002112269 001__ 2112269 002112269 005__ 20240216140400.0 002112269 0248_ $$aoai:cds.cern.ch:2112269$$pcerncds:CERN$$pcerncds:CERN:FULLTEXT$$pcerncds:FULLTEXT 002112269 0247_ $$2DOI$$a10.1140/epjc/s10052-016-4050-8 002112269 035__ $$9arXiv$$aoai:arXiv.org:1512.03657 002112269 035__ $$9Inspire$$a1409298 002112269 037__ $$9arXiv$$aarXiv:1512.03657$$chep-ex 002112269 037__ $$aCERN-PH-EP-2015-292 002112269 041__ $$aeng 002112269 084__ $$2CERN Library$$aPH-EP-2015-292 002112269 088__ $$9ATLAS-BPHY-2012-02-003 002112269 088__ $$aCERN-PH-EP-2015-292 002112269 100__ $$aAad, Georges$$iINSPIRE-00210391$$uMarseille, CPPM$$vCPPM - Aix-Marseille Université and CNRS/IN2P3 - Marseille - France 002112269 245__ $$aMeasurement of the differential cross-sections of prompt and non-prompt production of $J/\psi$ and $\psi(2\mathrm{S})$ in $pp$ collisions at $\sqrt{s} = 7$ and $8$ TeV with the ATLAS detector 002112269 246__ $$9arXiv$$aMeasurement of the differential cross-sections of prompt and non-prompt production of $J/\psi$ and $\psi(2\mathrm{S})$ in $pp$ collisions at $\sqrt{s} = 7$ and $8$ TeV with the ATLAS detector 002112269 269__ $$aGeneva$$bCERN$$c10 Dec 2015 002112269 260__ $$c2016-05-20 002112269 300__ $$a60 p 002112269 500__ $$9arXiv$$a42 pages plus author list + cover page (60 pages total), 13 figures, 3 tables, submitted to Eur. Phys. J. C. All figures including auxiliary figures are available at http://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/BPHY-2012-02/ 002112269 520__ $$aThe production rates of prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ mesons are measured using 2.1 $fb^{-1}$ and 11.4 $fb^{-1}$ of data collected with the ATLAS experiment at the LHC, in proton-proton collisions at $\sqrt{s}=7$ and 8 TeV respectively. Production cross-sections for both prompt and non-prompt production sources, ratios of $\psi(2\mathrm{S})$ to $J/\psi$ production, and fractions of non-prompt to inclusive production for $J/\psi$ and $\psi(2\mathrm{S})$ are measured double-differentially as a function of meson $p_{T}$ and rapidity. These measurements are made in a restricted fiducial volume and also corrected for geometrical acceptance after which they are compared to a variety of theoretical predictions. 002112269 520__ $$9HEPDATA$$hCERN-LHC. The production rates of prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ mesons are measured using 2.1 $fb^{-1}$ and 11.4 $fb^{-1}$ of data collected with the ATLAS experiment at the LHC, in proton-proton collisions at $\sqrt{s}=7$ and 8 TeV respectively. Production cross-sections for both prompt and non-prompt production sources, ratios of $\psi(2\mathrm{S})$ to $J/\psi$ production, and fractions of non-prompt to inclusive production for $J/\psi$ and $\psi(2\mathrm{S})$ are measured double-differentially as a function of meson $p_{T}$ and rapidity. These measurements are made in a restricted fiducial volume and also corrected for geometrical acceptance after which they are compared to a variety of theoretical predictions. 002112269 520__ $$9Springer$$aThe production rates of prompt and non-prompt $J/\psi $ and $\psi (2\mathrm {S})$ mesons in their dimuon decay modes are measured using 2.1 and 11.4 fb$^{-1}$ of data collected with the ATLAS experiment at the Large Hadron Collider, in proton–proton collisions at $\sqrt{s}=7$ and 8 respectively. Production cross-sections for prompt as well as non-prompt sources, ratios of $\psi (2\mathrm {S})$ to $J/\psi $ production, and the fractions of non-prompt production for $J/\psi $ and $\psi (2\mathrm {S})$ are measured as a function of meson transverse momentum and rapidity. The measurements are compared to theoretical predictions. 002112269 520__ $$9arXiv$$aThe production rates of prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ mesons are measured using 2.1 $fb^{-1}$ and 11.4 $fb^{-1}$ of data collected with the ATLAS experiment at the LHC, in proton-proton collisions at $\sqrt{s}=7$ and 8 TeV respectively. Production cross-sections for both prompt and non-prompt production sources, ratios of $\psi(2\mathrm{S})$ to $J/\psi$ production, and fractions of non-prompt to inclusive production for $J/\psi$ and $\psi(2\mathrm{S})$ are measured double-differentially as a function of meson $p_{T}$ and rapidity. These measurements are made in a restricted fiducial volume and also corrected for geometrical acceptance after which they are compared to a variety of theoretical predictions. 002112269 540__ $$3preprint$$aCC-BY-4.0 002112269 540__ $$3publication$$aCC-BY-4.0$$fSCOAP3 002112269 542__ $$3preprint$$dCERN$$g2015 002112269 542__ $$3publication$$dCERN$$g2016 002112269 595__ $$aautomerged 002112269 595__ $$aCERN-PH-EP 002112269 65017 $$2SzGeCERN$$aParticle Physics - Experiment 002112269 6531_ $$9CERN$$aflavor physics 002112269 6531_ $$9CERN$$aQCD 002112269 6531_ $$9CERN$$aB physics 002112269 6531_ $$9CERN$$acharm physics 002112269 6531_ $$9CERN$$aquarkonium 002112269 6531_ $$9CERN$$aheavy quark production 002112269 6531_ $$9CERN$$aexperimental results 002112269 693__ $$aCERN LHC$$eATLAS 002112269 690C_ $$aATLAS_Papers 002112269 690C_ $$aCERN 002112269 690C_ $$aARTICLE 002112269 695__ $$9LANL EDS$$ahep-ex 002112269 700__ $$aAbbott, Brad$$iINSPIRE-00060668$$uOklahoma U. 002112269 700__ $$aAbdallah, Jalal$$iINSPIRE-00305555$$uTaiwan, Inst. 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Eng. Inst. 002112269 700__ $$aBeltramello, Olga$$iINSPIRE-00211347$$uCERN 002112269 700__ $$aBenary, Odette$$iINSPIRE-00211360$$uTel Aviv U. 002112269 700__ $$aBenchekroun, Driss$$iINSPIRE-00211372$$uCasablanca U. 002112269 700__ $$aBender, Michael$$iINSPIRE-00387486$$uMunich U. 002112269 700__ $$aBendtz, Katarina$$iINSPIRE-00286205$$uStockholm U.$$uStockholm U., OKC 002112269 700__ $$aBenekos, Nektarios$$iINSPIRE-00066029$$uNatl. Tech. 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Phys. 002112269 700__ $$aBerger, Nicolas$$iINSPIRE-00066350$$uAnnecy, LAPP 002112269 700__ $$aBerghaus, Frank$$iINSPIRE-00036960$$uVictoria U. 002112269 700__ $$aBeringer, Jürg$$iINSPIRE-00066414$$uLBL, Berkeley 002112269 700__ $$aBernard, Clare$$iINSPIRE-00352198$$uBoston U. 002112269 700__ $$aBernard, Nathan Rogers$$iINSPIRE-00383935$$uMassachusetts U., Amherst 002112269 700__ $$aBernius, Catrin$$iINSPIRE-00211450$$uNew York U. 002112269 700__ $$aBernlochner, Florian Urs$$iINSPIRE-00144634$$uBonn U. 002112269 700__ $$aBerry, Tracey$$iINSPIRE-00041406$$uRoyal Holloway, U. of London 002112269 700__ $$aBerta, Peter$$iINSPIRE-00349738$$uCharles U. 002112269 700__ $$aBertella, Claudia$$iINSPIRE-00235836$$uMainz U. 002112269 700__ $$aBertoli, Gabriele$$iINSPIRE-00370978$$uStockholm U.$$uStockholm U., OKC 002112269 700__ $$aBertolucci, Federico$$iINSPIRE-00211461$$uINFN, Pisa$$uPisa U. 002112269 700__ $$aBertsche, Carolyn$$iINSPIRE-00375840$$uOklahoma U. 002112269 700__ $$aBertsche, David$$iINSPIRE-00377159$$uOklahoma U. 002112269 700__ $$aBesana, Maria Ilaria$$iINSPIRE-00211473$$uINFN, Milan 002112269 700__ $$aBesjes, Geert-Jan$$iINSPIRE-00286235$$uBohr Inst. 002112269 700__ $$aBessidskaia Bylund, Olga$$iINSPIRE-00348474$$uStockholm U.$$uStockholm U., OKC 002112269 700__ $$aBessner, Martin Florian$$iINSPIRE-00368451$$uDESY 002112269 700__ $$aBesson, Nathalie$$iINSPIRE-00211485$$uIRFU, Saclay 002112269 700__ $$aBetancourt, Christopher$$iINSPIRE-00362040$$uFreiburg U. 002112269 700__ $$aBethke, Siegfried$$iINSPIRE-00179262$$uMunich, Max Planck Inst. 002112269 700__ $$aBevan, Adrian John$$iINSPIRE-00042361$$uQueen Mary, U. of London 002112269 700__ $$aBhimji, Wahid$$iINSPIRE-00042527$$uLBL, Berkeley 002112269 700__ $$aBianchi, Riccardo-Maria$$iINSPIRE-00211497$$uPittsburgh U. 002112269 700__ $$aBianchini, Louis$$iINSPIRE-00295889$$uBrandeis U. 002112269 700__ $$aBianco, Michele$$iINSPIRE-00211509$$uCERN 002112269 700__ $$aBiebel, Otmar$$iINSPIRE-00066953$$uMunich U. 002112269 700__ $$aBiedermann, Dustin$$iINSPIRE-00392746$$uHumboldt U., Berlin 002112269 700__ $$aBieniek, Stephen Paul$$iINSPIRE-00235857$$uUniversity Coll. 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Inst. 002112269 700__ $$aBobbink, Gerjan$$iINSPIRE-00211581$$uFOM, Amsterdam 002112269 700__ $$aBobrovnikov, Victor$$iINSPIRE-00229343$$uNovosibirsk, IYF$$uNovosibirsk State U. 002112269 700__ $$aBocchetta, Simona Serena$$iINSPIRE-00235887$$uLund U. 002112269 700__ $$aBocci, Andrea$$iINSPIRE-00048999$$uDuke U. 002112269 700__ $$aBock, Christopher$$iINSPIRE-00367845$$uMunich U. 002112269 700__ $$aBoehler, Michael$$iINSPIRE-00211593$$uFreiburg U. 002112269 700__ $$aBogaerts, Joannes Andreas$$iINSPIRE-00211623$$uCERN 002112269 700__ $$aBogavac, Danijela$$iINSPIRE-00407355$$uBelgrade U. 002112269 700__ $$aBogdanchikov, Alexander$$iINSPIRE-00229367$$uNovosibirsk, IYF 002112269 700__ $$aBohm, Christian$$iINSPIRE-00324763$$uStockholm U. 002112269 700__ $$aBoisvert, Veronique$$iINSPIRE-00067915$$uRoyal Holloway, U. of London 002112269 700__ $$aBold, Tomasz$$iINSPIRE-00172488$$uAGH-UST, Cracow 002112269 700__ $$aBoldea, Venera$$iINSPIRE-00305639$$uBucharest, IFIN-HH 002112269 700__ $$aBoldyrev, Alexey$$iINSPIRE-00340190$$uMoscow State U. 002112269 700__ $$aBomben, Marco$$iINSPIRE-00052711$$uParis U., VI-VII 002112269 700__ $$aBona, Marcella$$iINSPIRE-00049930$$uQueen Mary, U. of London 002112269 700__ $$aBoonekamp, Maarten$$iINSPIRE-00211647$$uIRFU, Saclay 002112269 700__ $$aBorisov, Anatoly$$iINSPIRE-00226538$$uSerpukhov, IHEP 002112269 700__ $$aBorissov, Guennadi$$iINSPIRE-00068300$$uLancaster U. 002112269 700__ $$aBorroni, Sara$$iINSPIRE-00010952$$uDESY 002112269 700__ $$aBortfeldt, Jonathan$$iINSPIRE-00295897$$uMunich U. 002112269 700__ $$aBortolotto, Valerio$$iINSPIRE-00235896$$uHong Kong, Chinese U.$$uHong Kong U.$$uHong Kong U. 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Phys. Inst. 002112269 700__ $$aBrandt, Oleg$$iINSPIRE-00184109$$uKirchhoff Inst. Phys. 002112269 700__ $$aBratzler, Uwe$$iINSPIRE-00211726$$uTokyo Metropolitan U. 002112269 700__ $$aBrau, Benjamin$$iINSPIRE-00069043$$uMassachusetts U., Amherst 002112269 700__ $$aBrau, James$$iINSPIRE-00069055$$uOregon U. 002112269 700__ $$aBraun, Helmut$$iINSPIRE-00069076$$uWuppertal U. 002112269 700__ $$aBrazzale, Simone Federico$$iINSPIRE-00286276$$uINFN, Udine$$uUdine U. 002112269 700__ $$aBreaden Madden, William Dmitri$$iINSPIRE-00438010$$uGlasgow U. 002112269 700__ $$aBrendlinger, Kurt$$iINSPIRE-00338116$$uPennsylvania U. 002112269 700__ $$aBrennan, Amelia Jean$$iINSPIRE-00345743$$uMelbourne U. 002112269 700__ $$aBrenner, Lydia$$iINSPIRE-00386479$$uFOM, Amsterdam 002112269 700__ $$aBrenner, Richard$$iINSPIRE-00211740$$uUppsala U., Inst. Theor. Phys. 002112269 700__ $$aBressler, Shikma$$iINSPIRE-00211751$$uWeizmann Inst. 002112269 700__ $$aBristow, Kieran$$iINSPIRE-00356256$$uWitwatersrand U. 002112269 700__ $$aBristow, Timothy Michael$$iINSPIRE-00342520$$uEdinburgh U. 002112269 700__ $$aBritton, Dave$$iINSPIRE-00069310$$uGlasgow U. 002112269 700__ $$aBritzger, Daniel$$iINSPIRE-00306448$$uDESY 002112269 700__ $$aBrochu, Frederic$$iINSPIRE-00211763$$uCambridge U. 002112269 700__ $$aBrock, Ian$$iINSPIRE-00069330$$uBonn U. 002112269 700__ $$aBrock, Raymond$$iINSPIRE-00069341$$uMichigan State U. 002112269 700__ $$aBronner, Johanna$$iINSPIRE-00235910$$uMunich, Max Planck Inst. 002112269 700__ $$aBrooijmans, Gustaaf$$iINSPIRE-00069444$$uNevis Labs, Columbia U. 002112269 700__ $$aBrooks, Timothy$$iINSPIRE-00235925$$uRoyal Holloway, U. of London 002112269 700__ $$aBrooks, William$$iINSPIRE-00069460$$uSanta Maria U., Valparaiso 002112269 700__ $$aBrosamer, Jacquelyn$$iINSPIRE-00354197$$uLBL, Berkeley 002112269 700__ $$aBrost, Elizabeth$$iINSPIRE-00345015$$uOregon U. 002112269 700__ $$aBrown, Jonathan$$iINSPIRE-00342563$$uLPSC, Grenoble 002112269 700__ $$aBruckman de Renstrom, Pawel$$iINSPIRE-00180299$$uCracow, INP 002112269 700__ $$aBruncko, Dusan$$iINSPIRE-00179454$$uKosice, IEF 002112269 700__ $$aBruneliere, Renaud$$iINSPIRE-00240391$$uFreiburg U. 002112269 700__ $$aBruni, Alessia$$iINSPIRE-00069652$$uINFN, Bologna 002112269 700__ $$aBruni, Graziano$$iINSPIRE-00172026$$uINFN, Bologna 002112269 700__ $$aBruschi, Marco$$iINSPIRE-00211789$$uINFN, Bologna 002112269 700__ $$aBruscino, Nello$$iINSPIRE-00405244$$uBonn U. 002112269 700__ $$aBryngemark, Lene$$iINSPIRE-00329497$$uLund U. 002112269 700__ $$aBuanes, Trygve$$iINSPIRE-00229479$$uBergen U. 002112269 700__ $$aBuat, Quentin$$iINSPIRE-00235948$$uSimon Fraser U. 002112269 700__ $$aBuchholz, Peter$$iINSPIRE-00069835$$uSiegen U. 002112269 700__ $$aBuckley, Andrew$$iINSPIRE-00211807$$uGlasgow U. 002112269 700__ $$aBuda, Stelian Ioan$$iINSPIRE-00286284$$uBucharest, IFIN-HH 002112269 700__ $$aBudagov, Ioulian$$iINSPIRE-00211819$$uDubna, JINR 002112269 700__ $$aBuehrer, Felix$$iINSPIRE-00356527$$uFreiburg U. 002112269 700__ $$aBugge, Lars$$iINSPIRE-00211820$$uOslo U. 002112269 700__ $$aBugge, Magnar Kopangen$$iINSPIRE-00298334$$uOslo U. 002112269 700__ $$aBulekov, Oleg$$iINSPIRE-00211832$$uMoscow Phys. 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London 002112269 700__ $$aButti, Pierfrancesco$$iINSPIRE-00358725$$uFOM, Amsterdam 002112269 700__ $$aButtinger, William$$iINSPIRE-00229496$$uBrookhaven 002112269 700__ $$aBuzatu, Adrian$$iINSPIRE-00025104$$uGlasgow U. 002112269 700__ $$aBuzykaev, Aleksey$$iINSPIRE-00003784$$uNovosibirsk, IYF$$uNovosibirsk State U. 002112269 700__ $$aCabrera Urbán, Susana$$iINSPIRE-00211900$$uValencia U., IFIC 002112269 700__ $$aCaforio, Davide$$iINSPIRE-00211911$$uPrague, Tech. U. 002112269 700__ $$aCairo, Valentina$$iINSPIRE-00403090$$uINFN, Cosenza$$uCalabria U. 002112269 700__ $$aCakir, Orhan$$iINSPIRE-00211923$$uAnkara U. 002112269 700__ $$aCalace, Noemi$$iINSPIRE-00408949$$uGeneva U. 002112269 700__ $$aCalafiura, Paolo$$iINSPIRE-00070566$$uLBL, Berkeley 002112269 700__ $$aCalandri, Alessandro$$iINSPIRE-00366978$$uIRFU, Saclay 002112269 700__ $$aCalderini, Giovanni$$iINSPIRE-00070597$$uParis U., VI-VII 002112269 700__ $$aCalfayan, Philippe$$iINSPIRE-00032964$$uMunich U. 002112269 700__ $$aCaloba, Luiz$$iINSPIRE-00211947$$uRio de Janeiro Federal U. 002112269 700__ $$aCalvet, David$$iINSPIRE-00070696$$uClermont-Ferrand U. 002112269 700__ $$aCalvet, Samuel$$iINSPIRE-00019519$$uClermont-Ferrand U. 002112269 700__ $$aCamacho Toro, Reina$$iINSPIRE-00235957$$uChicago U., EFI 002112269 700__ $$aCamarda, Stefano$$iINSPIRE-00012655$$uDESY 002112269 700__ $$aCamarri, Paolo$$iINSPIRE-00226571$$uINFN, Rome$$uRome U., Tor Vergata 002112269 700__ $$aCameron, David$$iINSPIRE-00226583$$uOslo U. 002112269 700__ $$aCaminal Armadans, Roger$$iINSPIRE-00337611$$uIllinois U., Urbana 002112269 700__ $$aCampana, Simone$$iINSPIRE-00211959$$uCERN 002112269 700__ $$aCampanelli, Mario$$iINSPIRE-00070797$$uUniversity Coll. London 002112269 700__ $$aCampoverde, Angel$$iINSPIRE-00349667$$uSUNY, Stony Brook 002112269 700__ $$aCanale, Vincenzo$$iINSPIRE-00211960$$uINFN, Naples$$uNaples U. 002112269 700__ $$aCanepa, Anadi$$iINSPIRE-00045497$$uTRIUMF 002112269 700__ $$aCano Bret, Marc$$iINSPIRE-00361241$$uShanghai Jiao Tong U. 002112269 700__ $$aCantero, Josu$$iINSPIRE-00211972$$uMadrid, Autonoma U. 002112269 700__ $$aCantrill, Robert$$iINSPIRE-00235969$$uLIP, Lisbon 002112269 700__ $$aCao, Tingting$$iINSPIRE-00334314$$uSouthern Methodist U. 002112269 700__ $$aCapeans Garrido, Maria Del Mar$$iINSPIRE-00083814$$uCERN 002112269 700__ $$aCaprini, Irinel$$iINSPIRE-00070986$$uBucharest, IFIN-HH 002112269 700__ $$aCaprini, Mihai$$iINSPIRE-00211990$$uBucharest, IFIN-HH 002112269 700__ $$aCapua, Marcella$$iINSPIRE-00053925$$uINFN, Cosenza$$uCalabria U. 002112269 700__ $$aCaputo, Regina$$iINSPIRE-00212010$$uMainz U. 002112269 700__ $$aCardarelli, Roberto$$iINSPIRE-00212037$$uINFN, Rome 002112269 700__ $$aCardillo, Fabio$$iINSPIRE-00407956$$uFreiburg U. 002112269 700__ $$aCarli, Tancredi$$iINSPIRE-00212045$$uCERN 002112269 700__ $$aCarlino, Gianpaolo$$iINSPIRE-00212057$$uINFN, Naples 002112269 700__ $$aCarminati, Leonardo$$iINSPIRE-00212069$$uINFN, Milan$$uMilan U. 002112269 700__ $$aCaron, Sascha$$iINSPIRE-00057327$$uNIKHEF, Amsterdam 002112269 700__ $$aCarquin, Edson$$iINSPIRE-00023484$$uChile U., Catolica 002112269 700__ $$aCarrillo-Montoya, German D$$iINSPIRE-00212072$$uCERN 002112269 700__ $$aCarter, Janet$$iINSPIRE-00149979$$uCambridge U. 002112269 700__ $$aCarvalho, João$$iINSPIRE-00226606$$uLIP, Lisbon$$uCoimbra U. 002112269 700__ $$aCasadei, Diego$$iINSPIRE-00212084$$uUniversity Coll. London 002112269 700__ $$aCasado, Maria Pilar$$iINSPIRE-00071410$$uBarcelona, IFAE$$uBarcelona, Autonoma U. 002112269 700__ $$aCasolino, Mirkoantonio$$iINSPIRE-00366594$$uBarcelona, IFAE 002112269 700__ $$aCastaneda-Miranda, Elizabeth$$iINSPIRE-00212108$$uCape Town U. 002112269 700__ $$aCastelli, Angelantonio$$iINSPIRE-00342579$$uFOM, Amsterdam 002112269 700__ $$aCastillo Gimenez, Victoria$$iINSPIRE-00212120$$uValencia U., IFIC 002112269 700__ $$aCastro, Nuno Filipe$$iINSPIRE-00036257$$uLIP, Lisbon$$uPorto U. 002112269 700__ $$aCatastini, Pierluigi$$iINSPIRE-00041380$$uHarvard U., Phys. 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London 002112269 700__ $$aChitan, Adrian$$iINSPIRE-00236054$$uBucharest, IFIN-HH 002112269 700__ $$aChizhov, Mihail$$iINSPIRE-00227239$$uDubna, JINR 002112269 700__ $$aChoi, Kyungeon$$iINSPIRE-00180982$$uIndiana U. 002112269 700__ $$aChouridou, Sofia$$iINSPIRE-00212583$$uAthens U. 002112269 700__ $$aChow, Bonnie Kar Bo$$iINSPIRE-00334326$$uMunich U. 002112269 700__ $$aChristodoulou, Valentinos$$iINSPIRE-00407394$$uUniversity Coll. London 002112269 700__ $$aChromek-Burckhart, Doris$$iINSPIRE-00305640$$uCERN 002112269 700__ $$aChudoba, Jiri$$iINSPIRE-00150160$$uPrague, Inst. Phys. 002112269 700__ $$aChuinard, Annabelle Julia$$iINSPIRE-00378509$$uMcGill U. 002112269 700__ $$aChwastowski, Janusz$$iINSPIRE-00172390$$uCracow, INP 002112269 700__ $$aChytka, Ladislav$$iINSPIRE-00355090$$uPalacky U. 002112269 700__ $$aCiapetti, Guido$$iINSPIRE-00212602$$uINFN, Rome$$uRome U. 002112269 700__ $$aCiftci, Abbas Kenan$$iINSPIRE-00212614$$uAnkara U. 002112269 700__ $$aCinca, Diane$$iINSPIRE-00212637$$uGlasgow U. 002112269 700__ $$aCindro, Vladimir$$iINSPIRE-00073566$$uStefan Inst., Ljubljana 002112269 700__ $$aCioara, Irina Antonela$$iINSPIRE-00395821$$uBonn U. 002112269 700__ $$aCiocio, Alessandra$$iINSPIRE-00073579$$uLBL, Berkeley 002112269 700__ $$aCirotto, Francesco$$iINSPIRE-00414488$$uINFN, Naples$$uNaples U. 002112269 700__ $$aCitron, Zvi Hirsh$$iINSPIRE-00241320$$uWeizmann Inst. 002112269 700__ $$aCiubancan, Mihai$$iINSPIRE-00286339$$uBucharest, IFIN-HH 002112269 700__ $$aClark, Allan G$$iINSPIRE-00073664$$uGeneva U. 002112269 700__ $$aClark, Brian Lee$$iINSPIRE-00399058$$uHarvard U., Phys. 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U. Navale 002112269 700__ $$aCooke, Mark$$iINSPIRE-00183948$$uLBL, Berkeley 002112269 700__ $$aCooper, Ben$$iINSPIRE-00041328$$uUniversity Coll. London 002112269 700__ $$aCooper-Sarkar, Amanda$$iINSPIRE-00074346$$uOxford U. 002112269 700__ $$aCornelissen, Thijs$$iINSPIRE-00212766$$uWuppertal U. 002112269 700__ $$aCorradi, Massimo$$iINSPIRE-00001854$$uINFN, Rome$$uRome U. 002112269 700__ $$aCorriveau, Francois$$iINSPIRE-00074601$$uMcGill U.$$uIPP, Canada 002112269 700__ $$aCorso-Radu, Alina$$iINSPIRE-00305712$$uUC, Irvine 002112269 700__ $$aCortes-Gonzalez, Arely$$iINSPIRE-00212778$$uBarcelona, IFAE 002112269 700__ $$aCortiana, Giorgio$$iINSPIRE-00041311$$uMunich, Max Planck Inst. 002112269 700__ $$aCosta, Giuseppe$$iINSPIRE-00212780$$uINFN, Milan 002112269 700__ $$aCosta, María José$$iINSPIRE-00212791$$uValencia U., IFIC 002112269 700__ $$aCostanzo, Davide$$iINSPIRE-00212803$$uSheffield U. 002112269 700__ $$aCôté, David$$iINSPIRE-00027694$$uTexas U., Arlington 002112269 700__ $$aCottin, Giovanna$$iINSPIRE-00334334$$uCambridge U. 002112269 700__ $$aCowan, Glen$$iINSPIRE-00145177$$uRoyal Holloway, U. of London 002112269 700__ $$aCox, Brian$$iINSPIRE-00074854$$uManchester U. 002112269 700__ $$aCranmer, Kyle$$iINSPIRE-00074922$$uNew York U. 002112269 700__ $$aCree, Graham$$iINSPIRE-00349746$$uCarleton U. 002112269 700__ $$aCrépé-Renaudin, Sabine$$iINSPIRE-00074993$$uLPSC, Grenoble 002112269 700__ $$aCrescioli, Francesco$$iINSPIRE-00030662$$uParis U., VI-VII 002112269 700__ $$aCribbs, Wayne Allen$$iINSPIRE-00360698$$uStockholm U.$$uStockholm U., OKC 002112269 700__ $$aCrispin Ortuzar, Mireia$$iINSPIRE-00339030$$uOxford U. 002112269 700__ $$aCristinziani, Markus$$iINSPIRE-00058643$$uBonn U. 002112269 700__ $$aCroft, Vince$$iINSPIRE-00366990$$uNIKHEF, Amsterdam 002112269 700__ $$aCrosetti, Giovanni$$iINSPIRE-00212870$$uINFN, Cosenza$$uCalabria U. 002112269 700__ $$aCuhadar Donszelmann, Tulay$$iINSPIRE-00043040$$uSheffield U. 002112269 700__ $$aCummings, Jane$$iINSPIRE-00329170$$uYale U. 002112269 700__ $$aCuratolo, Maria$$iINSPIRE-00212948$$uFrascati 002112269 700__ $$aCúth, Jakub$$iINSPIRE-00384079$$uMainz U. 002112269 700__ $$aCuthbert, Cameron$$iINSPIRE-00286420$$uSydney U. 002112269 700__ $$aCzirr, Hendrik$$iINSPIRE-00229786$$uSiegen U. 002112269 700__ $$aCzodrowski, Patrick$$iINSPIRE-00236101$$uAlberta U. 002112269 700__ $$aD'Auria, Saverio$$iINSPIRE-00212973$$uGlasgow U. 002112269 700__ $$aD'Onofrio, Monica$$iINSPIRE-00041292$$uLiverpool U. 002112269 700__ $$aDa Cunha Sargedas De Sousa, Mario Jose$$iINSPIRE-00339043$$uLIP, Lisbon$$uLisbon U., CFNUL 002112269 700__ $$aDa Via, Cinzia$$iINSPIRE-00212924$$uManchester U. 002112269 700__ $$aDabrowski, Wladyslaw$$iINSPIRE-00178895$$uAGH-UST, Cracow 002112269 700__ $$aDafinca, Alexandru$$iINSPIRE-00236119$$uOxford U. 002112269 700__ $$aDai, Tiesheng$$iINSPIRE-00212987$$uMichigan U. 002112269 700__ $$aDale, Orjan$$iINSPIRE-00358740$$uBergen U. 002112269 700__ $$aDallaire, Frederick$$iINSPIRE-00334341$$uMontreal U. 002112269 700__ $$aDallapiccola, Carlo$$iINSPIRE-00075606$$uMassachusetts U., Amherst 002112269 700__ $$aDam, Mogens$$iINSPIRE-00075612$$uBohr Inst. 002112269 700__ $$aDandoy, Jeffrey Rogers$$iINSPIRE-00396074$$uChicago U., EFI 002112269 700__ $$aDang, Nguyen Phuong$$iINSPIRE-00410760$$uFreiburg U. 002112269 700__ $$aDaniells, Andrew Christopher$$iINSPIRE-00338698$$uBirmingham U. 002112269 700__ $$aDanninger, Matthias$$iINSPIRE-00324867$$uBritish Columbia U. 002112269 700__ $$aDano Hoffmann, Maria$$iINSPIRE-00354223$$uIRFU, Saclay 002112269 700__ $$aDao, Valerio$$iINSPIRE-00213005$$uFreiburg U. 002112269 700__ $$aDarbo, Giovanni$$iINSPIRE-00213017$$uINFN, Genoa 002112269 700__ $$aDarmora, Smita$$iINSPIRE-00337045$$uTexas U., Arlington 002112269 700__ $$aDassoulas, James$$iINSPIRE-00286438$$uAlberta U. 002112269 700__ $$aDattagupta, Aparajita$$iINSPIRE-00221224$$uIndiana U. 002112269 700__ $$aDavey, Will$$iINSPIRE-00213030$$uBonn U. 002112269 700__ $$aDavid, Claire$$iINSPIRE-00342591$$uVictoria U. 002112269 700__ $$aDavidek, Tomas$$iINSPIRE-00075913$$uCharles U. 002112269 700__ $$aDavies, Eleanor$$iINSPIRE-00236121$$uOxford U.$$uRutherford 002112269 700__ $$aDavies, Merlin$$iINSPIRE-00213066$$uTel Aviv U. 002112269 700__ $$aDavison, Peter$$iINSPIRE-00345754$$uUniversity Coll. 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U. Navale 002112269 700__ $$adella Volpe, Domenico$$iINSPIRE-00134280$$uGeneva U. 002112269 700__ $$aDelmastro, Marco$$iINSPIRE-00213273$$uAnnecy, LAPP 002112269 700__ $$aDelsart, Pierre-Antoine$$iINSPIRE-00213285$$uLPSC, Grenoble 002112269 700__ $$aDeluca, Carolina$$iINSPIRE-00018879$$uFOM, Amsterdam 002112269 700__ $$aDeMarco, David$$iINSPIRE-00381792$$uToronto U. 002112269 700__ $$aDemers, Sarah$$iINSPIRE-00177331$$uYale U. 002112269 700__ $$aDemichev, Mikhail$$iINSPIRE-00213297$$uDubna, JINR 002112269 700__ $$aDemilly, Aurelien$$iINSPIRE-00339052$$uParis U., VI-VII 002112269 700__ $$aDenisov, Sergey$$iINSPIRE-00076710$$uSerpukhov, IHEP 002112269 700__ $$aDerendarz, Dominik$$iINSPIRE-00229900$$uCracow, INP 002112269 700__ $$aDerkaoui, Jamal Eddine$$iINSPIRE-00213315$$uOujda U. 002112269 700__ $$aDerue, Frederic$$iINSPIRE-00051568$$uParis U., VI-VII 002112269 700__ $$aDervan, Paul$$iINSPIRE-00076798$$uLiverpool U. 002112269 700__ $$aDesch, Klaus Kurt$$iINSPIRE-00076819$$uBonn U. 002112269 700__ $$aDeterre, Cecile$$iINSPIRE-00220614$$uDESY 002112269 700__ $$aDeviveiros, Pier-Olivier$$iINSPIRE-00326955$$uCERN 002112269 700__ $$aDewhurst, Alastair$$iINSPIRE-00213327$$uRutherford 002112269 700__ $$aDhaliwal, Saminder$$iINSPIRE-00213340$$uBrandeis U. 002112269 700__ $$aDi Ciaccio, Anna$$iINSPIRE-00213364$$uINFN, Rome$$uRome U., Tor Vergata 002112269 700__ $$aDi Ciaccio, Lucia$$iINSPIRE-00213376$$uAnnecy, LAPP 002112269 700__ $$aDi Domenico, Antonio$$iINSPIRE-00332317$$uINFN, Rome$$uRome U. 002112269 700__ $$aDi Donato, Camilla$$iINSPIRE-00297740$$uINFN, Rome$$uRome U. 002112269 700__ $$aDi Girolamo, Alessandro$$iINSPIRE-00213388$$uCERN 002112269 700__ $$aDi Girolamo, Beniamino$$iINSPIRE-00085048$$uCERN 002112269 700__ $$aDi Mattia, Alessandro$$iINSPIRE-00213418$$uTechnion 002112269 700__ $$aDi Micco, Biagio$$iINSPIRE-00236191$$uINFN, Rome$$uRome III U. 002112269 700__ $$aDi Nardo, Roberto$$iINSPIRE-00213420$$uFrascati 002112269 700__ $$aDi Simone, Andrea$$iINSPIRE-00213431$$uFreiburg U. 002112269 700__ $$aDi Sipio, Riccardo$$iINSPIRE-00213443$$uToronto U. 002112269 700__ $$aDi Valentino, David$$iINSPIRE-00352611$$uCarleton U. 002112269 700__ $$aDiaconu, Cristinel$$iINSPIRE-00184938$$uMarseille, CPPM 002112269 700__ $$aDiamond, Miriam$$iINSPIRE-00389950$$uToronto U. 002112269 700__ $$aDias, Flavia$$iINSPIRE-00176100$$uEdinburgh U. 002112269 700__ $$aDiaz, Marco Aurelio$$iINSPIRE-00077083$$uChile U., Catolica 002112269 700__ $$aDiehl, Edward$$iINSPIRE-00213467$$uMichigan U. 002112269 700__ $$aDietrich, Janet$$iINSPIRE-00213479$$uHumboldt U., Berlin 002112269 700__ $$aDiglio, Sara$$iINSPIRE-00213492$$uMarseille, CPPM 002112269 700__ $$aDimitrievska, Aleksandra$$iINSPIRE-00358147$$uBelgrade U. 002112269 700__ $$aDingfelder, Jochen$$iINSPIRE-00049343$$uBonn U. 002112269 700__ $$aDita, Petre$$iINSPIRE-00213503$$uBucharest, IFIN-HH 002112269 700__ $$aDita, Sanda$$iINSPIRE-00306991$$uBucharest, IFIN-HH 002112269 700__ $$aDittus, Fridolin$$iINSPIRE-00077326$$uCERN 002112269 700__ $$aDjama, Fares$$iINSPIRE-00077370$$uMarseille, CPPM 002112269 700__ $$aDjobava, Tamar$$iINSPIRE-00213527$$uTbilisi State U. 002112269 700__ $$aDjuvsland, Julia Isabell$$iINSPIRE-00338727$$uKirchhoff Inst. 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U. 002112269 700__ $$aDyndal, Mateusz$$iINSPIRE-00359621$$uAGH-UST, Cracow 002112269 700__ $$aEckardt, Christoph$$iINSPIRE-00397250$$uDESY 002112269 700__ $$aEcker, Katharina Maria$$iINSPIRE-00387516$$uMunich, Max Planck Inst. 002112269 700__ $$aEdgar, Ryan Christopher$$iINSPIRE-00265484$$uMichigan U. 002112269 700__ $$aEdson, William$$iINSPIRE-00236226$$uSUNY, Albany 002112269 700__ $$aEdwards, Nicholas Charles$$iINSPIRE-00160603$$uEdinburgh U. 002112269 700__ $$aEhrenfeld, Wolfgang$$iINSPIRE-00054636$$uBonn U. 002112269 700__ $$aEifert, Till$$iINSPIRE-00305775$$uCERN 002112269 700__ $$aEigen, Gerald$$iINSPIRE-00079187$$uBergen U. 002112269 700__ $$aEinsweiler, Kevin$$iINSPIRE-00213832$$uLBL, Berkeley 002112269 700__ $$aEkelof, Tord$$iINSPIRE-00079263$$uUppsala U., Inst. Theor. Phys. 002112269 700__ $$aEl Kacimi, Mohamed$$iINSPIRE-00213844$$uCadi Ayyad U., Marrakech 002112269 700__ $$aEllert, Mattias$$iINSPIRE-00079322$$uUppsala U., Inst. Theor. 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Theor. Phys. 002112269 700__ $$aFerrari, Pamela$$iINSPIRE-00214210$$uFOM, Amsterdam 002112269 700__ $$aFerrari, Roberto$$iINSPIRE-00214221$$uINFN, Pavia 002112269 700__ $$aFerreira de Lima, Danilo Enoque$$iINSPIRE-00286519$$uGlasgow U. 002112269 700__ $$aFerrer, Antonio$$iINSPIRE-00080972$$uValencia U., IFIC 002112269 700__ $$aFerrere, Didier$$iINSPIRE-00188574$$uGeneva U. 002112269 700__ $$aFerretti, Claudio$$iINSPIRE-00028525$$uMichigan U. 002112269 700__ $$aFerretto Parodi, Andrea$$iINSPIRE-00214233$$uINFN, Genoa$$uGenoa U. 002112269 700__ $$aFiascaris, Maria$$iINSPIRE-00214245$$uChicago U., EFI 002112269 700__ $$aFiedler, Frank$$iINSPIRE-00081065$$uMainz U. 002112269 700__ $$aFilipčič, Andrej$$iINSPIRE-00081160$$uStefan Inst., Ljubljana 002112269 700__ $$aFilipuzzi, Marco$$iINSPIRE-00342629$$uDESY 002112269 700__ $$aFilthaut, Frank$$iINSPIRE-00081209$$uNIKHEF, Amsterdam 002112269 700__ $$aFincke-Keeler, Margret$$iINSPIRE-00081234$$uVictoria U. 002112269 700__ $$aFinelli, Kevin Daniel$$iINSPIRE-00337620$$uSydney U. 002112269 700__ $$aFiolhais, Miguel$$iINSPIRE-00214269$$uLIP, Lisbon$$uCoimbra U. 002112269 700__ $$aFiorini, Luca$$iINSPIRE-00214275$$uValencia U., IFIC 002112269 700__ $$aFiran, Ana$$iINSPIRE-00214287$$uSouthern Methodist U. 002112269 700__ $$aFischer, Adam$$iINSPIRE-00376085$$uSUNY, Albany 002112269 700__ $$aFischer, Cora$$iINSPIRE-00387867$$uBarcelona, IFAE 002112269 700__ $$aFischer, Julia$$iINSPIRE-00336608$$uWuppertal U. 002112269 700__ $$aFisher, Wade Cameron$$iINSPIRE-00052479$$uMichigan State U. 002112269 700__ $$aFitzgerald, Eric Andrew$$iINSPIRE-00291897$$uBrandeis U. 002112269 700__ $$aFlaschel, Nils$$iINSPIRE-00371327$$uDESY 002112269 700__ $$aFleck, Ivor$$iINSPIRE-00081605$$uSiegen U. 002112269 700__ $$aFleischmann, Philipp$$iINSPIRE-00214324$$uMichigan U. 002112269 700__ $$aFleischmann, Sebastian$$iINSPIRE-00214336$$uWuppertal U. 002112269 700__ $$aFletcher, Gareth Thomas$$iINSPIRE-00334379$$uSheffield U. 002112269 700__ $$aFletcher, Gregory$$iINSPIRE-00332919$$uQueen Mary, U. of London 002112269 700__ $$aFletcher, Rob Roy MacGregor$$iINSPIRE-00405355$$uPennsylvania U. 002112269 700__ $$aFlick, Tobias$$iINSPIRE-00214348$$uWuppertal U. 002112269 700__ $$aFloderus, Anders$$iINSPIRE-00291905$$uLund U. 002112269 700__ $$aFlores Castillo, Luis$$iINSPIRE-00041212$$uHong Kong, Chinese U. 002112269 700__ $$aFlowerdew, Michael$$iINSPIRE-00214350$$uMunich, Max Planck Inst. 002112269 700__ $$aFormica, Andrea$$iINSPIRE-00081940$$uIRFU, Saclay 002112269 700__ $$aForti, Alessandra$$iINSPIRE-00027700$$uManchester U. 002112269 700__ $$aFournier, Daniel$$iINSPIRE-00144690$$uOrsay, LAL 002112269 700__ $$aFox, Harald$$iINSPIRE-00082068$$uLancaster U. 002112269 700__ $$aFracchia, Silvia$$iINSPIRE-00361393$$uBarcelona, IFAE 002112269 700__ $$aFrancavilla, Paolo$$iINSPIRE-00305814$$uParis U., VI-VII 002112269 700__ $$aFranchini, Matteo$$iINSPIRE-00293056$$uINFN, Bologna$$uBologna U. 002112269 700__ $$aFrancis, David$$iINSPIRE-00214393$$uCERN 002112269 700__ $$aFranconi, Laura$$iINSPIRE-00371528$$uOslo U. 002112269 700__ $$aFranklin, Melissa$$iINSPIRE-00082230$$uHarvard U., Phys. 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Sci. 002112269 700__ $$aFuster, Juan$$iINSPIRE-00214444$$uValencia U., IFIC 002112269 700__ $$aGabaldon, Carolina$$iINSPIRE-00214457$$uLPSC, Grenoble 002112269 700__ $$aGabizon, Ofir$$iINSPIRE-00214469$$uWuppertal U. 002112269 700__ $$aGabrielli, Alessandro$$iINSPIRE-00342638$$uINFN, Bologna$$uBologna U. 002112269 700__ $$aGabrielli, Andrea$$iINSPIRE-00339066$$uINFN, Rome$$uRome U. 002112269 700__ $$aGach, Grzegorz$$iINSPIRE-00184415$$uBirmingham U. 002112269 700__ $$aGadatsch, Stefan$$iINSPIRE-00342641$$uCERN 002112269 700__ $$aGadomski, Szymon$$iINSPIRE-00083092$$uGeneva U. 002112269 700__ $$aGagliardi, Guido$$iINSPIRE-00214470$$uINFN, Genoa$$uGenoa U. 002112269 700__ $$aGagnon, Pauline$$iINSPIRE-00083104$$uIndiana U. 002112269 700__ $$aGalea, Cristina$$iINSPIRE-00039048$$uNIKHEF, Amsterdam 002112269 700__ $$aGalhardo, Bruno$$iINSPIRE-00291919$$uLIP, Lisbon$$uCoimbra U. 002112269 700__ $$aGallas, Elizabeth$$iINSPIRE-00083337$$uOxford U. 002112269 700__ $$aGallop, Bruce$$iINSPIRE-00214494$$uRutherford 002112269 700__ $$aGallus, Petr$$iINSPIRE-00015179$$uPrague, Tech. 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London 002112269 700__ $$aHessey, Nigel$$iINSPIRE-00090012$$uFOM, Amsterdam 002112269 700__ $$aHetherly, Jeffrey Wayne$$iINSPIRE-00392821$$uSouthern Methodist U. 002112269 700__ $$aHickling, Robert$$iINSPIRE-00333090$$uQueen Mary, U. of London 002112269 700__ $$aHigón-Rodriguez, Emilio$$iINSPIRE-00215655$$uValencia U., IFIC 002112269 700__ $$aHill, Ewan$$iINSPIRE-00345031$$uVictoria U. 002112269 700__ $$aHill, John$$iINSPIRE-00090279$$uCambridge U. 002112269 700__ $$aHiller, Karl Heinz$$iINSPIRE-00185199$$uDESY 002112269 700__ $$aHillier, Stephen$$iINSPIRE-00090318$$uBirmingham U. 002112269 700__ $$aHinchliffe, Ian$$iINSPIRE-00161746$$uLBL, Berkeley 002112269 700__ $$aHines, Elizabeth$$iINSPIRE-00215709$$uPennsylvania U. 002112269 700__ $$aHinman, Rachel Reisner$$iINSPIRE-00384144$$uLBL, Berkeley 002112269 700__ $$aHirose, Minoru$$iINSPIRE-00215710$$uTokyo Inst. Tech. 002112269 700__ $$aHirschbuehl, Dominic$$iINSPIRE-00041134$$uWuppertal U. 002112269 700__ $$aHobbs, John$$iINSPIRE-00090491$$uSUNY, Stony Brook 002112269 700__ $$aHod, Noam$$iINSPIRE-00215734$$uFOM, Amsterdam 002112269 700__ $$aHodgkinson, Mark$$iINSPIRE-00030600$$uSheffield U. 002112269 700__ $$aHodgson, Paul$$iINSPIRE-00215746$$uSheffield U. 002112269 700__ $$aHoecker, Andreas$$iINSPIRE-00090516$$uCERN 002112269 700__ $$aHoeferkamp, Martin$$iINSPIRE-00021230$$uNew Mexico U. 002112269 700__ $$aHoenig, Friedrich$$iINSPIRE-00376466$$uMunich U. 002112269 700__ $$aHohlfeld, Marc$$iINSPIRE-00039005$$uMainz U. 002112269 700__ $$aHohn, David$$iINSPIRE-00392879$$uBonn U. 002112269 700__ $$aHolmes, Tova Ray$$iINSPIRE-00349798$$uLBL, Berkeley 002112269 700__ $$aHomann, Michael$$iINSPIRE-00381480$$uDortmund U. 002112269 700__ $$aHong, Tae Min$$iINSPIRE-00042918$$uPittsburgh U. 002112269 700__ $$aHooft van Huysduynen, Loek$$iINSPIRE-00236399$$uNew York U. 002112269 700__ $$aHopkins, Walter$$iINSPIRE-00009068$$uOregon U. 002112269 700__ $$aHorii, Yasuyuki$$iINSPIRE-00370685$$uNagoya U. 002112269 700__ $$aHorton, Arthur James$$iINSPIRE-00376759$$uSimon Fraser U. 002112269 700__ $$aHostachy, Jean-Yves$$iINSPIRE-00215837$$uLPSC, Grenoble 002112269 700__ $$aHou, Suen$$iINSPIRE-00091198$$uTaiwan, Inst. Phys. 002112269 700__ $$aHoummada, Abdeslam$$iINSPIRE-00215849$$uCasablanca U. 002112269 700__ $$aHoward, Jacob$$iINSPIRE-00286560$$uOxford U. 002112269 700__ $$aHowarth, James$$iINSPIRE-00230643$$uDESY 002112269 700__ $$aHrabovsky, Miroslav$$iINSPIRE-00334449$$uPalacky U. 002112269 700__ $$aHristova, Ivana$$iINSPIRE-00286578$$uHumboldt U., Berlin 002112269 700__ $$aHrivnac, Julius$$iINSPIRE-00215850$$uOrsay, LAL 002112269 700__ $$aHryn'ova, Tetiana$$iINSPIRE-00049739$$uAnnecy, LAPP 002112269 700__ $$aHrynevich, Aliaksei$$iINSPIRE-00383643$$uMinsk, High Energy Phys. Ctr. 002112269 700__ $$aHsu, Catherine$$iINSPIRE-00375245$$uWitwatersrand U. 002112269 700__ $$aHsu, Pai-hsien Jennifer$$iINSPIRE-00036505$$uTaiwan, Inst. Phys.$$uTaiwan, Natl. Tsing Hua U. 002112269 700__ $$aHsu, Shih-Chieh$$iINSPIRE-00041120$$uWashington U., Seattle 002112269 700__ $$aHu, Diedi$$iINSPIRE-00295905$$uNevis Labs, Columbia U. 002112269 700__ $$aHu, Qipeng$$iINSPIRE-00386928$$uHefei, CUST 002112269 700__ $$aHu, Xueye$$iINSPIRE-00338739$$uMichigan U. 002112269 700__ $$aHuang, Yanping$$iINSPIRE-00340219$$uDESY 002112269 700__ $$aHubacek, Zdenek$$iINSPIRE-00032940$$uPrague, Tech. U. 002112269 700__ $$aHubaut, Fabrice$$iINSPIRE-00215862$$uMarseille, CPPM 002112269 700__ $$aHuegging, Fabian$$iINSPIRE-00215874$$uBonn U. 002112269 700__ $$aHuffman, Todd Brian$$iINSPIRE-00215888$$uOxford U. 002112269 700__ $$aHughes, Emlyn$$iINSPIRE-00091540$$uNevis Labs, Columbia U. 002112269 700__ $$aHughes, Gareth$$iINSPIRE-00091551$$uLancaster U. 002112269 700__ $$aHuhtinen, Mika$$iINSPIRE-00320486$$uCERN 002112269 700__ $$aHülsing, Tobias Alexander$$iINSPIRE-00286581$$uMainz U. 002112269 700__ $$aHuseynov, Nazim$$iINSPIRE-00215894$$uDubna, JINR$$uBaku, Inst. 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Chem. Phys. 002112269 700__ $$aJaekel, Martin$$iINSPIRE-00216071$$uCERN 002112269 700__ $$aJain, Vivek$$iINSPIRE-00093006$$uSUNY, Albany 002112269 700__ $$aJakobs, Karl$$iINSPIRE-00093013$$uFreiburg U. 002112269 700__ $$aJakobsen, Sune$$iINSPIRE-00216083$$uCERN 002112269 700__ $$aJakoubek, Tomas$$iINSPIRE-00236452$$uPrague, Inst. Phys. 002112269 700__ $$aJakubek, Jan$$iINSPIRE-00216095$$uPrague, Tech. U. 002112269 700__ $$aJamin, David Olivier$$iINSPIRE-00019160$$uOklahoma State U. 002112269 700__ $$aJana, Dilip$$iINSPIRE-00216107$$uLouisiana Tech. U. 002112269 700__ $$aJansen, Eric$$iINSPIRE-00216120$$uUniversity Coll. London 002112269 700__ $$aJansky, Roland$$iINSPIRE-00389298$$uInnsbruck U. 002112269 700__ $$aJanssen, Jens$$iINSPIRE-00339121$$uBonn U. 002112269 700__ $$aJanus, Michel$$iINSPIRE-00216144$$uGottingen U., II. Phys. Inst. 002112269 700__ $$aJarlskog, Göran$$iINSPIRE-00175123$$uLund U. 002112269 700__ $$aJavadov, Namig$$iINSPIRE-00358780$$uDubna, JINR$$uBaku, Inst. 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Phys. 002112269 700__ $$aJorge, Pedro$$iINSPIRE-00227131$$uLIP, Lisbon$$uLisbon U., CFNUL 002112269 700__ $$aJoshi, Kiran Daniel$$iINSPIRE-00286612$$uManchester U. 002112269 700__ $$aJovicevic, Jelena$$iINSPIRE-00286620$$uTRIUMF 002112269 700__ $$aJu, Xiangyang$$iINSPIRE-00230799$$uWisconsin U., Madison 002112269 700__ $$aJung, Christian$$iINSPIRE-00236485$$uDortmund U. 002112269 700__ $$aJussel, Patrick$$iINSPIRE-00216304$$uInnsbruck U. 002112269 700__ $$aJuste Rozas, Aurelio$$iINSPIRE-00094149$$uBarcelona, IFAE$$uICREA, Barcelona 002112269 700__ $$aKaci, Mohammed$$iINSPIRE-00216328$$uValencia U., IFIC 002112269 700__ $$aKaczmarska, Anna$$iINSPIRE-00216330$$uCracow, INP 002112269 700__ $$aKado, Marumi$$iINSPIRE-00216354$$uOrsay, LAL 002112269 700__ $$aKagan, Harris$$iINSPIRE-00144825$$uOhio State U. 002112269 700__ $$aKagan, Michael$$iINSPIRE-00008953$$uSLAC 002112269 700__ $$aKahn, Sebastien Jonathan$$iINSPIRE-00388044$$uMarseille, CPPM 002112269 700__ $$aKajomovitz, Enrique$$iINSPIRE-00216378$$uDuke U. 002112269 700__ $$aKalderon, Charles William$$iINSPIRE-00358313$$uOxford U. 002112269 700__ $$aKama, Sami$$iINSPIRE-00216391$$uSouthern Methodist U. 002112269 700__ $$aKamenshchikov, Andrey$$iINSPIRE-00374470$$uSerpukhov, IHEP 002112269 700__ $$aKanaya, Naoko$$iINSPIRE-00197922$$uTokyo U., ICEPP 002112269 700__ $$aKaneti, Steven$$iINSPIRE-00236623$$uCambridge U. 002112269 700__ $$aKantserov, Vadim$$iINSPIRE-00216415$$uMoscow Phys. 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Phys. 002112269 700__ $$aNemethy, Peter$$iINSPIRE-00321590$$uNew York U. 002112269 700__ $$aNepomuceno, Andre Asevedo$$iINSPIRE-00221072$$uRio de Janeiro Federal U. 002112269 700__ $$aNessi, Marzio$$iINSPIRE-00221084$$uCERN$$uGeneva U. 002112269 700__ $$aNeubauer, Mark$$iINSPIRE-00110982$$uIllinois U., Urbana 002112269 700__ $$aNeumann, Manuel$$iINSPIRE-00288618$$uWuppertal U. 002112269 700__ $$aNeves, Ricardo$$iINSPIRE-00221104$$uNew York U. 002112269 700__ $$aNevski, Pavel$$iINSPIRE-00221110$$uBrookhaven 002112269 700__ $$aNewman, Paul$$iINSPIRE-00111158$$uBirmingham U. 002112269 700__ $$aNguyen, Duong Hai$$iINSPIRE-00009056$$uArgonne 002112269 700__ $$aNickerson, Richard$$iINSPIRE-00221121$$uOxford U. 002112269 700__ $$aNicolaidou, Rosy$$iINSPIRE-00216944$$uIRFU, Saclay 002112269 700__ $$aNicquevert, Bertrand$$iINSPIRE-00111358$$uCERN 002112269 700__ $$aNielsen, Jason$$iINSPIRE-00111400$$uUC, Santa Cruz 002112269 700__ $$aNikiforou, Nikiforos$$iINSPIRE-00237074$$uNevis Labs, Columbia U. 002112269 700__ $$aNikiforov, Andriy$$iINSPIRE-00185481$$uHumboldt U., Berlin 002112269 700__ $$aNikolaenko, Vladimir$$iINSPIRE-00231894$$uSerpukhov, IHEP$$uMoscow, MIPT 002112269 700__ $$aNikolic-Audit, Irena$$iINSPIRE-00306103$$uParis U., VI-VII 002112269 700__ $$aNikolopoulos, Konstantinos$$iINSPIRE-00221145$$uBirmingham U. 002112269 700__ $$aNilsen, Jon Kerr$$iINSPIRE-00393094$$uOslo U. 002112269 700__ $$aNilsson, Paul$$iINSPIRE-00221150$$uBrookhaven 002112269 700__ $$aNinomiya, Yoichi$$iINSPIRE-00231907$$uTokyo U., ICEPP 002112269 700__ $$aNisati, Aleandro$$iINSPIRE-00221160$$uINFN, Rome 002112269 700__ $$aNisius, Richard$$iINSPIRE-00111714$$uMunich, Max Planck Inst. 002112269 700__ $$aNobe, Takuya$$iINSPIRE-00286888$$uTokyo U., ICEPP 002112269 700__ $$aNodulman, Lawrence$$iINSPIRE-00111767$$uArgonne 002112269 700__ $$aNomachi, Masaharu$$iINSPIRE-00111877$$uOsaka U. 002112269 700__ $$aNomidis, Ioannis$$iINSPIRE-00221178$$uCarleton U. 002112269 700__ $$aNooney, Tamsin$$iINSPIRE-00389111$$uQueen Mary, U. of London 002112269 700__ $$aNorberg, Scarlet$$iINSPIRE-00286896$$uOklahoma U. 002112269 700__ $$aNordberg, Markus$$iINSPIRE-00111954$$uCERN 002112269 700__ $$aNovgorodova, Olga$$iINSPIRE-00285705$$uDresden, Tech. U. 002112269 700__ $$aNowak, Sebastian$$iINSPIRE-00390105$$uMunich, Max Planck Inst. 002112269 700__ $$aNozaki, Mitsuaki$$iINSPIRE-00226787$$uKEK, Tsukuba 002112269 700__ $$aNozka, Libor$$iINSPIRE-00152530$$uPalacky U. 002112269 700__ $$aNtekas, Konstantinos$$iINSPIRE-00349891$$uNatl. Tech. U., Athens 002112269 700__ $$aNunes Hanninger, Guilherme$$iINSPIRE-00221202$$uMelbourne U. 002112269 700__ $$aNunnemann, Thomas$$iINSPIRE-00046334$$uMunich U. 002112269 700__ $$aNurse, Emily$$iINSPIRE-00052439$$uUniversity Coll. London 002112269 700__ $$aNuti, Francesco$$iINSPIRE-00346170$$uMelbourne U. 002112269 700__ $$aO'Brien, Brendan Joseph$$iINSPIRE-00286904$$uEdinburgh U. 002112269 700__ $$aO'grady, Fionnbarr$$iINSPIRE-00354252$$uArizona U. 002112269 700__ $$aO'Neil, Dugan$$iINSPIRE-00112324$$uSimon Fraser U. 002112269 700__ $$aO'Shea, Val$$iINSPIRE-00112370$$uGlasgow U. 002112269 700__ $$aOakham, Gerald$$iINSPIRE-00112393$$uCarleton U.$$uTRIUMF 002112269 700__ $$aOberlack, Horst$$iINSPIRE-00112415$$uMunich, Max Planck Inst. 002112269 700__ $$aObermann, Theresa$$iINSPIRE-00362697$$uBonn U. 002112269 700__ $$aOcariz, Jose$$iINSPIRE-00112459$$uParis U., VI-VII 002112269 700__ $$aOchi, Atsuhiko$$iINSPIRE-00112469$$uKobe U. 002112269 700__ $$aOchoa, Ines$$iINSPIRE-00335577$$uUniversity Coll. London 002112269 700__ $$aOchoa-Ricoux, Juan Pedro$$iINSPIRE-00404468$$uChile U., Catolica 002112269 700__ $$aOda, Susumu$$iINSPIRE-00036017$$uKyushu U. 002112269 700__ $$aOdaka, Shigeru$$iINSPIRE-00221251$$uKEK, Tsukuba 002112269 700__ $$aOgren, Harold$$iINSPIRE-00112633$$uIndiana U. 002112269 700__ $$aOh, Alexander$$iINSPIRE-00320498$$uManchester U. 002112269 700__ $$aOh, Seog$$iINSPIRE-00112667$$uDuke U. 002112269 700__ $$aOhm, Christian$$iINSPIRE-00221275$$uLBL, Berkeley 002112269 700__ $$aOhman, Henrik$$iINSPIRE-00342728$$uUppsala U., Inst. Theor. Phys. 002112269 700__ $$aOide, Hideyuki$$iINSPIRE-00379657$$uCERN 002112269 700__ $$aOkamura, Wataru$$iINSPIRE-00295913$$uOsaka U. 002112269 700__ $$aOkawa, Hideki$$iINSPIRE-00221308$$uTsukuba U. 002112269 700__ $$aOkumura, Yasuyuki$$iINSPIRE-00221310$$uChicago U., EFI 002112269 700__ $$aOkuyama, Toyonobu$$iINSPIRE-00226798$$uKEK, Tsukuba 002112269 700__ $$aOlariu, Albert$$iINSPIRE-00237105$$uBucharest, IFIN-HH 002112269 700__ $$aOlivares Pino, Sebastian Andres$$iINSPIRE-00286912$$uEdinburgh U. 002112269 700__ $$aOliveira Damazio, Denis$$iINSPIRE-00221335$$uBrookhaven 002112269 700__ $$aOliver Garcia, Elena$$iINSPIRE-00221347$$uValencia U., IFIC 002112269 700__ $$aOlszewski, Andrzej$$iINSPIRE-00256380$$uCracow, INP 002112269 700__ $$aOlszowska, Jolanta$$iINSPIRE-00221360$$uCracow, INP 002112269 700__ $$aOnofre, António$$iINSPIRE-00221372$$uLIP, Lisbon$$uMinho U. 002112269 700__ $$aOnogi, Kouta$$iINSPIRE-00415586$$uNagoya U. 002112269 700__ $$aOnyisi, Peter$$iINSPIRE-00057397$$uChicago U., EFI$$uTexas U. 002112269 700__ $$aOram, Christopher$$iINSPIRE-00113272$$uTRIUMF 002112269 700__ $$aOreglia, Mark$$iINSPIRE-00113317$$uChicago U., EFI 002112269 700__ $$aOren, Yona$$iINSPIRE-00221389$$uTel Aviv U. 002112269 700__ $$aOrestano, Domizia$$iINSPIRE-00113321$$uINFN, Rome$$uRome III U. 002112269 700__ $$aOrlando, Nicola$$iINSPIRE-00286920$$uAristotle U., Thessaloniki 002112269 700__ $$aOropeza Barrera, Cristina$$iINSPIRE-00010114$$uGlasgow U. 002112269 700__ $$aOrr, Robert$$iINSPIRE-00113411$$uToronto U. 002112269 700__ $$aOsculati, Bianca$$iINSPIRE-00221407$$uINFN, Genoa$$uGenoa U. 002112269 700__ $$aOspanov, Rustem$$iINSPIRE-00029272$$uManchester U. 002112269 700__ $$aOtero y Garzon, Gustavo$$iINSPIRE-00046137$$uBuenos Aires U. 002112269 700__ $$aOtono, Hidetoshi$$iINSPIRE-00348488$$uKyushu U. 002112269 700__ $$aOuchrif, Mohamed$$iINSPIRE-00232012$$uOujda U. 002112269 700__ $$aOuld-Saada, Farid$$iINSPIRE-00221439$$uOslo U. 002112269 700__ $$aOuraou, Ahmimed$$iINSPIRE-00221444$$uIRFU, Saclay 002112269 700__ $$aOussoren, Koen Pieter$$iINSPIRE-00342930$$uFOM, Amsterdam 002112269 700__ $$aOuyang, Qun$$iINSPIRE-00221456$$uBeijing, Inst. High Energy Phys. 002112269 700__ $$aOvcharova, Ana$$iINSPIRE-00237127$$uLBL, Berkeley 002112269 700__ $$aOwen, Mark$$iINSPIRE-00007985$$uGlasgow U. 002112269 700__ $$aOwen, Rhys Edward$$iINSPIRE-00390165$$uBirmingham U. 002112269 700__ $$aOzcan, Veysi Erkcan$$iINSPIRE-00221480$$uBogazici U. 002112269 700__ $$aOzturk, Nurcan$$iINSPIRE-00026861$$uTexas U., Arlington 002112269 700__ $$aPachal, Katherine$$iINSPIRE-00337371$$uSimon Fraser U. 002112269 700__ $$aPacheco Pages, Andres$$iINSPIRE-00221495$$uBarcelona, IFAE 002112269 700__ $$aPadilla Aranda, Cristobal$$iINSPIRE-00306128$$uBarcelona, IFAE 002112269 700__ $$aPagáčová, Martina$$iINSPIRE-00359670$$uFreiburg U. 002112269 700__ $$aPagan Griso, Simone$$iINSPIRE-00022647$$uLBL, Berkeley 002112269 700__ $$aPaganis, Efstathios$$iINSPIRE-00221502$$uSheffield U. 002112269 700__ $$aPaige, Frank$$iINSPIRE-00221520$$uBrookhaven 002112269 700__ $$aPais, Preema$$iINSPIRE-00237142$$uMassachusetts U., Amherst 002112269 700__ $$aPajchel, Katarina$$iINSPIRE-00221539$$uOslo U. 002112269 700__ $$aPalacino, Gabriel$$iINSPIRE-00237152$$uYork U., Canada 002112269 700__ $$aPalestini, Sandro$$iINSPIRE-00221549$$uCERN 002112269 700__ $$aPalka, Marek$$iINSPIRE-00371751$$uJagiellonian U. 002112269 700__ $$aPallin, Dominique$$iINSPIRE-00221552$$uClermont-Ferrand U. 002112269 700__ $$aPalma, Alberto$$iINSPIRE-00221564$$uLIP, Lisbon$$uLisbon U., CFNUL 002112269 700__ $$aPan, Yibin$$iINSPIRE-00145162$$uWisconsin U., Madison 002112269 700__ $$aPanagiotopoulou, Evgenia$$iINSPIRE-00232057$$uNatl. Tech. U., Athens 002112269 700__ $$aPandini, Carlo Enrico$$iINSPIRE-00388516$$uParis U., VI-VII 002112269 700__ $$aPanduro Vazquez, William$$iINSPIRE-00042480$$uRoyal Holloway, U. of London 002112269 700__ $$aPani, Priscilla$$iINSPIRE-00291943$$uStockholm U.$$uStockholm U., OKC 002112269 700__ $$aPanitkin, Sergey$$iINSPIRE-00114270$$uBrookhaven 002112269 700__ $$aPantea, Dan$$iINSPIRE-00114319$$uBucharest, IFIN-HH 002112269 700__ $$aPaolozzi, Lorenzo$$iINSPIRE-00349900$$uGeneva U. 002112269 700__ $$aPapadopoulou, Theodora$$iINSPIRE-00185572$$uNatl. Tech. U., Athens 002112269 700__ $$aPapageorgiou, Konstantinos$$iINSPIRE-00114455$$uAristotle U., Thessaloniki 002112269 700__ $$aParamonov, Alexander$$iINSPIRE-00040880$$uArgonne 002112269 700__ $$aParedes Hernandez, Daniela$$iINSPIRE-00286969$$uAristotle U., Thessaloniki 002112269 700__ $$aParker, Michael Andrew$$iINSPIRE-00114726$$uCambridge U. 002112269 700__ $$aParker, Kerry Ann$$iINSPIRE-00371766$$uSheffield U. 002112269 700__ $$aParodi, Fabrizio$$iINSPIRE-00339598$$uINFN, Genoa$$uGenoa U. 002112269 700__ $$aParsons, John$$iINSPIRE-00114789$$uNevis Labs, Columbia U. 002112269 700__ $$aParzefall, Ulrich$$iINSPIRE-00114827$$uFreiburg U. 002112269 700__ $$aPasqualucci, Enrico$$iINSPIRE-00221595$$uINFN, Rome 002112269 700__ $$aPassaggio, Stefano$$iINSPIRE-00114912$$uINFN, Genoa 002112269 700__ $$aPastore, Fernanda$$iINSPIRE-00221629$$uINFN, Rome$$uRome III U. 002112269 700__ $$aPastore, Francesca$$iINSPIRE-00221618$$uRoyal Holloway, U. of London 002112269 700__ $$aPásztor, Gabriella$$iINSPIRE-00115001$$uCarleton U. 002112269 700__ $$aPataraia, Sophio$$iINSPIRE-00221648$$uWuppertal U. 002112269 700__ $$aPatel, Nikhul$$iINSPIRE-00221656$$uSydney U. 002112269 700__ $$aPater, Joleen$$iINSPIRE-00221668$$uManchester U. 002112269 700__ $$aPauly, Thilo$$iINSPIRE-00221680$$uCERN 002112269 700__ $$aPearce, James$$iINSPIRE-00333118$$uVictoria U. 002112269 700__ $$aPearson, Benjamin$$iINSPIRE-00368502$$uOklahoma U. 002112269 700__ $$aPedersen, Lars Egholm$$iINSPIRE-00379022$$uBohr Inst. 002112269 700__ $$aPedersen, Maiken$$iINSPIRE-00298350$$uOslo U. 002112269 700__ $$aPedraza Lopez, Sebastian$$iINSPIRE-00288626$$uValencia U., IFIC 002112269 700__ $$aPedro, Rute$$iINSPIRE-00357018$$uLIP, Lisbon$$uLisbon U., CFNUL 002112269 700__ $$aPeleganchuk, Sergey$$iINSPIRE-00221714$$uNovosibirsk, IYF$$uNovosibirsk State U. 002112269 700__ $$aPelikan, Daniel$$iINSPIRE-00286977$$uUppsala U., Inst. Theor. Phys. 002112269 700__ $$aPenc, Ondrej$$iINSPIRE-00408388$$uPrague, Inst. Phys. 002112269 700__ $$aPeng, Cong$$iINSPIRE-00407696$$uBeijing, Inst. High Energy Phys. 002112269 700__ $$aPeng, Haiping$$iINSPIRE-00217635$$uHefei, CUST 002112269 700__ $$aPenning, Bjoern$$iINSPIRE-00007584$$uChicago U., EFI 002112269 700__ $$aPenwell, John$$iINSPIRE-00221730$$uIndiana U. 002112269 700__ $$aPerepelitsa, Dennis$$iINSPIRE-00342739$$uBrookhaven 002112269 700__ $$aPerez Codina, Estel$$iINSPIRE-00221766$$uTRIUMF 002112269 700__ $$aPérez García-Estañ, María Teresa$$iINSPIRE-00221771$$uValencia U., IFIC 002112269 700__ $$aPerini, Laura$$iINSPIRE-00221789$$uINFN, Milan$$uMilan U. 002112269 700__ $$aPernegger, Heinz$$iINSPIRE-00115755$$uCERN 002112269 700__ $$aPerrella, Sabrina$$iINSPIRE-00377109$$uINFN, Naples$$uNaples U. 002112269 700__ $$aPeschke, Richard$$iINSPIRE-00356050$$uDESY 002112269 700__ $$aPeshekhonov, Vladimir$$iINSPIRE-00221820$$uDubna, JINR 002112269 700__ $$aPeters, Krisztian$$iINSPIRE-00055152$$uCERN 002112269 700__ $$aPeters, Yvonne$$iINSPIRE-00008252$$uManchester U. 002112269 700__ $$aPetersen, Brian$$iINSPIRE-00115959$$uCERN 002112269 700__ $$aPetersen, Troels$$iINSPIRE-00221831$$uBohr Inst. 002112269 700__ $$aPetit, Elisabeth$$iINSPIRE-00221840$$uDESY 002112269 700__ $$aPetridis, Andreas$$iINSPIRE-00232124$$uAdelaide U., Sch. Chem. Phys. 002112269 700__ $$aPetridou, Chariclia$$iINSPIRE-00116033$$uAristotle U., Thessaloniki 002112269 700__ $$aPetroff, Pierre$$iINSPIRE-00116049$$uOrsay, LAL 002112269 700__ $$aPetrolo, Emilio$$iINSPIRE-00221866$$uINFN, Rome 002112269 700__ $$aPetrucci, Fabrizio$$iINSPIRE-00221875$$uINFN, Rome$$uRome III U. 002112269 700__ $$aPettersson, Nora Emilia$$iINSPIRE-00360876$$uTokyo Inst. Tech. 002112269 700__ $$aPezoa, Raquel$$iINSPIRE-00221890$$uSanta Maria U., Valparaiso 002112269 700__ $$aPhillips, Peter William$$iINSPIRE-00116199$$uRutherford 002112269 700__ $$aPiacquadio, Giacinto$$iINSPIRE-00221917$$uSLAC 002112269 700__ $$aPianori, Elisabetta$$iINSPIRE-00009958$$uWarwick U. 002112269 700__ $$aPicazio, Attilio$$iINSPIRE-00286993$$uGeneva U. 002112269 700__ $$aPiccaro, Elisa$$iINSPIRE-00221925$$uQueen Mary, U. of London 002112269 700__ $$aPiccinini, Maurizio$$iINSPIRE-00116257$$uINFN, Bologna$$uBologna U. 002112269 700__ $$aPickering, Mark Andrew$$iINSPIRE-00378953$$uOxford U. 002112269 700__ $$aPiegaia, Ricardo$$iINSPIRE-00152829$$uBuenos Aires U. 002112269 700__ $$aPignotti, David$$iINSPIRE-00287001$$uOhio State U. 002112269 700__ $$aPilcher, James$$iINSPIRE-00116477$$uChicago U., EFI 002112269 700__ $$aPilkington, Andrew$$iINSPIRE-00221938$$uManchester U. 002112269 700__ $$aPin, Arnaud Willy J$$iINSPIRE-00191428$$uManchester U. 002112269 700__ $$aPina, João Antonio$$iINSPIRE-00306151$$uLIP, Lisbon$$uLisbon U., CFNUL 002112269 700__ $$aPinamonti, Michele$$iINSPIRE-00221947$$uINFN, Udine$$uUdine U.$$uSISSA, Trieste 002112269 700__ $$aPinfold, James$$iINSPIRE-00116512$$uAlberta U. 002112269 700__ $$aPingel, Almut$$iINSPIRE-00332954$$uBohr Inst. 002112269 700__ $$aPires, Sylvestre$$iINSPIRE-00362919$$uParis U., VI-VII 002112269 700__ $$aPirumov, Hayk$$iINSPIRE-00243807$$uDESY 002112269 700__ $$aPitt, Michael$$iINSPIRE-00354261$$uWeizmann Inst. 002112269 700__ $$aPizio, Caterina$$iINSPIRE-00221965$$uINFN, Milan$$uMilan U. 002112269 700__ $$aPlazak, Lukas$$iINSPIRE-00374596$$uComenius U. 002112269 700__ $$aPleier, Marc-Andre$$iINSPIRE-00046720$$uBrookhaven 002112269 700__ $$aPleskot, Vojtech$$iINSPIRE-00335597$$uCharles U. 002112269 700__ $$aPlotnikova, Elena$$iINSPIRE-00237193$$uDubna, JINR 002112269 700__ $$aPlucinski, Pawel$$iINSPIRE-00174206$$uStockholm U.$$uStockholm U., OKC 002112269 700__ $$aPluth, Daniel$$iINSPIRE-00365906$$uIowa State U. 002112269 700__ $$aPoettgen, Ruth$$iINSPIRE-00335606$$uStockholm U.$$uStockholm U., OKC 002112269 700__ $$aPoggioli, Luc$$iINSPIRE-00221996$$uOrsay, LAL 002112269 700__ $$aPohl, David-leon$$iINSPIRE-00288837$$uBonn U. 002112269 700__ $$aPolesello, Giacomo$$iINSPIRE-00117049$$uINFN, Pavia 002112269 700__ $$aPoley, Anne-luise$$iINSPIRE-00407830$$uDESY 002112269 700__ $$aPolicicchio, Antonio$$iINSPIRE-00020903$$uINFN, Cosenza$$uCalabria U. 002112269 700__ $$aPolifka, Richard$$iINSPIRE-00185642$$uToronto U. 002112269 700__ $$aPolini, Alessandro$$iINSPIRE-00172064$$uINFN, Bologna 002112269 700__ $$aPollard, Christopher Samuel$$iINSPIRE-00345073$$uGlasgow U. 002112269 700__ $$aPolychronakos, Venetios$$iINSPIRE-00177114$$uBrookhaven 002112269 700__ $$aPommès, Kathy$$iINSPIRE-00222020$$uCERN 002112269 700__ $$aPontecorvo, Ludovico$$iINSPIRE-00222031$$uINFN, Rome 002112269 700__ $$aPope, Bernard$$iINSPIRE-00117279$$uMichigan State U. 002112269 700__ $$aPopeneciu, Gabriel Alexandru$$iINSPIRE-00226844$$uINCDTIM, Cluj Napoca 002112269 700__ $$aPopovic, Dragan$$iINSPIRE-00222048$$uBelgrade U. 002112269 700__ $$aPoppleton, Alan$$iINSPIRE-00222058$$uCERN 002112269 700__ $$aPospisil, Stanislav$$iINSPIRE-00222085$$uPrague, Tech. U. 002112269 700__ $$aPotamianos, Karolos$$iINSPIRE-00019188$$uLBL, Berkeley 002112269 700__ $$aPotrap, Igor$$iINSPIRE-00222100$$uDubna, JINR 002112269 700__ $$aPotter, Christina$$iINSPIRE-00222115$$uSussex U. 002112269 700__ $$aPotter, Christopher$$iINSPIRE-00042218$$uOregon U. 002112269 700__ $$aPoulard, Gilbert$$iINSPIRE-00222120$$uCERN 002112269 700__ $$aPoveda, Joaquin$$iINSPIRE-00222132$$uCERN 002112269 700__ $$aPozdnyakov, Valery$$iINSPIRE-00237200$$uDubna, JINR 002112269 700__ $$aPralavorio, Pascal$$iINSPIRE-00117512$$uMarseille, CPPM 002112269 700__ $$aPranko, Aliaksandr$$iINSPIRE-00049000$$uLBL, Berkeley 002112269 700__ $$aPrasad, Srivas$$iINSPIRE-00256773$$uCERN 002112269 700__ $$aPrell, Soeren$$iINSPIRE-00117610$$uIowa State U. 002112269 700__ $$aPrice, Darren$$iINSPIRE-00027472$$uManchester U. 002112269 700__ $$aPrice, Lawrence$$iINSPIRE-00117710$$uArgonne 002112269 700__ $$aPrimavera, Margherita$$iINSPIRE-00117740$$uINFN, Lecce 002112269 700__ $$aPrince, Sebastien$$iINSPIRE-00359694$$uMcGill U. 002112269 700__ $$aProissl, Manuel$$iINSPIRE-00255144$$uEdinburgh U. 002112269 700__ $$aProkofiev, Kirill$$iINSPIRE-00002760$$uHong Kong U. Sci. Tech. 002112269 700__ $$aProkoshin, Fedor$$iINSPIRE-00030407$$uSanta Maria U., Valparaiso 002112269 700__ $$aProtopapadaki, Eftychia-sofia$$iINSPIRE-00337664$$uIRFU, Saclay 002112269 700__ $$aProtopopescu, Serban$$iINSPIRE-00117905$$uBrookhaven 002112269 700__ $$aProudfoot, James$$iINSPIRE-00117915$$uArgonne 002112269 700__ $$aPrzybycien, Mariusz$$iINSPIRE-00117955$$uAGH-UST, Cracow 002112269 700__ $$aPtacek, Elizabeth$$iINSPIRE-00222177$$uOregon U. 002112269 700__ $$aPuddu, Daniele$$iINSPIRE-00367527$$uINFN, Rome$$uRome III U. 002112269 700__ $$aPueschel, Elisa$$iINSPIRE-00047574$$uMassachusetts U., Amherst 002112269 700__ $$aPuldon, David$$iINSPIRE-00237218$$uSUNY, Stony Brook 002112269 700__ $$aPurohit, Milind$$iINSPIRE-00118098$$uBrookhaven$$uSouth Carolina U. 002112269 700__ $$aPuzo, Patrick$$iINSPIRE-00222199$$uOrsay, LAL 002112269 700__ $$aQian, Jianming$$iINSPIRE-00118167$$uMichigan U. 002112269 700__ $$aQin, Gang$$iINSPIRE-00273074$$uGlasgow U. 002112269 700__ $$aQin, Yang$$iINSPIRE-00367059$$uManchester U. 002112269 700__ $$aQuadt, Arnulf$$iINSPIRE-00118216$$uGottingen U., II. Phys. Inst. 002112269 700__ $$aQuarrie, David$$iINSPIRE-00222245$$uLBL, Berkeley 002112269 700__ $$aQuayle, William$$iINSPIRE-00222250$$uINFN, Udine$$uICTP, Trieste 002112269 700__ $$aQueitsch-Maitland, Michaela$$iINSPIRE-00367060$$uManchester U. 002112269 700__ $$aQuilty, Donnchadha$$iINSPIRE-00014465$$uGlasgow U. 002112269 700__ $$aRaddum, Silje$$iINSPIRE-00380321$$uOslo U. 002112269 700__ $$aRadeka, Veljko$$iINSPIRE-00304240$$uBrookhaven 002112269 700__ $$aRadescu, Voica$$iINSPIRE-00028751$$uDESY 002112269 700__ $$aRadhakrishnan, Sooraj Krishnan$$iINSPIRE-00354278$$uSUNY, Stony Brook 002112269 700__ $$aRadloff, Peter$$iINSPIRE-00237221$$uOregon U. 002112269 700__ $$aRados, Pere$$iINSPIRE-00362130$$uMelbourne U. 002112269 700__ $$aRagusa, Francesco$$iINSPIRE-00194492$$uINFN, Milan$$uMilan U. 002112269 700__ $$aRahal, Ghita$$iINSPIRE-00301248$$uCC, Villeurbanne 002112269 700__ $$aRajagopalan, Srinivasan$$iINSPIRE-00222308$$uBrookhaven 002112269 700__ $$aRammensee, Michael$$iINSPIRE-00222312$$uCERN 002112269 700__ $$aRangel-Smith, Camila$$iINSPIRE-00237235$$uUppsala U., Inst. Theor. Phys. 002112269 700__ $$aRauscher, Felix$$iINSPIRE-00222332$$uMunich U. 002112269 700__ $$aRave, Stefan$$iINSPIRE-00386585$$uMainz U. 002112269 700__ $$aRavenscroft, Thomas$$iINSPIRE-00334506$$uGlasgow U. 002112269 700__ $$aRaymond, Michel$$iINSPIRE-00222353$$uCERN 002112269 700__ $$aRead, Alexander Lincoln$$iINSPIRE-00119327$$uOslo U. 002112269 700__ $$aReadioff, Nathan Peter$$iINSPIRE-00368514$$uLiverpool U. 002112269 700__ $$aRebuzzi, Daniela$$iINSPIRE-00222361$$uINFN, Pavia$$uPavia U. 002112269 700__ $$aRedelbach, Andreas$$iINSPIRE-00222375$$uWurzburg U. 002112269 700__ $$aRedlinger, George$$iINSPIRE-00119430$$uBrookhaven 002112269 700__ $$aReece, Ryan$$iINSPIRE-00016749$$uUC, Santa Cruz 002112269 700__ $$aReeves, Kendall$$iINSPIRE-00142245$$uTexas U., Dallas 002112269 700__ $$aRehnisch, Laura$$iINSPIRE-00354285$$uHumboldt U., Berlin 002112269 700__ $$aReichert, Joseph$$iINSPIRE-00423182$$uPennsylvania U. 002112269 700__ $$aReisin, Hernan$$iINSPIRE-00237260$$uBuenos Aires U. 002112269 700__ $$aRelich, Matthew$$iINSPIRE-00334510$$uUC, Irvine 002112269 700__ $$aRembser, Christoph$$iINSPIRE-00222420$$uCERN 002112269 700__ $$aRen, Huan$$iINSPIRE-00360700$$uBeijing, Inst. High Energy Phys. 002112269 700__ $$aRenaud, Adrien$$iINSPIRE-00287044$$uOrsay, LAL 002112269 700__ $$aRescigno, Marco$$iINSPIRE-00119727$$uINFN, Rome 002112269 700__ $$aResconi, Silvia$$iINSPIRE-00222441$$uINFN, Milan 002112269 700__ $$aRezanova, Olga$$iINSPIRE-00235827$$uNovosibirsk, IYF$$uNovosibirsk State U. 002112269 700__ $$aReznicek, Pavel$$iINSPIRE-00222462$$uCharles U. 002112269 700__ $$aRezvani, Reyhaneh$$iINSPIRE-00226862$$uMontreal U. 002112269 700__ $$aRichter, Robert$$iINSPIRE-00120026$$uMunich, Max Planck Inst. 002112269 700__ $$aRichter, Stefan$$iINSPIRE-00393156$$uUniversity Coll. London 002112269 700__ $$aRichter-Was, Elzbieta$$iINSPIRE-00222485$$uJagiellonian U. 002112269 700__ $$aRicken, Oliver$$iINSPIRE-00394440$$uBonn U. 002112269 700__ $$aRidel, Melissa$$iINSPIRE-00052999$$uParis U., VI-VII 002112269 700__ $$aRieck, Patrick$$iINSPIRE-00333614$$uHumboldt U., Berlin 002112269 700__ $$aRiegel, Christian Johann$$iINSPIRE-00390368$$uWuppertal U. 002112269 700__ $$aRieger, Julia$$iINSPIRE-00367854$$uGottingen U., II. Phys. Inst. 002112269 700__ $$aRifki, Othmane$$iINSPIRE-00421293$$uOklahoma U. 002112269 700__ $$aRijssenbeek, Michael$$iINSPIRE-00120164$$uSUNY, Stony Brook 002112269 700__ $$aRimoldi, Adele$$iINSPIRE-00120224$$uINFN, Pavia$$uPavia U. 002112269 700__ $$aRinaldi, Lorenzo$$iINSPIRE-00222509$$uINFN, Bologna 002112269 700__ $$aRistić, Branislav$$iINSPIRE-00442335$$uGeneva U. 002112269 700__ $$aRitsch, Elmar$$iINSPIRE-00334537$$uCERN 002112269 700__ $$aRiu, Imma$$iINSPIRE-00120419$$uBarcelona, IFAE 002112269 700__ $$aRizatdinova, Flera$$iINSPIRE-00048668$$uOklahoma State U. 002112269 700__ $$aRizvi, Eram$$iINSPIRE-00120467$$uQueen Mary, U. of London 002112269 700__ $$aRobertson, Steven$$iINSPIRE-00120586$$uMcGill U.$$uIPP, Canada 002112269 700__ $$aRobichaud-Veronneau, Andree$$iINSPIRE-00220239$$uMcGill U. 002112269 700__ $$aRobinson, Dave$$iINSPIRE-00222525$$uCambridge U. 002112269 700__ $$aRobinson, James$$iINSPIRE-00222565$$uDESY 002112269 700__ $$aRobson, Aidan$$iINSPIRE-00052951$$uGlasgow U. 002112269 700__ $$aRoda, Chiara$$iINSPIRE-00222584$$uINFN, Pisa$$uPisa U. 002112269 700__ $$aRoe, Shaun$$iINSPIRE-00222620$$uCERN 002112269 700__ $$aRøhne, Ole$$iINSPIRE-00120872$$uOslo U. 002112269 700__ $$aRolli, Simona$$iINSPIRE-00120949$$uTufts U. 002112269 700__ $$aRomaniouk, Anatoli$$iINSPIRE-00222643$$uMoscow Phys. Eng. Inst. 002112269 700__ $$aRomano, Marino$$iINSPIRE-00237277$$uINFN, Bologna$$uBologna U. 002112269 700__ $$aRomano Saez, Silvestre Marino$$iINSPIRE-00390473$$uClermont-Ferrand U. 002112269 700__ $$aRomero Adam, Elena$$iINSPIRE-00237280$$uValencia U., IFIC 002112269 700__ $$aRompotis, Nikolaos$$iINSPIRE-00311758$$uWashington U., Seattle 002112269 700__ $$aRonzani, Manfredi$$iINSPIRE-00265551$$uFreiburg U. 002112269 700__ $$aRoos, Lydia$$iINSPIRE-00121125$$uParis U., VI-VII 002112269 700__ $$aRos, Eduardo$$iINSPIRE-00222681$$uValencia U., IFIC 002112269 700__ $$aRosati, Stefano$$iINSPIRE-00226874$$uINFN, Rome 002112269 700__ $$aRosbach, Kilian$$iINSPIRE-00237292$$uFreiburg U. 002112269 700__ $$aRose, Peyton$$iINSPIRE-00376762$$uUC, Santa Cruz 002112269 700__ $$aRosendahl, Peter Lundgaard$$iINSPIRE-00222703$$uBergen U. 002112269 700__ $$aRosenthal, Oliver$$iINSPIRE-00237317$$uSiegen U. 002112269 700__ $$aRossetti, Valerio$$iINSPIRE-00222722$$uStockholm U.$$uStockholm U., OKC 002112269 700__ $$aRossi, Elvira$$iINSPIRE-00232312$$uINFN, Naples$$uNaples U. 002112269 700__ $$aRossi, Leonardo Paolo$$iINSPIRE-00222731$$uINFN, Genoa 002112269 700__ $$aRosten, Jonatan$$iINSPIRE-00396349$$uCambridge U. 002112269 700__ $$aRosten, Rachel$$iINSPIRE-00345760$$uWashington U., Seattle 002112269 700__ $$aRotaru, Marina$$iINSPIRE-00185709$$uBucharest, IFIN-HH 002112269 700__ $$aRoth, Itamar$$iINSPIRE-00232324$$uWeizmann Inst. 002112269 700__ $$aRothberg, Joseph$$iINSPIRE-00147103$$uWashington U., Seattle 002112269 700__ $$aRousseau, David$$iINSPIRE-00121457$$uOrsay, LAL 002112269 700__ $$aRoyon, Christophe$$iINSPIRE-00121542$$uIRFU, Saclay 002112269 700__ $$aRozanov, Alexandre$$iINSPIRE-00121556$$uMarseille, CPPM 002112269 700__ $$aRozen, Yoram$$iINSPIRE-00222740$$uTechnion 002112269 700__ $$aRuan, Xifeng$$iINSPIRE-00227177$$uWitwatersrand U. 002112269 700__ $$aRubbo, Francesco$$iINSPIRE-00263547$$uSLAC 002112269 700__ $$aRubinskiy, Igor$$iINSPIRE-00287058$$uDESY 002112269 700__ $$aRud, Viacheslav$$iINSPIRE-00222774$$uMoscow State U. 002112269 700__ $$aRudolph, Christian$$iINSPIRE-00237326$$uDresden, Tech. U. 002112269 700__ $$aRudolph, Matthew Scott$$iINSPIRE-00176709$$uToronto U. 002112269 700__ $$aRühr, Frederik$$iINSPIRE-00222786$$uFreiburg U. 002112269 700__ $$aRuiz-Martinez, Aranzazu$$iINSPIRE-00222798$$uCERN 002112269 700__ $$aRurikova, Zuzana$$iINSPIRE-00217990$$uFreiburg U. 002112269 700__ $$aRusakovich, Nikolai$$iINSPIRE-00301212$$uDubna, JINR 002112269 700__ $$aRuschke, Alexander$$iINSPIRE-00295921$$uMunich U. 002112269 700__ $$aRussell, Heather$$iINSPIRE-00381301$$uWashington U., Seattle 002112269 700__ $$aRutherfoord, John$$iINSPIRE-00122016$$uArizona U. 002112269 700__ $$aRuthmann, Nils$$iINSPIRE-00334543$$uFreiburg U. 002112269 700__ $$aRyabov, Yury$$iINSPIRE-00306193$$uSt. Petersburg, INP 002112269 700__ $$aRybar, Martin$$iINSPIRE-00287074$$uIllinois U., Urbana 002112269 700__ $$aRybkin, Grigori$$iINSPIRE-00222835$$uOrsay, LAL 002112269 700__ $$aRyder, Nick$$iINSPIRE-00232381$$uOxford U. 002112269 700__ $$aSaavedra, Aldo$$iINSPIRE-00222859$$uSydney U. 002112269 700__ $$aSabato, Gabriele$$iINSPIRE-00375930$$uFOM, Amsterdam 002112269 700__ $$aSacerdoti, Sabrina$$iINSPIRE-00339152$$uBuenos Aires U. 002112269 700__ $$aSaddique, Asif$$iINSPIRE-00237330$$uAlberta U. 002112269 700__ $$aSadrozinski, Hartmut$$iINSPIRE-00122290$$uUC, Santa Cruz 002112269 700__ $$aSadykov, Renat$$iINSPIRE-00222866$$uDubna, JINR 002112269 700__ $$aSafai Tehrani, Francesco$$iINSPIRE-00041870$$uINFN, Rome 002112269 700__ $$aSaha, Puja$$iINSPIRE-00418043$$uNorthern Illinois U. 002112269 700__ $$aSahinsoy, Merve$$iINSPIRE-00394595$$uKirchhoff Inst. Phys. 002112269 700__ $$aSaimpert, Matthias$$iINSPIRE-00387311$$uIRFU, Saclay 002112269 700__ $$aSaito, Tomoyuki$$iINSPIRE-00399900$$uTokyo U., ICEPP 002112269 700__ $$aSakamoto, Hiroshi$$iINSPIRE-00122550$$uTokyo U., ICEPP 002112269 700__ $$aSakurai, Yuki$$iINSPIRE-00263552$$uWaseda U. 002112269 700__ $$aSalamanna, Giuseppe$$iINSPIRE-00040818$$uINFN, Rome$$uRome III U. 002112269 700__ $$aSalamon, Andrea$$iINSPIRE-00226887$$uINFN, Rome 002112269 700__ $$aSalazar Loyola, Javier Esteban$$iINSPIRE-00393200$$uSanta Maria U., Valparaiso 002112269 700__ $$aSaleem, Muhammad$$iINSPIRE-00055510$$uOklahoma U. 002112269 700__ $$aSalek, David$$iINSPIRE-00185720$$uFOM, Amsterdam 002112269 700__ $$aSales De Bruin, Pedro Henrique$$iINSPIRE-00354071$$uWashington U., Seattle 002112269 700__ $$aSalihagic, Denis$$iINSPIRE-00122755$$uMunich, Max Planck Inst. 002112269 700__ $$aSalnikov, Andrei$$iINSPIRE-00122791$$uSLAC 002112269 700__ $$aSalt, José$$iINSPIRE-00222878$$uValencia U., IFIC 002112269 700__ $$aSalvatore, Daniela$$iINSPIRE-00222890$$uINFN, Cosenza$$uCalabria U. 002112269 700__ $$aSalvatore, Pasquale Fabrizio$$iINSPIRE-00042310$$uSussex U. 002112269 700__ $$aSalvucci, Antonio$$iINSPIRE-00222904$$uHong Kong, Chinese U. 002112269 700__ $$aSalzburger, Andreas$$iINSPIRE-00222917$$uCERN 002112269 700__ $$aSammel, Dirk$$iINSPIRE-00394771$$uFreiburg U. 002112269 700__ $$aSampsonidis, Dimitrios$$iINSPIRE-00222923$$uAristotle U., Thessaloniki 002112269 700__ $$aSanchez, Arturo$$iINSPIRE-00237353$$uINFN, Naples$$uNaples U. 002112269 700__ $$aSánchez, Javier$$iINSPIRE-00224147$$uValencia U., IFIC 002112269 700__ $$aSanchez Martinez, Victoria$$iINSPIRE-00237361$$uValencia U., IFIC 002112269 700__ $$aSandaker, Heidi$$iINSPIRE-00222934$$uOslo U. 002112269 700__ $$aSandbach, Ruth Laura$$iINSPIRE-00358569$$uQueen Mary, U. of London 002112269 700__ $$aSander, Heinz Georg$$iINSPIRE-00325963$$uMainz U. 002112269 700__ $$aSanders, Michiel$$iINSPIRE-00038712$$uMunich U. 002112269 700__ $$aSandhoff, Marisa$$iINSPIRE-00008264$$uWuppertal U. 002112269 700__ $$aSandoval, Carlos$$iINSPIRE-00237372$$uAntonio Narino U. 002112269 700__ $$aSandstroem, Rikard$$iINSPIRE-00007979$$uMunich, Max Planck Inst. 002112269 700__ $$aSankey, Dave$$iINSPIRE-00123095$$uRutherford 002112269 700__ $$aSannino, Mario$$iINSPIRE-00123116$$uINFN, Genoa$$uGenoa U. 002112269 700__ $$aSansoni, Andrea$$iINSPIRE-00222964$$uFrascati 002112269 700__ $$aSantoni, Claudio$$iINSPIRE-00161887$$uClermont-Ferrand U. 002112269 700__ $$aSantonico, Rinaldo$$iINSPIRE-00222976$$uINFN, Rome$$uRome U., Tor Vergata 002112269 700__ $$aSantos, Helena$$iINSPIRE-00232412$$uLIP, Lisbon 002112269 700__ $$aSantoyo Castillo, Itzebelt$$iINSPIRE-00291958$$uSussex U. 002112269 700__ $$aSapp, Kevin$$iINSPIRE-00335926$$uPittsburgh U. 002112269 700__ $$aSapronov, Andrey$$iINSPIRE-00011775$$uDubna, JINR 002112269 700__ $$aSaraiva, João$$iINSPIRE-00306227$$uLIP, Lisbon$$uLisbon U., CFNUL 002112269 700__ $$aSarrazin, Bjorn$$iINSPIRE-00334550$$uBonn U. 002112269 700__ $$aSasaki, Osamu$$iINSPIRE-00123320$$uKEK, Tsukuba 002112269 700__ $$aSasaki, Yuichi$$iINSPIRE-00287109$$uTokyo U., ICEPP 002112269 700__ $$aSato, Koji$$iINSPIRE-00048967$$uTsukuba U. 002112269 700__ $$aSauvage, Gilles$$iINSPIRE-00222998$$uAnnecy, LAPP 002112269 700__ $$aSauvan, Emmanuel$$iINSPIRE-00185747$$uAnnecy, LAPP 002112269 700__ $$aSavage, Graham$$iINSPIRE-00375948$$uRoyal Holloway, U. of London 002112269 700__ $$aSavard, Pierre$$iINSPIRE-00123492$$uToronto U.$$uTRIUMF 002112269 700__ $$aSawyer, Craig$$iINSPIRE-00337679$$uRutherford 002112269 700__ $$aSawyer, Lee$$iINSPIRE-00123608$$uLouisiana Tech. U. 002112269 700__ $$aSaxon, James$$iINSPIRE-00332965$$uChicago U., EFI 002112269 700__ $$aSbarra, Carla$$iINSPIRE-00223003$$uINFN, Bologna 002112269 700__ $$aSbrizzi, Antonio$$iINSPIRE-00223019$$uINFN, Bologna$$uBologna U. 002112269 700__ $$aScanlon, Tim$$iINSPIRE-00038709$$uUniversity Coll. London 002112269 700__ $$aScannicchio, Diana$$iINSPIRE-00223137$$uUC, Irvine 002112269 700__ $$aScarcella, Mark$$iINSPIRE-00287125$$uSydney U. 002112269 700__ $$aScarfone, Valerio$$iINSPIRE-00356284$$uINFN, Cosenza$$uCalabria U. 002112269 700__ $$aSchaarschmidt, Jana$$iINSPIRE-00223142$$uWeizmann Inst. 002112269 700__ $$aSchacht, Peter$$iINSPIRE-00223156$$uMunich, Max Planck Inst. 002112269 700__ $$aSchaefer, Douglas$$iINSPIRE-00332120$$uCERN 002112269 700__ $$aSchaefer, Ralph$$iINSPIRE-00362142$$uDESY 002112269 700__ $$aSchaeffer, Jan$$iINSPIRE-00354291$$uMainz U. 002112269 700__ $$aSchaepe, Steffen$$iINSPIRE-00237394$$uBonn U. 002112269 700__ $$aSchaetzel, Sebastian$$iINSPIRE-00217959$$uHeidelberg U. 002112269 700__ $$aSchäfer, Uli$$iINSPIRE-00146919$$uMainz U. 002112269 700__ $$aSchaffer, Arthur$$iINSPIRE-00223168$$uOrsay, LAL 002112269 700__ $$aSchaile, Dorothee$$iINSPIRE-00300542$$uMunich U. 002112269 700__ $$aSchamberger, R Dean$$iINSPIRE-00123848$$uSUNY, Stony Brook 002112269 700__ $$aScharf, Veit$$iINSPIRE-00223180$$uKirchhoff Inst. 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C$$v76$$y2016 002112269 859__ [email protected] 002112269 8564_ $$s11047988$$uhttp://inspirehep.net/record/1409298/files/scoap3-fulltext.pdf?subformat=pdfa$$xpdfa$$yArticle from SCOAP3 002112269 8564_ $$81171580$$s1605974$$uhttp://cds.cern.ch/record/2112269/files/arXiv:1512.03657.pdf 002112269 8564_ $$81171256$$s1826475$$uhttp://cds.cern.ch/record/2112269/files/BPHY-2012-02.pdf$$yFulltext 002112269 8564_ $$81171256$$s3193049$$uhttp://cds.cern.ch/record/2112269/files/BPHY-2012-02.pdf?subformat=pdfa$$xpdfa 002112269 8564_ $$81171561$$s59990$$uhttp://cds.cern.ch/record/2112269/files/figures_ct_8TeV_JpsiP_xSec.png$$y00006 The differential prompt cross-section times dimuon branching fraction of \jpsi\ (left) and \psiprime\ (right) as a function of $\pt(\mu\mu)$ for each slice of rapidity. The top (bottom) row shows the 7~\TeV\ (8~\TeV) results. For each increasing rapidity slice, an additional scaling factor of 10 is applied to the plotted points for visual clarity. The centre of each bin on the horizontal axis represents the mean of the weighted $\pt$ distribution. The horizontal error bars represent the range of $\pt$ for the bin, and the vertical error bar covers the statistical and systematic uncertainty (with the same multiplicative scaling applied). The NLO NRQCD theory predictions are also shown. 002112269 8564_ $$81171562$$s56239$$uhttp://cds.cern.ch/record/2112269/files/figures_ct_8TeV_Psi2SNP_theoryRatio_lin.png$$y00027 The ratio of the FONLL theoretical predictions to data are presented for the differential non-prompt cross-section of \jpsi\ (left) and \psiprime\ (right) as a function of $\pt(\mu\mu)$ for each rapidity slice. The top (bottom) row shows the 7~\TeV\ (8~\TeV) results. The error on the data is the relative error of each data point, while the error bars on the theory prediction are the relative error of each theory point. 002112269 8564_ $$81171563$$s48951$$uhttp://cds.cern.ch/record/2112269/files/figures_ct_7TeV_NPF_Jpsi.png$$y00012 The non-prompt fraction of \jpsi\ (left) and \psiprime\ (right), as a function of $\pt(\mu\mu)$ for each slice of rapidity. The top (bottom) row shows the 7~\TeV\ (8~\TeV) results. For each increasing rapidity slice, an additional factor of 0.2 is applied to the plotted points for visual clarity. The centre of each bin on the horizontal axis represents the mean of the weighted $\pt$ distribution. The horizontal error bars represent the range of $\pt$ for the bin, and the vertical error bar covers the statistical and systematic uncertainty (with the same multiplicative scaling applied). 002112269 8564_ $$81171564$$s60133$$uhttp://cds.cern.ch/record/2112269/files/figures_c_c_Mass_5_5.png$$y00000 Projections of the fit result over the mass (left) and pseudo-proper decay time (right) distributions for data collected at $7$~\TeV\ for one typical interval. The data are shown with error bars in black, superimposed with the individual components of the fit result projections, where the total prompt and non-prompt components are represented by the dashed and dotted lines, respectively, and the shaded areas show the signal $\psi$ prompt and non-prompt contributions. 002112269 8564_ $$81171565$$s60352$$uhttp://cds.cern.ch/record/2112269/files/figures_ct_7TeV_Psi2SNP_theoryRatio_lin.png$$y00025 The ratio of the FONLL theoretical predictions to data are presented for the differential non-prompt cross-section of \jpsi\ (left) and \psiprime\ (right) as a function of $\pt(\mu\mu)$ for each rapidity slice. The top (bottom) row shows the 7~\TeV\ (8~\TeV) results. The error on the data is the relative error of each data point, while the error bars on the theory prediction are the relative error of each theory point. 002112269 8564_ $$81171566$$s84044$$uhttp://cds.cern.ch/record/2112269/files/figures_c_c_Tau_5_5.png$$y00001 Projections of the fit result over the mass (left) and pseudo-proper decay time (right) distributions for data collected at $7$~\TeV\ for one typical interval. The data are shown with error bars in black, superimposed with the individual components of the fit result projections, where the total prompt and non-prompt components are represented by the dashed and dotted lines, respectively, and the shaded areas show the signal $\psi$ prompt and non-prompt contributions. 002112269 8564_ $$81171567$$s49762$$uhttp://cds.cern.ch/record/2112269/files/figures_ct_8TeV_NPF_Psi.png$$y00015 The non-prompt fraction of \jpsi\ (left) and \psiprime\ (right), as a function of $\pt(\mu\mu)$ for each slice of rapidity. The top (bottom) row shows the 7~\TeV\ (8~\TeV) results. For each increasing rapidity slice, an additional factor of 0.2 is applied to the plotted points for visual clarity. The centre of each bin on the horizontal axis represents the mean of the weighted $\pt$ distribution. The horizontal error bars represent the range of $\pt$ for the bin, and the vertical error bar covers the statistical and systematic uncertainty (with the same multiplicative scaling applied). 002112269 8564_ $$81171568$$s45906$$uhttp://cds.cern.ch/record/2112269/files/figures_ct_7TeV_NP_Ratio.png$$y00017 The ratio of \psiprime\ to \jpsi\ production times dimuon branching fraction for prompt (left) and non-prompt (right) processes as a function of $\pt(\mu\mu)$ for each of the slices of rapidity. For each increasing rapidity slice, an additional factor of 0.1 is applied to the plotted points for visual clarity. The top (bottom) row shows the 7~\TeV\ (8~\TeV) results. The centre of each bin on the horizontal axis represents the mean of the weighted $\pt$ distribution. The horizontal error bars represent the range of $\pt$ for the bin, and the vertical error bar covers the statistical and systematic uncertainty. 002112269 8564_ $$81171569$$s48795$$uhttp://cds.cern.ch/record/2112269/files/figures_ct_8TeV_NPF_Jpsi.png$$y00014 The non-prompt fraction of \jpsi\ (left) and \psiprime\ (right), as a function of $\pt(\mu\mu)$ for each slice of rapidity. The top (bottom) row shows the 7~\TeV\ (8~\TeV) results. For each increasing rapidity slice, an additional factor of 0.2 is applied to the plotted points for visual clarity. The centre of each bin on the horizontal axis represents the mean of the weighted $\pt$ distribution. The horizontal error bars represent the range of $\pt$ for the bin, and the vertical error bar covers the statistical and systematic uncertainty (with the same multiplicative scaling applied). 002112269 8564_ $$81171570$$s56180$$uhttp://cds.cern.ch/record/2112269/files/figures_ct_8TeV_JpsiNP_theoryRatio_lin.png$$y00026 The ratio of the FONLL theoretical predictions to data are presented for the differential non-prompt cross-section of \jpsi\ (left) and \psiprime\ (right) as a function of $\pt(\mu\mu)$ for each rapidity slice. The top (bottom) row shows the 7~\TeV\ (8~\TeV) results. The error on the data is the relative error of each data point, while the error bars on the theory prediction are the relative error of each theory point. 002112269 8564_ $$81171571$$s59893$$uhttp://cds.cern.ch/record/2112269/files/figures_ct_7TeV_JpsiP_theoryRatio_lin.png$$y00020 The ratios of the NRQCD theoretical predictions to data are presented for the differential prompt cross-section of \jpsi\ (left) and \psiprime\ (right) as a function of $\pt(\mu\mu)$ for each rapidity slice. The top (bottom) row shows the 7~\TeV\ (8~\TeV) results. The error on the data is the relative error of each data point, while the error bars on the theory prediction are the relative error of each theory point. 002112269 8564_ $$81171572$$s54448$$uhttp://cds.cern.ch/record/2112269/files/figures_ct_7TeV_NPF_Psi.png$$y00013 The non-prompt fraction of \jpsi\ (left) and \psiprime\ (right), as a function of $\pt(\mu\mu)$ for each slice of rapidity. The top (bottom) row shows the 7~\TeV\ (8~\TeV) results. For each increasing rapidity slice, an additional factor of 0.2 is applied to the plotted points for visual clarity. The centre of each bin on the horizontal axis represents the mean of the weighted $\pt$ distribution. The horizontal error bars represent the range of $\pt$ for the bin, and the vertical error bar covers the statistical and systematic uncertainty (with the same multiplicative scaling applied). 002112269 8564_ $$81171573$$s63521$$uhttp://cds.cern.ch/record/2112269/files/figures_rt_th_xSecP_J.png$$y00028 The ratio of the 8~\TeV\ and 7~\TeV\ differential cross-sections are presented for prompt~(top) and non-prompt~(bottom) $\jpsi$~(left) and $\psiprime$~(right) for both data~(red points with error bars) and theoretical predictions~(green points). The theoretical predictions used are NRQCD for prompt and FONLL for non-prompt production. The uncertainty on the data ratio does not account for possible correlations between 7 and 8 \TeV\ data, and no uncertainty is shown for the ratio of theory predictions. 002112269 8564_ $$81171574$$s71710$$uhttp://cds.cern.ch/record/2112269/files/figures_rt_th_xSecNP_P.png$$y00031 The ratio of the 8~\TeV\ and 7~\TeV\ differential cross-sections are presented for prompt~(top) and non-prompt~(bottom) $\jpsi$~(left) and $\psiprime$~(right) for both data~(red points with error bars) and theoretical predictions~(green points). The theoretical predictions used are NRQCD for prompt and FONLL for non-prompt production. The uncertainty on the data ratio does not account for possible correlations between 7 and 8 \TeV\ data, and no uncertainty is shown for the ratio of theory predictions. 002112269 8564_ $$81171575$$s53530$$uhttp://cds.cern.ch/record/2112269/files/figures_ct_7TeV_Psi2SNP_xSec.png$$y00009 The differential non-prompt cross-section times dimuon branching fraction of \jpsi\ (left) and \psiprime\ (right) as a function of $\pt(\mu\mu)$ for each slice of rapidity. The top (bottom) row shows the 7~\TeV\ (8~\TeV) results. For each increasing rapidity slice, an additional scaling factor of 10 is applied to the plotted points for visual clarity. The centre of each bin on the horizontal axis represents the mean of the weighted $\pt$ distribution. The horizontal error bars represent the range of $\pt$ for the bin, and the vertical error bar covers the statistical and systematic uncertainty (with the same multiplicative scaling applied). The FONLL theory predictions are also shown. 002112269 8564_ $$81171576$$s44373$$uhttp://cds.cern.ch/record/2112269/files/figures_ct_8TeV_NP_Ratio.png$$y00019 The ratio of \psiprime\ to \jpsi\ production times dimuon branching fraction for prompt (left) and non-prompt (right) processes as a function of $\pt(\mu\mu)$ for each of the slices of rapidity. For each increasing rapidity slice, an additional factor of 0.1 is applied to the plotted points for visual clarity. The top (bottom) row shows the 7~\TeV\ (8~\TeV) results. The centre of each bin on the horizontal axis represents the mean of the weighted $\pt$ distribution. The horizontal error bars represent the range of $\pt$ for the bin, and the vertical error bar covers the statistical and systematic uncertainty. 002112269 8564_ $$81171577$$s58387$$uhttp://cds.cern.ch/record/2112269/files/figures_ct_8TeV_Psi2SP_theoryRatio_lin.png$$y00023 The ratios of the NRQCD theoretical predictions to data are presented for the differential prompt cross-section of \jpsi\ (left) and \psiprime\ (right) as a function of $\pt(\mu\mu)$ for each rapidity slice. The top (bottom) row shows the 7~\TeV\ (8~\TeV) results. The error on the data is the relative error of each data point, while the error bars on the theory prediction are the relative error of each theory point. 002112269 8564_ $$81171578$$s56340$$uhttp://cds.cern.ch/record/2112269/files/figures_ct_8TeV_JpsiP_theoryRatio_lin.png$$y00022 The ratios of the NRQCD theoretical predictions to data are presented for the differential prompt cross-section of \jpsi\ (left) and \psiprime\ (right) as a function of $\pt(\mu\mu)$ for each rapidity slice. The top (bottom) row shows the 7~\TeV\ (8~\TeV) results. The error on the data is the relative error of each data point, while the error bars on the theory prediction are the relative error of each theory point. 002112269 8564_ $$81171579$$s59228$$uhttp://cds.cern.ch/record/2112269/files/figures_ct_8TeV_Psi2SNP_xSec.png$$y00011 The differential non-prompt cross-section times dimuon branching fraction of \jpsi\ (left) and \psiprime\ (right) as a function of $\pt(\mu\mu)$ for each slice of rapidity. The top (bottom) row shows the 7~\TeV\ (8~\TeV) results. For each increasing rapidity slice, an additional scaling factor of 10 is applied to the plotted points for visual clarity. The centre of each bin on the horizontal axis represents the mean of the weighted $\pt$ distribution. The horizontal error bars represent the range of $\pt$ for the bin, and the vertical error bar covers the statistical and systematic uncertainty (with the same multiplicative scaling applied). The FONLL theory predictions are also shown. 002112269 8564_ $$81171581$$s56608$$uhttp://cds.cern.ch/record/2112269/files/figures_c_8TeV_c_Mass_23_0.png$$y00002 Projections of the fit result over the mass (left) and pseudo-proper decay time (right) distributions for data collected at $8$~\TeV\ for one high-$\pt$ interval. The data are shown with error bars in black, superimposed with the individual components of the fit result projections, where the total prompt and non-prompt components are represented by the dashed and dotted lines, respectively, and the shaded areas show the signal $\psi$ prompt and non-prompt contributions. 002112269 8564_ $$81171582$$s63243$$uhttp://cds.cern.ch/record/2112269/files/figures_rt_th_xSecNP_J.png$$y00030 The ratio of the 8~\TeV\ and 7~\TeV\ differential cross-sections are presented for prompt~(top) and non-prompt~(bottom) $\jpsi$~(left) and $\psiprime$~(right) for both data~(red points with error bars) and theoretical predictions~(green points). The theoretical predictions used are NRQCD for prompt and FONLL for non-prompt production. The uncertainty on the data ratio does not account for possible correlations between 7 and 8 \TeV\ data, and no uncertainty is shown for the ratio of theory predictions. 002112269 8564_ $$81171583$$s44531$$uhttp://cds.cern.ch/record/2112269/files/figures_ct_8TeV_P_Ratio.png$$y00018 The ratio of \psiprime\ to \jpsi\ production times dimuon branching fraction for prompt (left) and non-prompt (right) processes as a function of $\pt(\mu\mu)$ for each of the slices of rapidity. For each increasing rapidity slice, an additional factor of 0.1 is applied to the plotted points for visual clarity. The top (bottom) row shows the 7~\TeV\ (8~\TeV) results. The centre of each bin on the horizontal axis represents the mean of the weighted $\pt$ distribution. The horizontal error bars represent the range of $\pt$ for the bin, and the vertical error bar covers the statistical and systematic uncertainty. 002112269 8564_ $$81171584$$s56504$$uhttp://cds.cern.ch/record/2112269/files/figures_ct_7TeV_JpsiP_xSec.png$$y00004 The differential prompt cross-section times dimuon branching fraction of \jpsi\ (left) and \psiprime\ (right) as a function of $\pt(\mu\mu)$ for each slice of rapidity. The top (bottom) row shows the 7~\TeV\ (8~\TeV) results. For each increasing rapidity slice, an additional scaling factor of 10 is applied to the plotted points for visual clarity. The centre of each bin on the horizontal axis represents the mean of the weighted $\pt$ distribution. The horizontal error bars represent the range of $\pt$ for the bin, and the vertical error bar covers the statistical and systematic uncertainty (with the same multiplicative scaling applied). The NLO NRQCD theory predictions are also shown. 002112269 8564_ $$81171585$$s53904$$uhttp://cds.cern.ch/record/2112269/files/figures_ct_7TeV_JpsiNP_xSec.png$$y00008 The differential non-prompt cross-section times dimuon branching fraction of \jpsi\ (left) and \psiprime\ (right) as a function of $\pt(\mu\mu)$ for each slice of rapidity. The top (bottom) row shows the 7~\TeV\ (8~\TeV) results. For each increasing rapidity slice, an additional scaling factor of 10 is applied to the plotted points for visual clarity. The centre of each bin on the horizontal axis represents the mean of the weighted $\pt$ distribution. The horizontal error bars represent the range of $\pt$ for the bin, and the vertical error bar covers the statistical and systematic uncertainty (with the same multiplicative scaling applied). The FONLL theory predictions are also shown. 002112269 8564_ $$81171586$$s59619$$uhttp://cds.cern.ch/record/2112269/files/figures_ct_7TeV_JpsiNP_theoryRatio_lin.png$$y00024 The ratio of the FONLL theoretical predictions to data are presented for the differential non-prompt cross-section of \jpsi\ (left) and \psiprime\ (right) as a function of $\pt(\mu\mu)$ for each rapidity slice. The top (bottom) row shows the 7~\TeV\ (8~\TeV) results. The error on the data is the relative error of each data point, while the error bars on the theory prediction are the relative error of each theory point. 002112269 8564_ $$81171587$$s45117$$uhttp://cds.cern.ch/record/2112269/files/figures_ct_7TeV_P_Ratio.png$$y00016 The ratio of \psiprime\ to \jpsi\ production times dimuon branching fraction for prompt (left) and non-prompt (right) processes as a function of $\pt(\mu\mu)$ for each of the slices of rapidity. For each increasing rapidity slice, an additional factor of 0.1 is applied to the plotted points for visual clarity. The top (bottom) row shows the 7~\TeV\ (8~\TeV) results. The centre of each bin on the horizontal axis represents the mean of the weighted $\pt$ distribution. The horizontal error bars represent the range of $\pt$ for the bin, and the vertical error bar covers the statistical and systematic uncertainty. 002112269 8564_ $$81171588$$s21393$$uhttp://cds.cern.ch/record/2112269/files/figures_ct_8TeV_JpsiNP_xSec.png$$y00010 The differential non-prompt cross-section times dimuon branching fraction of \jpsi\ (left) and \psiprime\ (right) as a function of $\pt(\mu\mu)$ for each slice of rapidity. The top (bottom) row shows the 7~\TeV\ (8~\TeV) results. For each increasing rapidity slice, an additional scaling factor of 10 is applied to the plotted points for visual clarity. The centre of each bin on the horizontal axis represents the mean of the weighted $\pt$ distribution. The horizontal error bars represent the range of $\pt$ for the bin, and the vertical error bar covers the statistical and systematic uncertainty (with the same multiplicative scaling applied). The FONLL theory predictions are also shown. 002112269 8564_ $$81171589$$s71643$$uhttp://cds.cern.ch/record/2112269/files/figures_rt_th_xSecP_P.png$$y00029 The ratio of the 8~\TeV\ and 7~\TeV\ differential cross-sections are presented for prompt~(top) and non-prompt~(bottom) $\jpsi$~(left) and $\psiprime$~(right) for both data~(red points with error bars) and theoretical predictions~(green points). The theoretical predictions used are NRQCD for prompt and FONLL for non-prompt production. The uncertainty on the data ratio does not account for possible correlations between 7 and 8 \TeV\ data, and no uncertainty is shown for the ratio of theory predictions. 002112269 8564_ $$81171590$$s62052$$uhttp://cds.cern.ch/record/2112269/files/figures_ct_8TeV_Psi2SP_xSec.png$$y00007 The differential prompt cross-section times dimuon branching fraction of \jpsi\ (left) and \psiprime\ (right) as a function of $\pt(\mu\mu)$ for each slice of rapidity. The top (bottom) row shows the 7~\TeV\ (8~\TeV) results. For each increasing rapidity slice, an additional scaling factor of 10 is applied to the plotted points for visual clarity. The centre of each bin on the horizontal axis represents the mean of the weighted $\pt$ distribution. The horizontal error bars represent the range of $\pt$ for the bin, and the vertical error bar covers the statistical and systematic uncertainty (with the same multiplicative scaling applied). The NLO NRQCD theory predictions are also shown. 002112269 8564_ $$81171591$$s55967$$uhttp://cds.cern.ch/record/2112269/files/figures_ct_7TeV_Psi2SP_xSec.png$$y00005 The differential prompt cross-section times dimuon branching fraction of \jpsi\ (left) and \psiprime\ (right) as a function of $\pt(\mu\mu)$ for each slice of rapidity. The top (bottom) row shows the 7~\TeV\ (8~\TeV) results. For each increasing rapidity slice, an additional scaling factor of 10 is applied to the plotted points for visual clarity. The centre of each bin on the horizontal axis represents the mean of the weighted $\pt$ distribution. The horizontal error bars represent the range of $\pt$ for the bin, and the vertical error bar covers the statistical and systematic uncertainty (with the same multiplicative scaling applied). The NLO NRQCD theory predictions are also shown. 002112269 8564_ $$81171592$$s55053$$uhttp://cds.cern.ch/record/2112269/files/figures_c_8TeV_c_Tau_23_0.png$$y00003 Projections of the fit result over the mass (left) and pseudo-proper decay time (right) distributions for data collected at $8$~\TeV\ for one high-$\pt$ interval. The data are shown with error bars in black, superimposed with the individual components of the fit result projections, where the total prompt and non-prompt components are represented by the dashed and dotted lines, respectively, and the shaded areas show the signal $\psi$ prompt and non-prompt contributions. 002112269 8564_ $$81171593$$s62409$$uhttp://cds.cern.ch/record/2112269/files/figures_ct_7TeV_Psi2SP_theoryRatio_lin.png$$y00021 The ratios of the NRQCD theoretical predictions to data are presented for the differential prompt cross-section of \jpsi\ (left) and \psiprime\ (right) as a function of $\pt(\mu\mu)$ for each rapidity slice. The top (bottom) row shows the 7~\TeV\ (8~\TeV) results. The error on the data is the relative error of each data point, while the error bars on the theory prediction are the relative error of each theory point. 002112269 8564_ $$81244389$$s11047988$$uhttp://cds.cern.ch/record/2112269/files/epjc-76-283.pdf$$ySpringer Open Access article 002112269 8564_ $$81244389$$s15103302$$uhttp://cds.cern.ch/record/2112269/files/epjc-76-283.pdf?subformat=pdfa$$xpdfa$$ySpringer Open Access article 002112269 8564_ $$81373901$$s11047988$$uhttp://cds.cern.ch/record/2112269/files/scoap3-fulltext.pdf$$yArticle from SCOAP3 002112269 8564_ $$82333980$$s11047988$$uhttp://cds.cern.ch/record/2112269/files/scoap.pdf$$yArticle from SCOAP3 002112269 916__ $$sn$$w201549 002112269 925__ $$b24 Dec 2015 002112269 960__ $$a13 002112269 980__ $$aARTICLE 002112269 980__ $$aATLAS_Papers