, and in the forward-lepton, central-jet validation, and forward-lepton/central-jet fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00131 Unfolded normalized differential \wjets production cross sections as a function of the leading-jet \pt in the inclusive fiducial region with four thresholds on the dijet invariant mass (0.5~\TeV, 1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00124 Unfolded absolute differential \wjets production cross sections as a function of leading-jet $\pt$ for the inclusive fiducial region when the dijet invariant mass threshold is progressively raised in 500~\GeV~increments from 0.5~\TeV~(top left) to 2.0~\TeV~(bottom right). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00145 Unfolded normalized differential \wjets production cross sections as a function of dijet $\pt$ in the inclusive (top), forward-lepton/central-jet (middle left), forward-lepton (middle right), central-jet (bottom left), and high-mass signal (bottom right) fiducial regions. The inclusive regions show the distributions for \mjj thresholds of 1.5~\TeV~(left) and 2.0~\TeV~(right). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00120 Unfolded differential \wjets production cross sections as a function of lepton centrality in the inclusive fiducial region with four thresholds on the dijet invariant mass (0.5~\TeV, 1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). The bottom plot shows the normalized distribution for $\mjj> 2.0$~\TeV. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00133 Unfolded absolute differential \wjets production cross sections as a function of leading-jet $\pt$ for the forward-lepton control region (top left), forward-lepton/central-jet fiducial region (top right), the signal regions with $\mjj>0.5$~TeV (middle left) and 1.0~\TeV (middle right), and the central-jet validation region (bottom). The absolute (left) and normalized (right) distributions are shown in the central-jet region. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00121 Unfolded differential \wjets production cross sections as a function of lepton centrality in the inclusive fiducial region with four thresholds on the dijet invariant mass (0.5~\TeV, 1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). The bottom plot shows the normalized distribution for $\mjj> 2.0$~\TeV. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00007 Predicted and observed distributions of the lepton centrality (top) and the minimum centrality of additional jets (bottom) for events in the inclusive fiducial region (i.e. after preselection) in 7~\TeV~(left) and 8~\TeV~(right) data. The arrows in the lepton-centrality distributions separate the signal-region selection (to the left) from the control-region selection (to the right). The arrows in the jet-centrality distributions separate the signal-region selection (to the right) from the validation-region selection (to the left). The bottom panel in each distribution shows the ratio of data to the prediction. The shaded band represents the statistical and experimental uncertainties summed in quadrature.$$y00071 Unfolded normalized differential \wjets production cross sections as a function of dijet $\pt$ for the inclusive (top) and signal (bottom) regions with $\mjj>0.5$~\TeV~(left) and $\mjj > 1.0$~\TeV~(right). The bottom right distribution shows EW~\wjets production and the other distributions show QCD+EW~\wjets production. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00154 Differential \wjets production cross sections as a function of dijet $\pt$ in the inclusive fiducial region with four thresholds on the dijet invariant mass (0.5~\TeV, 1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00072 Unfolded normalized differential \wjets production cross sections as a function of dijet $\pt$ for the inclusive (top) and signal (bottom) regions with $\mjj>0.5$~\TeV~(left) and $\mjj > 1.0$~\TeV~(right). The bottom right distribution shows EW~\wjets production and the other distributions show QCD+EW~\wjets production. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00078 Unfolded normalized differential EW~\wjets production cross sections as a function of the azimuthal angle between the two leading jets, for the inclusive and signal fiducial regions with $\mjj > 1.0$~\TeV. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00093 Unfolded absolute differential \wjets production cross sections as a function of $\dyjj$ for the inclusive fiducial region with progressively increasing dijet mass thresholds. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00175 Differential electroweak \wjets production cross sections as a function of $\Delta\phi(j_1,j_2)$ in the high-mass signal region and the inclusive fiducial region with three thresholds on the dijet invariant mass (1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). The bottom two distributions are normalized, the rest are absolute. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00128 Unfolded normalized differential \wjets production cross sections as a function of the leading-jet \pt in the inclusive fiducial region with four thresholds on the dijet invariant mass (0.5~\TeV, 1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00069 Unfolded normalized differential EW~\wjets production cross sections as a function of the leading-jet $\pt$ for the inclusive fiducial region with three thresholds on the dijet invariant mass (1.0~\TeV, 1.5~\TeV, and 2.0~\TeV), and for the signal-enriched fiducial region with a minimum dijet invariant mass of 1.0~\TeV. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00038 Unfolded normalized differential \wjets production cross sections as a function of dijet invariant mass in the inclusive, forward-lepton/central-jet, forward-lepton, and central-jet fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00053 Unfolded normalized distribution of the number of jets with $\pt>30$~\GeV~in the rapidity interval bounded by the two highest-$\pt$ jets in the inclusive fiducial region with $\mjj$ thresholds of 0.5~\TeV~(top left),~1.0~\TeV~(top right),~1.5~\TeV~(bottom left), and 2.0~\TeV~(bottom right). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00138 Differential electroweak \wjets production cross sections as a function of the leading-jet $\pt$ in the high-mass signal region and the inclusive fiducial region with three thresholds on the dijet invariant mass (1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00039 Unfolded normalized differential \wjets production cross sections as a function of dijet invariant mass in the inclusive, forward-lepton/central-jet, forward-lepton, and central-jet fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00000 Vector boson fusion$W$~bremsstrahlung$$y00132 Unfolded absolute differential \wjets production cross sections as a function of leading-jet $\pt$ for the forward-lepton control region (top left), forward-lepton/central-jet fiducial region (top right), the signal regions with $\mjj>0.5$~TeV (middle left) and 1.0~\TeV (middle right), and the central-jet validation region (bottom). The absolute (left) and normalized (right) distributions are shown in the central-jet region. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00072 Unfolded normalized differential EW~\wjets production cross sections as a function of $\dyjj$ for the inclusive fiducial region with three thresholds on the dijet invariant mass, 1.0~\TeV~(top left), 1.5~\TeV~(bottom left), and 2.0~\TeV~(bottom right), and for the signal-enriched fiducial region with a minimum dijet invariant mass of 1.0~\TeV~(top right). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00119 Unfolded differential \wjets production cross sections as a function of lepton centrality in the inclusive fiducial region with four thresholds on the dijet invariant mass (0.5~\TeV, 1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). The bottom plot shows the normalized distribution for $\mjj> 2.0$~\TeV. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00048 Unfolded normalized differential EW~\wjets production cross sections as a function of the dijet invariant mass (top) and $\dyjj$ (bottom) for the inclusive (left) and signal (right) fiducial regions with $\mjj > 1.0$~\TeV. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00125 Unfolded absolute differential \wjets production cross sections as a function of leading-jet $\pt$ for the inclusive fiducial region when the dijet invariant mass threshold is progressively raised in 500~\GeV~increments from 0.5~\TeV~(top left) to 2.0~\TeV~(bottom right). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00052 Unfolded normalized distribution of the number of jets with $\pt>30$~\GeV~in the rapidity interval bounded by the two highest-$\pt$ jets in the inclusive fiducial region with $\mjj$ thresholds of 0.5~\TeV~(top left),~1.0~\TeV~(top right),~1.5~\TeV~(bottom left), and 2.0~\TeV~(bottom right). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00049 Unfolded normalized differential EW~\wjets production cross sections as a function of the dijet invariant mass (top) and $\dyjj$ (bottom) for the inclusive (left) and signal (right) fiducial regions with $\mjj > 1.0$~\TeV. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00084 Unfolded differential \wjets production cross sections as a function of dijet mass for the inclusive (top left), forward-lepton (top right), central-jet (bottom left), and forward-lepton/central-jet (bottom right) fiducial regions, which are enriched in strong \wjets production. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00113 Differential \wjets production cross sections as a function of jet centrality in the inclusive fiducial region with four thresholds on the dijet invariant mass (0.5~\TeV, 1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00066 Unfolded normalized differential EW~\wjets production cross sections as a function of the leading-jet $\pt$ for the inclusive fiducial region with three thresholds on the dijet invariant mass (1.0~\TeV, 1.5~\TeV, and 2.0~\TeV), and for the signal-enriched fiducial region with a minimum dijet invariant mass of 1.0~\TeV. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00112 Differential \wjets production cross sections as a function of jet centrality in the inclusive fiducial region with four thresholds on the dijet invariant mass (0.5~\TeV, 1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00174 Differential electroweak \wjets production cross sections as a function of $\Delta\phi(j_1,j_2)$ in the high-mass signal region and the inclusive fiducial region with three thresholds on the dijet invariant mass (1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). The bottom two distributions are normalized, the rest are absolute. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00156 Differential \wjets production cross sections as a function of dijet $\pt$ in the inclusive fiducial region with four thresholds on the dijet invariant mass (0.5~\TeV, 1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00081 The observed (solid blue) and expected (open dashed) 95\% C.L. allowed regions in two-parameter planes for $\Lambda = 4$~\TeV. The regions are derived using a single measured yield and therefore reduce to the corresponding one-parameter interval when the other parameter is set to zero. Constraints on $\tilde{\lambda}_V$ are similar to those on $\lambda_V$.$$y00030 Integrated production cross sections QCD+EW \wjets (solid data points) and EW \wjets (open data points) production in each measured particle-level fiducial region in a single lepton channel; EW \wjets production is only measured in fiducial regions where there is sufficient purity. For each measurement the error bar represents the statistical and systematic uncertainties summed in quadrature. Comparisons are made to predictions from \powheg + \pythia and the bottom pane shows the ratio of data to these predictions.$$y00127 Unfolded absolute differential \wjets production cross sections as a function of leading-jet $\pt$ for the inclusive fiducial region when the dijet invariant mass threshold is progressively raised in 500~\GeV~increments from 0.5~\TeV~(top left) to 2.0~\TeV~(bottom right). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00046 Unfolded normalized differential EW~\wjets production cross sections as a function of the dijet invariant mass (top) and $\dyjj$ (bottom) for the inclusive (left) and signal (right) fiducial regions with $\mjj > 1.0$~\TeV. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00015 Comparison of the predicted QCD \wjets dijet mass distribution to data with background processes subtracted, for events in the forward-lepton control region in 7~\TeV~(left) and 8~\TeV~(right) data. The bottom panel in each distribution shows the ratio of data to the QCD~\wjets prediction, and the result of a linear fit to the ratio. The error bars represent statistical and experimental uncertainties summed in quadrature.$$y00021 Measurements of the cross section times branching fractions of electroweak production of a single $W$, $Z$, or Higgs boson at high dijet invariant mass, divided by the SM predictions (\powheg+\pythia for ATLAS, \madgraph+\pythia for CMS, and \powheg+\pythia for the LHC combination). The lighter shaded band (where shown) represents the statistical uncertainty of the measurement, the outer darker band represents the total measurement uncertainty. Theoretical uncertainties in the SM prediction are represented by the shaded region centred at unity.$$y00168 Differential \wjets production cross sections as a function of $\Delta\phi(j_1,j_2)$ in the inclusive fiducial region with four thresholds on the dijet invariant mass (0.5~\TeV, 1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00025 Relative uncertainties in example unfolded differential cross sections for the combined QCD+EW~\wjets processes. The examples are: the number of jets in the rapidity gap between the two highest-$\pt$ jets in the inclusive region (top left); the lepton centrality distribution in the inclusive $\mjj>1$~TeV region (top right); $\mjj$ in the inclusive region (bottom left); and the dijet $\pt$ in the signal region (bottom right). Dominant contributions to the total systematic uncertainty are highlighted separately.$$y00111 Differential \wjets production cross sections as a function of jet centrality in the inclusive fiducial region with four thresholds on the dijet invariant mass (0.5~\TeV, 1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00014 Predicted and observed distributions of the dijet invariant mass (top) and $\dyjj$ (bottom) for events in the signal region in 7~\TeV~(left) and 8~\TeV~(right) data. The bottom panel in each distribution shows the ratio of data to the prediction. The shaded band represents the statistical and experimental uncertainties summed in quadrature.$$y00137 Unfolded absolute differential \wjets production cross sections as a function of leading-jet $\pt$ for the forward-lepton control region (top left), forward-lepton/central-jet fiducial region (top right), the signal regions with $\mjj>0.5$~TeV (middle left) and 1.0~\TeV (middle right), and the central-jet validation region (bottom). The absolute (left) and normalized (right) distributions are shown in the central-jet region. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00116 Unfolded normalized differential \wjets production cross sections as a function of jet centrality (top) and lepton centrality (bottom) for the inclusive fiducial region with $\mjj > 1.5$~\TeV~(left) and 2.0~\TeV~(right). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00016 Comparison of the predicted QCD \wjets dijet mass distribution to data with background processes subtracted, for events in the forward-lepton control region in 7~\TeV~(left) and 8~\TeV~(right) data. The bottom panel in each distribution shows the ratio of data to the QCD~\wjets prediction, and the result of a linear fit to the ratio. The error bars represent statistical and experimental uncertainties summed in quadrature.$$y00141 Differential electroweak \wjets production cross sections as a function of the leading-jet $\pt$ in the high-mass signal region and the inclusive fiducial region with three thresholds on the dijet invariant mass (1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00076 Unfolded normalized differential \wjets production cross sections as a function of $\Delta\phi(j_1,j_2)$ for the inclusive, forward-lepton control, central-jet validation, and signal fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).Unfolded normalized differential production cross sections as a function of $\Delta\phi(j_1,j_2)$ for the inclusive, forward-lepton control, central-jet validation, and signal fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).Unfolded normalized differential \wjets production cross sections as a function of $\Delta\phi(j_1,j_2)$ in the signal, high-mass signal, forward-lepton/central-jet, forward-lepton, and central-jet fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00051 Unfolded normalized distribution of the number of jets with $\pt>30$~\GeV~in the rapidity interval bounded by the two highest-$\pt$ jets in the inclusive fiducial region with $\mjj$ thresholds of 0.5~\TeV~(top left),~1.0~\TeV~(top right),~1.5~\TeV~(bottom left), and 2.0~\TeV~(bottom right). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00070 Unfolded normalized differential \wjets production cross sections as a function of dijet $\pt$ for the inclusive (top) and signal (bottom) regions with $\mjj>0.5$~\TeV~(left) and $\mjj > 1.0$~\TeV~(right). The bottom right distribution shows EW~\wjets production and the other distributions show QCD+EW~\wjets production. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00129 Unfolded normalized differential \wjets production cross sections as a function of the leading-jet \pt in the inclusive fiducial region with four thresholds on the dijet invariant mass (0.5~\TeV, 1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00106 Differential \wjets production cross sections as a function of the number of hard jets in the rapidity interval between the two leading jets in the inclusive fiducial region with four thresholds on the dijet invariant mass (0.5~\TeV, 1.0~\TeV, 1.5~\TeV, and 2.0~\TeV). Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00029 Relative uncertainties in example unfolded differential cross sections for the EW \wjets processes. The examples are $\mjj$ (top left) and $\dyjj$ (top right) in the high-mass signal region; $\mjj$ in the $\mjj>1$~TeV inclusive region (bottom left); and leading-jet $\pt$ in the high-mass signal region (bottom right). Dominant contributions to the total systematic uncertainty are highlighted separately.$$y00005 Illustration of the central region used to count leptons and jets in the definition of the signal, control, and validation regions. The rapidity range of the region corresponds to $C_{\textrm{max}}=0.4$ in Eq.~(\ref{evtsel:rapinterval}). An object in the direction of the dashed line has $C = 0$.$$y00165 Differential \wjets production cross sections as a function of $\Delta\phi(j_1,j_2)$ in the signal, high-mass signal, forward-lepton/central-jet, forward-lepton, and central-jet fiducial regions. Both statistical (inner bar) and total (outer bar) measurement uncertainties are shown, as well as ratios of the theoretical predictions to the data (the bottom panel in each distribution).$$y00013 Predicted and observed distributions of the dijet invariant mass (top) and $\dyjj$ (bottom) for events in the signal region in 7~\TeV~(left) and 8~\TeV~(right) data. The bottom panel in each distribution shows the ratio of data to the prediction. The shaded band represents the statistical and experimental uncertainties summed in quadrature.$$yArticle from SCOAP3$$yArticle from SCOAP3
002255384 916__ $$sn$$w201711
002255384 925__ $$b27 Mar 2017
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002255384 980__ $$aARTICLE$$aATLAS_Papers