SISTEMA DE BIBLIOTECAS DA UNICAMP
REPOSITÓRIO DA PRODUÇÃO CIENTIFICA E INTELECTUAL DA UNICAMP
Versão do arquivo anexado / Version of attached file:
Versão do Editor / Published Version
Mais informações no site da editora / Further information on publisher's website:
https://www.sciencedirect.com/science/article/pii/S037026931600143X
DOI: 10.1016/j.physletb.2016.02.047
Direitos autorais / Publisher's copyright statement:
©2016 by Elsevier. All rights reserved.
DIRETORIA DE TRATAMENTO DA INFORMAÇÃO Cidade Universitária Zeferino Vaz Barão Geraldo
CEP 13083-970 – Campinas SP Fone: (19) 3521-6493 http://www.repositorio.unicamp.br
Contents lists available atScienceDirect
Physics
Letters
B
www.elsevier.com/locate/physletb
Measurement
of
the
ratio
B
(
B
0s→
J
/ψ
f
0(
980
))/
B
(
B
0s→
J
/ψφ (
1020
))
in
pp
collisions
at
√
s
=
7 TeV
.CMSCollaboration CERN,Switzerland a r t i c l e i n f o a b s t ra c t Articlehistory: Received24January2015Receivedinrevisedform6January2016 Accepted23February2016
Availableonline27February2016 Editor:M.Doser
AmeasurementoftheratioofthebranchingfractionsoftheB0
smesontoJ/ψf0(980)andtoJ/ψφ (1020) is presented.TheJ/ψ,f0(980),and φ(1020) areobservedthroughtheirdecaystoμ+μ−,π+π−,and K+K−,respectively. The f0 and the φ are identified byrequiring |Mπ+π−−974 MeV|<50 MeV and
|MK+K−−1020 MeV|<10 MeV. Theanalysis is basedonadata sampleof ppcollisions ata centre-of-mass energyof7 TeV,collectedbytheCMS experimentattheLHC, correspondingtoanintegrated luminosityof5.3 fb−1.Themeasuredratiois B(B0
s→J/ψf0)B(f0→π+π−)
B(B0
s→J/ψφ)B(φ→K+K−) =0.140±0.008(stat)±0.023(syst), wherethefirstuncertaintyisstatisticalandthesecondissystematic.
©2016CERNforthebenefitoftheCMSCollaboration.PublishedbyElsevierB.V.Thisisanopenaccess articleundertheCCBYlicense(http://creativecommons.org/licenses/by/4.0/).FundedbySCOAP3.
1. Introduction
SincetheobservationofthedecayB0
s→J/ψπ+π−withJ/ψ→
μ+μ−, andthe π+π− massspectrum indicating a large f0(980) component[1],thischannelhasbeenregardedwithgreatinterest inheavy-flavor physics.Moredetailedstudiesofthe π+π−mass spectrumhaveshownthe π+π− systemto bealmostentirelyCP odd[2,3]. Thisopensup thepossibilityofdirectly measuringthe lifetimeoftheCP-oddpartoftheB0s meson[4,5].Inaddition,the B0
s→J/ψπ+π− decayhasbeenusedforthemeasurementofthe CP-violating phase φs [6,7], making an important contributionto
the world-average value of φs [8–13]. The phase φs is predicted
tobe smallinthe standardmodel[14],making itsdetermination interesting becauseof thelarge enhancements that can be intro-ducedbynewphysics[15,16].Inwhatfollows,wewillrefertothe f0(980)asf0 andtheφ (1020)asφ.
ThisLetterpresentsthemeasurementoftheratio Rf0/φ ofthe
branching fractions B(B0s →J/ψf0)B(f0→π+π−) and B(B0s → J/ψφ)B(φ →K+K−), where in both cases the J/ψ is detected throughitsdecayto μ+μ−.Thef0andtheφareidentifiedby re-quiring|Mπ+π−−974 MeV|<50 MeV and|MK+K−−1020 MeV|< 10 MeV.TheappearanceofB0s→J/ψf0 decayswasfirstdiscussed in[17]withatheoreticalestimatefor Rf0/φ ofapproximately0.2,
whichisconsistentwithresultsfromseveralexperiments[2,4,18, 19]. Detailed studies of the π+π− mass spectrum of the B0
s →
J/ψπ+π− decayin0.3<Mπ+π−<2.5 GeV[2,3]revealthisfinal E-mailaddress:cms-publication-committee-chair@cern.ch.
statetohavecontributionsfromseveralresonancesinMπ+π−,and thef0 componenttorangefrom65.0%to94.5%.However, accord-ingtothesameresults,thecontaminationsfromotherresonances in|Mπ+π−−974 MeV|<50 MeV areseveralordersofmagnitude lower thanthef0 component,includingthenon-resonantS-wave. Based on this, the measurement of Rf0/φ is performedassuming
thattheselectedregionofMπ+π− isdominatedbyB0
s→J/ψf0 de-caysandneglectingotherresonances.Systematicuncertainties are assignedto themeasurementowing totheseassumptions,taking into account the uncertainty in the f0 componentandthe inter-ferences withother resonancesin the selected masswindow for Mπ+π−.
Experimentally,theratio Rf0/φisgivenby
Rf0/φ= B(B0s →J/ψf0)B(f0→π+π−) B(B0s→J/ψφ)B(φ→K+K−) =N f0 obs Nφobs φ/f0 reco, (1) whereNf0 obsandN φ
obsaretheobservedyieldsofB0s→J/ψ(μ+μ−)f0 withf0→π+π−andB0s→J/ψ(μ+μ−)φwithφ→K+K−decays, respectively, and φ/f0
reco istheratioofthedetectionefficienciesfor theB0s decaymodewithaφtothedecaymodewithaf0. Uncer-taintiesinthebquarkproductioncrosssectioncancelintheratio, asdothosefromtheJ/ψ→μ+μ−branchingfractionandthe in-tegrated luminosity.Giventhesimilar topologies ofthe twofinal states, systematic uncertainties related to the tracking efficiency andthemuonidentificationalsocancelintheratio.
http://dx.doi.org/10.1016/j.physletb.2016.02.047
0370-2693/©2016CERNforthebenefitoftheCMSCollaboration.PublishedbyElsevierB.V.ThisisanopenaccessarticleundertheCCBYlicense (http://creativecommons.org/licenses/by/4.0/).FundedbySCOAP3.
2. TheCMSdetector
ThecentralfeatureoftheCMSapparatusisasuperconducting solenoid of 6 m internal diameter. Within the 3.8 T field vol-umeare asilicon pixelandstrip tracker, alead tungstatecrystal electromagnetic calorimeter, and a brass and scintillator hadron calorimeter,each composed ofa barrelandtwo endcapsections. Muonsaremeasuredinthepseudorapidityrange|η|<2.4 in gas-ionization detectors embedded in the steelflux-return yoke out-sidethe solenoid,which aremadeusingthree technologies:drift tubes, cathode strip chambers, and resistive-plate chambers. Ex-tensive forward calorimetry complements the coverage provided bythebarrelandendcapdetectors.Themainsubdetectorsusedin thisanalysisarethesilicontrackerandthemuonsystems.
Thesilicontrackermeasureschargedparticleswithinthe pseu-dorapidity range|η|<2.5 and consistsof 1440silicon pixel and 15 148silicon strip detectormodules. Matching muons to tracks measuredinthesilicontrackerresultsinarelativetransverse mo-mentumresolutionformuonswith20<pT<100 GeV of1.3–2.0% inthe barrel and better than 6% in the endcaps. The pT resolu-tion in the barrel is better than 10% for muons with pT up to 1 TeV[20].
ThefirstleveloftheCMStriggersystem, composedofcustom hardware processors,uses informationfrom thecalorimeters and muon detectors to select the most interesting events in a fixed timeintervaloflessthan4 μs.Thehigh-leveltrigger(HLT) proces-sorfarmfurtherdecreasestheeventratetolessthan1 kHz,before datastorage.
AmoredetaileddescriptionoftheCMSdetector,togetherwith adefinitionofthecoordinatesystemusedandtherelevant kine-maticvariables,canbefoundinRef.[21].
3. Eventselection
The data sample used for this measurement was collected in 2011by the CMSexperimentat the CERNLHC in proton–proton collisionsatacentre-of-massenergyof7 TeVandcorrespondsto anintegratedluminosityof5.3 fb−1.
The search for B0s →J/ψf0 decays is performed in events withtwo muon candidatesselectedby thedimuon triggeratthe HLT, requiring the muon pair to originate froma displaced ver-tex.The dimuon candidates are further required to complywith Lxy/σxy>3,where Lxy isthemagnitudeofthevector Lxy,which
liesinaplanetransversetothebeamaxisandpointsfromthe in-teraction point to the dimuon vertex, and σxy is its uncertainty;
cosαJ/ψ >0.9, where αJ/ψ is the angle between the direction
of the dimuon transverse momentum and Lxy; pT>4 GeV and
|η|<2.2 for each muon candidate; pT>7 GeV for the dimuon; thedistanceofclosestapproach ofeach muontrackwithrespect totheothermuontrack<0.5 cm.
ReconstructionoftheB0
s→J/ψf0decaysbeginswiththesearch forJ/ψcandidatesbycombiningtwomuonsofoppositechargeto formavertexwitha fitprobability >0.5% andaninvariant mass (MJ/ψ) within |MJ/ψ−3097.6 MeV|<150 MeV. To search for f0 candidates,twotracksofoppositechargeassumedtobepionsare constrainedtoavertexwithaprobability>5%.Onepioncandidate must have pT>1 GeV and the other pT>2.5 GeV. In addition, the f0 candidate must have pT>3.5 GeV and Mf0 in the range
|Mf0−974 MeV|<50 MeV.The974 MeVisthemeasuredmassof
f0 signal in datamodeled by a Breit–Wigner function.This value isconsistent withthe f0 massfromthe Particle Data Group [22] andthe LHCb measurement [1]. Finally, a vertexis formed with the J/ψ and f0 candidates,constraining thedimuon mass to the nominalJ/ψ mass [22]. The Bs0→J/ψf0 candidates are required tohavea vertexprobability >10%, pT>13 GeV, cosαB0
s >0.994,
Fig. 1. Invariantmass distributionofthe B0
s→J/ψ(μ+μ−)f0(π+π−) candidates
(filledcircles).Thesignalismodeled asaGaussian(dot-dashedline),the combina-torialbackgroundasafirst-orderpolynomialfunction(dashed–double-dottedline), andthepeakingbackgroundbyaGaussian(dottedline).Theresultofthetotalfit isshownwiththesolidline.Thebottomplotshowsthepull,whichisthedeviation ofthedatafromthefitdividedbytheuncertaintyinthedata.
where αB0
s is the angle between the direction of the B
0 s trans-verse momentum andthe vector Lxy, anda proper decaylength
>100 μm.Theproperdecaylengthisdefinedas(Lxy· pTMB/p2T), where pT is the transverse momentum of the B0s candidate and MB is theworld-averageB0s mass[22].Inthe caseofmultipleB0s candidatesperevent,theonewithsmallestB0
s vertexfit χ2 is se-lected.The selectioncriteriafortheB0
s candidatesareestablished by maximizing S/√S+B, where S is the signal yield obtained fromMonteCarlo(MC) simulationandB isthe backgroundyield takenfromsidebandregions,definedasthenumberofeventswith a μ+μ−π+π− invariant mass in the range 5.27 to 5.30 GeV or 5.43 to5.46 GeV.
The same procedure and selection criteria are applied to the reconstruction of the normalization channel B0
s →J/ψφ, except that the invariant massrequirement |Mφ−1020 MeV|<10 MeV
istighterthanthatforthef0.
4. Results
The signal yields of both decay channels are extracted using unbinned maximum-likelihoodfits ofthe massdistributions. The invariant mass distribution of the J/ψ(μ+μ−)f0(π+π−) candi-dates isshownin Fig. 1.It isfit witha superpositionofa Gaus-sian function representing the signal, a polynomial function to account for the combinatorial background, andanother Gaussian function for any possible peaking background. The latter mod-els resonant structures that could appear in the left sideband of the J/ψ(μ+μ−)f0(π+π−) signal mass owing to the misidentifi-cation of a kaon as a pion coming from decays such as B0→ J/ψK∗(892)(K+π−)andB0s→J/ψK+K−,asexamples.Inaddition, B+→J/ψK+(π+) decays can be a source of background when combined with an extra background pion candidate. When al-lowing all parameters to float, the fit returns Nf0
obs=873±49 events anda B0
s mass of 5369.1±0.9 MeV, witha resolution of 15.9±0.9 MeV, where the uncertainties are statistical only. The measured valuesofthe B0s mass anditsresolution areconsistent withtheMCsimulation.
Fig. 2. Invariant mass distribution ofthe B0
s→J/ψ(μ+μ−)φ(K+K−)candidates
(blackfilledcircles).ThesignalmodelisadoubleGaussian(dot-dashedline),while the combinatorial backgroundmodelis aconstantfunction (dash-double-dotted line).Thetotalfitisrepresentedbythesolidline.Thebottomplotshowsthe devi-ationofthedatatothefitdividedbythestatisticaluncertaintyinthedata.
The J/ψ(μ+μ−)φ (K+K−) invariant mass distribution is mod-eled bytwoGaussianfunctionsforthesignalandaconstant func-tion for the combinatorial background. A signal yield of Nφobs= 8377±107 eventsisobtained,withaBs0massof5366.8±0.2 MeV andaresolutionof17.1±0.1 MeV,whichareconsistentwiththe MC simulation. The corresponding invariant mass distribution is presentedinFig. 2.
UsingtheMCsimulation,thedetectionefficienciesforthetwo processesarecalculatedastheratioofthereconstructedand gen-eratedyields.TheB0
s mesonproductionissimulatedusing pythia 6.4.24 [23] and its decays simulated with evtgen [24]. The B0 s mass and lifetime are set to 5369.6 MeV and 438 μm in the simulation. The decay model used for the B0s →J/ψf0 decay is a phase-space model reweighted to reflect the spin-1 structure of the J/ψ→μ+μ− decay. The corresponding models for the B0
s→J/ψφdecayare:apseudoscalar–vector–vectorwithCP viola-tion[25,26]fortheB0
s decay,withparameters[24] A||2=0.24,
A02=0.6,A⊥2=0.16, φ||=2.5, φ0=0, andφ⊥= −0.17;a vector–lepton–lepton model with radiation (photos) [27] forthe J/ψ→μ+μ−decay;andavector–scalar–scalarmodel[24]forthe
φ→K+K− decay. Theeventsare processedwitha Geant4-based detectorsimulation [28] and the same reconstruction algorithms usedondata.InordertovalidatetheMCsimulationsamples, rel-evant kinematicandgeometric variablesof bothsimulated decay channelsarecomparedwiththedataafterbackgroundsubtraction andfound to be inagreement. Forexample,Fig. 3 comparesthe pT and invariant mass distributions of the f0(π+π−) candidates forbackground-subtracted dataandMC simulation. The f0 width was setto 50 MeVin theMC simulation.This isconsistent with what isobserved in ourdata asshown inthe Fig. 3.b. The ratio ofthedetectionefficienciesforthetwo B0s decaysiscalculatedto be φ/f0
reco =1.344±0.095, wherethe uncertaintyreflects the lim-itedsize ofsimulatedsamples.Using thecorresponding valuesof Nf0
obs,N
φ
obs,and
φ/f0
reco inEq.(1),wemeasure Rf0/φ=0.140±0.008,
wheretheuncertaintyisstatisticalonly.
Thestabilityofthe Rf0/φ measurementisverifiedwithcontrol
checksusingdifferentrunperiods,selectioncriteria,andgeometric acceptances.Tostudypossibleeffectsfromvaryingrunconditions,
Fig. 3. Comparison of normalized MC simulation (triangles) and background-subtracteddata(squared)for(a)thepTand(b)invariantmassdistributionsofthe
f0(π+π−)candidates.
thevalueofRf0/φ isdeterminedfortwosubsamples,foundby
di-vidingthedataintotwo.Theratioisalsomeasuredafterchanging theselectioncriteriafortheproperdecaylengthandpT oftheB0s candidates andthe pT of theleading andsubleading pion candi-dates,andbyusingdifferentazimuthalangleand ηrequirements forthemuons.Noneofthesecross-checksrevealedanystatistically significantbias.
5. Systematicuncertainties
PotentialsystematicuncertaintiesinthemeasurementofRf0/φ
come from sources such as the B0
s signal yield extraction proce-dure,therelative efficiencyestimation,andpossiblecontributions to the B0s yields fromother decaysproducing theJ/ψπ+π− and J/ψK+K−finalstates.
Systematicuncertaintiesinthesignal yieldextractionare esti-matedbychangingthemodelingofthesignalandthebackground invariant mass distributionsin thelikelihood fits.Forthe caseof the B0s →J/ψf0 mass distribution thesignal shape is changed to adouble-Gaussianfunctionandthebackgroundtoan exponential function, whilefortheB0
s →J/ψφ massdistributionthesignal is changedtoaGaussianfunctionanditsbackgroundismodeled asa first-orderpolynomialfunction.Thesechangesleadtoamaximum variationof2.1%inRf0/φ.
There areseveralfactorsthat mayaffecttheestimate of φ/f0
reco. While the MC simulation package uses a Breit–Wigner model to simulate the f0→π+π− process, it has been pointed out [2,3]
thataFlattémodelisabetterdescriptionofthisdecay.Toestimate theeffectofthe simulationmodel, theBreit–Wigner modelused in the simulation is compared to a Flatté model in the selected Mπ+π− region.The differenceinthemodels reflectsa systematic errorof5.8%in φ/f0
reco.Thisisquotedasasystematicuncertainty.In addition,intheMCsimulationthef0 widthissetto50 MeV.This valueisvariedby ±10 MeV,resultinginasystematicuncertainty of 8.6% in Rf0/φ. The models used in the MC simulation of the
Bs decaysaresettophase-space[24]insteadofthedefaultdecay
models,leading toa 6.2%systematicuncertaintyin Rf0/φ.Finally,
thestatistical uncertaintyin φ/f0
reco owing to thefinite numberof MC events, which corresponds to 7.1%, is added as a systematic uncertainty.
Asmentionedintheintroduction,detailedstudiesofthe π+π−
massspectrumoftheB0
s→J/ψπ+π−decay[2,3]inamass win-dow of0.3–2.5 GeV, reveal this final state to have contributions fromseveralresonancesinMπ+π−,andthef0componenttorange from65.0to 94.5% in theentire masswindow studied by LHCb. To studythe effects of the interferences and the f0 fraction ob-servedbyLHCbintheestimateof φ/f0
reco,themodelreportedin[3] forthelowestf0fractionandlargestnon-resonantcomponentwas comparedtothe singleBreit–Wigner modelusedinthe MC sim-ulation of the f0→π+π decay. The comparison in the selected Mπ+π− region showsa variation of5.6% in Rf0/φ. Thisis quoted
asasystematicuncertaintycomingfromthissource.Itcanbe ob-servedinthesameLHCbstudythatthecontaminationsfromother resonancesinthemassregion |Mπ+π−−974 MeV|<50 MeV are severalordersofmagnitudelowerthanthef0 component, includ-ingthe non-resonant S-wave. Toestimate thevariation inthe B0s yieldcomingfromthesepossible contributions,thef0 mass win-dowiswidenedfrom50to100 MeVaroundthef0mass,resulting inavariation in Rf0/φ of6.4%that isquoted asa systematic
un-certainty.Forthe B0
s→J/ψK+K− decaychannel,thecontribution oftheS-waveinaφmasswindowsimilartowhatisusedinthis analysishasbeenfoundtobenegligible[29].
Combining these uncertainties in quadrature leads to a total systematicuncertaintyof16.5%.
6. Summary
Usingdatacollected by theCMSexperimentin proton–proton collisionsat√s=7 TeV, corresponding toan integrated luminos-ityof5.3 fb−1,873±49 eventsofB0s→J/ψ(μ+μ−)f0(π+π−)and 8377±107 eventsofB0
s→J/ψ(μ+μ−)φ (K+K−)areobserved.The f0 andφ areidentifiedinthemassranges|Mπ+π−−974 MeV|<
50 MeV and|MK+K−−1020 MeV|<10 MeV,respectively.The ra-tioofthebranchingfractionofB0
s→J/ψ(μ+μ−)f0(π+π−)tothe branchingfractionofB0s→J/ψ(μ+μ−)φ (K+K−),Rf0/φ,isfoundto
be
B(B0s→J/ψf0)B(f0→π+π−)
B(B0s→J/ψ φ)B(φ→K+K−)
=0.140±0.008(stat)±0.023(syst). (2)
Thisresultisconsistentwiththetheoreticalpredictionofabout 0.2 [17] and with previous measurements in different ranges of Mπ+π− [2,4,19].
Acknowledgements
WecongratulateourcolleaguesintheCERNaccelerator depart-ments for the excellent performance of the LHC and thank the technicalandadministrativestaffs atCERN andatother CMS in-stitutes for their contributions to the success of the CMS effort. Inaddition,wegratefullyacknowledgethecomputingcentresand
personneloftheWorldwideLHCComputingGridfordeliveringso effectivelythe computinginfrastructureessential to ouranalyses. Finally, we acknowledge the enduring support for the construc-tion and operation of the LHC and the CMS detector provided by the following funding agencies: BMWFW and FWF (Austria); Fonds DeLa Recherche Scientifique – FNRS and FWO (Belgium); CNPq,CAPES,FAPERJ, andFAPESP(Brazil); MES (Bulgaria);CERN; CAS,MoST,andNSFC(China); COLCIENCIAS(Colombia);MSESand CSF (Croatia); RPF (Cyprus); MoER, ERC IUT and ERDF (Estonia); AcademyofFinland,MEC,andHIP(Finland);CEAandCNRS/IN2P3 (France); BMBF, DFG, and HGF (Germany); GSRT (Greece); OTKA andNIH(Hungary);DAEandDST(India);IPM(Iran);SFI(Ireland); INFN (Italy); MSIPand NRF (Republic of Korea); LAS (Lithuania); MOE and UM(Malaysia); CINVESTAV,CONACYT, SEP, and UASLP-FAI (Mexico); MBIE (New Zealand); PAEC (Pakistan); MSHE and NSC (Poland); FCT (Portugal); JINR(Dubna); MON, RosAtom, RAS andRFBR(Russia);MESTD(Serbia);SEIDIandCPAN(Spain);Swiss Funding Agencies (Switzerland); MST (Taipei); ThEPCenter, IPST, STAR and NSTDA (Thailand); TUBITAK andTAEK (Turkey); NASU andSFFR(Ukraine);STFC(UnitedKingdom);DOEandNSF(USA).
Individuals have received support from the Marie-Curie pro-gramme and the European Research Council and EPLANET (Eu-ropean Union); the Leventis Foundation; the A.P. Sloan Founda-tion; the Alexander von Humboldt Foundation; the Belgian Fed-eral Science Policy Office; the Fonds pour la Formation à la Recherchedansl’Industrieetdansl’Agriculture(FRIA-Belgium);the AgentschapvoorInnovatiedoorWetenschapenTechnologie (IWT-Belgium); theMinistry ofEducation, YouthandSports (MEYS) of theCzechRepublic;theCouncilofScienceandIndustrialResearch, India; the HOMING PLUS programme of Foundation for Polish Science, cofinanced from European Union, Regional Development Fund;the CompagniadiSan Paolo(Torino); the Consorzioper la Fisica (Trieste); MIURproject20108T4XTM (Italy);the Thalisand Aristeia programmes cofinanced by EU-ESF andthe Greek NSRF; andtheNationalPrioritiesResearchProgrambyQatarNational Re-searchFund.
References
[1] LHCb Collaboration, First observation of B0
s →J/ψf0(980) decays, Phys.
Lett.B698(2011)115,http://dx.doi.org/10.1016/j.physletb.2011.03.006,arXiv: 1102.0206.
[2] LHCbCollaboration,AnalysisoftheresonantcomponentsinB0s→J/ψπ+π−,
Phys.Rev.D86(2012)052006,http://dx.doi.org/10.1103/PhysRevD.86.052006, arXiv:1204.5643.
[3] LHCbCollaboration,MeasurementoftheresonantandCP componentsinB0 s→
J/ψπ+π− decays,Phys.Rev.D89(2014) 092006,http://dx.doi.org/10.1103/ PhysRevD.89.092006,arXiv:1402.6248.
[4] CDFCollaboration,T.Aaltonen,etal.,MeasurementofbranchingratioandB0 s
lifetimeinthedecayB0
s→J/ψf0(980)atCDF,Phys.Rev.D84(2011)052012,
http://dx.doi.org/10.1103/PhysRevD.84.052012,arXiv:1106.3682. [5] LHCbCollaboration,MeasurementoftheB0
s effectivelifetimeintheJ/ψf0(980)
final state, Phys. Rev. Lett. 109 (2012) 152002, http://dx.doi.org/10.1103/ PhysRevLett.109.152002,arXiv:1207.0878.
[6] LHCb Collaboration, Measurement of the CP-violating phase φs in B 0 s →
J/ψf0(980), Phys.Lett.B707(2012)497,http://dx.doi.org/10.1016/j.physletb.
2012.01.017,arXiv:1112.3056.
[7] LHCb Collaboration, Measurement of the CP-violating phase φs in B 0 s →
J/ψπ+π− decays,Phys. Lett. B736 (2014)186, http://dx.doi.org/10.1016/j. physletb.2014.06.079,arXiv:1405.4140.
[8] D0Collaboration,V.M.Abazov,etal.,MeasurementofB0
s mixingparameters
fromtheflavor-taggeddecayB0
s→J/ψφ,Phys.Rev.Lett.101(2008)241801,
http://dx.doi.org/10.1103/PhysRevLett.101.241801,arXiv:0802.2255.
[9] CDF Collaboration, T. Aaltonen, et al., First flavor-tagged determination of bounds on mixing-induced CP violation in B0
s→J/ψφ decays, Phys. Rev.
Lett. 100 (2008) 161802, http://dx.doi.org/10.1103/PhysRevLett.100.161802, arXiv:0712.2397.
[10] D0Collaboration,V.M.Abazov,etal.,MeasurementoftheCP-violatingphase
Phys.Rev.D85(2012)032006,http://dx.doi.org/10.1103/PhysRevD.85.032006, arXiv:1109.3166.
[11] LHCbCollaboration, Measurement of the CP-violating phase φs in the
de-cayB0
s→J/ψφ,Phys.Rev.Lett.108(2012)101803,http://dx.doi.org/10.1103/
PhysRevLett.108.101803,arXiv:1112.3183.
[12] ATLASCollaboration,Time-dependentangularanalysisofthedecayB0 s→J/ψφ
and extraction of s and the CP-violating weak phase φs by ATLAS, J.
HighEnergyPhys.12(2012)072,http://dx.doi.org/10.1007/JHEP12(2012)072, arXiv:1208.0572.
[13]CMSCollaboration,MeasurementoftheCP-violatingweakphaseφsandthe
decaywidthdifferencesusingtheBs0→J/ψφ(1020)decaychannelinpp
collisionsat√s=8 TeV,Phys.Lett.B(2015),arXiv:1507.07527,submittedfor publication.
[14] J.Charles,O. Deschamps, S. Descotes-Genon, R. Itoh,H. Lacker, A.Menzel, S. Monteil, V.Niess,J. Ocariz, J. Orloff, S. T’Jampens, V.Tisserand, K. Tra-belsi,Predictionsofselectedflavourobservableswithinthestandard model, Phys.Rev.D84(2011)033005,http://dx.doi.org/10.1103/PhysRevD.84.033005, arXiv:1106.4041.
[15] P. Ball,R.Fleischer, Probingnew physicsthrough Bmixing: status, bench-marksandprospects,Eur.Phys.J.C48(2006)413,http://dx.doi.org/10.1140/ epjc/s10052-006-0034-4,arXiv:hep-ph/0604249.
[16] A.Lenz,UnparticlephysicseffectsinBs–Bs mixing,Phys.Rev.D76(2007)
065006,http://dx.doi.org/10.1103/PhysRevD.76.065006,arXiv:0707.1535. [17] S.Stone,L.Zhang,S-wavesandthemeasurementofCP-violatingphasesinBs
decays,Phys.Rev.D79(2009)074024,http://dx.doi.org/10.1103/PhysRevD.79. 074024,arXiv:0812.2832.
[18] BELLECollaboration,J.Li,etal.,ObservationofB0
s→J/ψf0(980)andevidence
for B0
s→J/ψf0(1370),Phys. Rev.Lett.106(2011)121802,http://dx.doi.org/
10.1103/PhysRevLett.106.121802,arXiv:1102.2759.
[19] D0 Collaboration, V.M.Abazov,et al., Measurementof the relative branch-ingratioofB0
s→J/ψf0(980)toB0s→J/ψφ,Phys.Rev.D85(2012)011103,
http://dx.doi.org/10.1103/PhysRevD.85.011103,arXiv:1110.4272.
[20] CMSCollaboration,PerformanceofCMSmuonreconstructioninppcollision eventsat√s=7 TeV,J.Instrum.7(2012)P10002,http://dx.doi.org/10.1088/ 1748-0221/7/10/P10002,arXiv:1206.4071.
[21] CMSCollaboration,TheCMSexperimentattheCERNLHC,J.Instrum.03(2008) S08004,http://dx.doi.org/10.1088/1748-0221/3/08/S08004.
[22] ParticleDataGroup,J.Beringer,etal.,Reviewofparticlephysics,Phys.Rev.D 86(2012)010001,http://dx.doi.org/10.1103/PhysRevD.86.010001.
[23] T. Sjöstrand, S.Mrenna, P.Skands, PYTHIA6.4 physicsand manual, J.High EnergyPhys.05(2006)026,http://dx.doi.org/10.1088/1126-6708/2006/05/026, arXiv:hep-ph/0603175.
[24] D.Lange,TheEvtGenparticledecaysimulationpackage,Nucl.Instrum. Meth-odsA462(2001)152,http://dx.doi.org/10.1016/S0168-9002(01)00089-4. [25] I. Dunietz, H. Quinn, A. Snyder, W. Toki, H.J. Lipkin, How to extract
CP-violatingasymmetriesfromangularcorrelations,Phys.Rev.D43(1991)2193, http://dx.doi.org/10.1103/PhysRevD.43.2193.
[26] BaBarCollaboration,B.Aubert,etal.,MeasurementoftheB→J/ψK∗(892) de-cayamplitudes,Phys. Rev.Lett.87(2001) 241801,http://dx.doi.org/10.1103/ PhysRevLett.87.241801,hep-ex/0107049.
[27] P.Golonka,Z.Was,PHOTOSMonteCarlo:aprecisiontoolforQEDcorrections in Z andW decays,Eur.Phys. J.C45(2006) 97,http://dx.doi.org/10.1140/ epjc/s2005-02396-4,arXiv:hep-ph/0506026.
[28] GEANT4Collaboration,S.Agostinelli,etal.,Geant4—asimulationtoolkit,Nucl. Instrum.MethodsA506(2003)250,http://dx.doi.org/10.1016/S0168-9002(03) 01368-8.
[29] CDFCollaboration,T.Aaltonen,etal.,Measurementofthebottom-strange me-sonmixingphaseinthefullCDFdataset,Phys.Rev.Lett.109(2012)171802, http://dx.doi.org/10.1103/PhysRevLett.109.171802,arXiv:1208.2967.
CMSCollaboration
V. Khachatryan,A.M. Sirunyan, A. Tumasyan
YerevanPhysicsInstitute,Yerevan,Armenia
W. Adam, T. Bergauer, M. Dragicevic,J. Erö, M. Friedl,R. Frühwirth1,V.M. Ghete, C. Hartl, N. Hörmann, J. Hrubec, M. Jeitler1, W. Kiesenhofer,V. Knünz, M. Krammer1, I. Krätschmer,D. Liko, I. Mikulec, D. Rabady2,B. Rahbaran, H. Rohringer, R. Schöfbeck, J. Strauss, W. Treberer-Treberspurg,
W. Waltenberger, C.-E. Wulz1
InstitutfürHochenergiephysikderOeAW,Wien,Austria
V. Mossolov,N. Shumeiko, J. Suarez Gonzalez
NationalCentreforParticleandHighEnergyPhysics,Minsk,Belarus
S. Alderweireldt, S. Bansal,T. Cornelis, E.A. De Wolf,X. Janssen, A. Knutsson,J. Lauwers, S. Luyckx, S. Ochesanu,R. Rougny, M. Van De Klundert, H. Van Haevermaet,P. Van Mechelen, N. Van Remortel, A. Van Spilbeeck
UniversiteitAntwerpen,Antwerpen,Belgium
F. Blekman,S. Blyweert, J. D’Hondt,N. Daci, N. Heracleous, J. Keaveney,S. Lowette, M. Maes, A. Olbrechts, Q. Python, D. Strom, S. Tavernier,W. Van Doninck, P. Van Mulders, G.P. Van Onsem, I. Villella
VrijeUniversiteitBrussel,Brussel,Belgium
C. Caillol, B. Clerbaux, G. De Lentdecker, D. Dobur, L. Favart, A.P.R. Gay, A. Grebenyuk,A. Léonard, A. Mohammadi, L. Perniè2, A. Randle-conde,T. Reis,T. Seva, L. Thomas, C. Vander Velde, P. Vanlaer, J. Wang, F. Zenoni
UniversitéLibredeBruxelles,Bruxelles,Belgium
V. Adler,K. Beernaert, L. Benucci, A. Cimmino,S. Costantini, S. Crucy, A. Fagot,G. Garcia, J. Mccartin, A.A. Ocampo Rios, D. Poyraz,D. Ryckbosch, S. Salva Diblen, M. Sigamani,N. Strobbe, F. Thyssen, M. Tytgat, E. Yazgan, N. Zaganidis
S. Basegmez, C. Beluffi3, G. Bruno,R. Castello, A. Caudron, L. Ceard, G.G. Da Silveira,C. Delaere, T. du Pree,D. Favart,L. Forthomme, A. Giammanco4,J. Hollar, A. Jafari,P. Jez, M. Komm, V. Lemaitre, C. Nuttens, D. Pagano,L. Perrini, A. Pin, K. Piotrzkowski,A. Popov5,L. Quertenmont, M. Selvaggi, M. Vidal Marono, J.M. Vizan Garcia
UniversitéCatholiquedeLouvain,Louvain-la-Neuve,Belgium
N. Beliy,T. Caebergs, E. Daubie, G.H. Hammad
UniversitédeMons,Mons,Belgium
W.L. Aldá Júnior, G.A. Alves,L. Brito,M. Correa Martins Junior, T. Dos Reis Martins, J. Molina, C. Mora Herrera,M.E. Pol, P. Rebello Teles
CentroBrasileirodePesquisasFisicas,RiodeJaneiro,Brazil
W. Carvalho,J. Chinellato6, A. Custódio, E.M. Da Costa, D. De Jesus Damiao,C. De Oliveira Martins, S. Fonseca De Souza, H. Malbouisson,D. Matos Figueiredo, L. Mundim, H. Nogima,W.L. Prado Da Silva, J. Santaolalla,A. Santoro, A. Sznajder,E.J. Tonelli Manganote6, A. Vilela Pereira
UniversidadedoEstadodoRiodeJaneiro,RiodeJaneiro,Brazil
C.A. Bernardesb, S. Dograa,T.R. Fernandez Perez Tomeia, E.M. Gregoresb, P.G. Mercadanteb, S.F. Novaesa, Sandra S. Padulaa
aUniversidadeEstadualPaulista,SãoPaulo,Brazil bUniversidadeFederaldoABC,SãoPaulo,Brazil
A. Aleksandrov, V. Genchev2, R. Hadjiiska,P. Iaydjiev, A. Marinov, S. Piperov,M. Rodozov, S. Stoykova, G. Sultanov,M. Vutova
InstituteforNuclearResearchandNuclearEnergy,Sofia,Bulgaria
A. Dimitrov,I. Glushkov, L. Litov, B. Pavlov,P. Petkov
UniversityofSofia,Sofia,Bulgaria
J.G. Bian,G.M. Chen, H.S. Chen, M. Chen, T. Cheng,R. Du, C.H. Jiang, R. Plestina7, F. Romeo,J. Tao, Z. Wang
InstituteofHighEnergyPhysics,Beijing,China
C. Asawatangtrakuldee, Y. Ban,S. Liu, Y. Mao,S.J. Qian, D. Wang, Z. Xu,L. Zhang, W. Zou
StateKeyLaboratoryofNuclearPhysicsandTechnology,PekingUniversity,Beijing,China
C. Avila,A. Cabrera, L.F. Chaparro Sierra, C. Florez,J.P. Gomez, B. Gomez Moreno, J.C. Sanabria
UniversidaddeLosAndes,Bogota,Colombia
N. Godinovic, D. Lelas,D. Polic, I. Puljak
UniversityofSplit,FacultyofElectricalEngineering,MechanicalEngineeringandNavalArchitecture,Split,Croatia
Z. Antunovic,M. Kovac
UniversityofSplit,FacultyofScience,Split,Croatia
V. Brigljevic,K. Kadija, J. Luetic,D. Mekterovic, L. Sudic
InstituteRudjerBoskovic,Zagreb,Croatia
A. Attikis, G. Mavromanolakis,J. Mousa, C. Nicolaou, F. Ptochos,P.A. Razis, H. Rykaczewski
M. Bodlak,M. Finger, M. Finger Jr.8
CharlesUniversity,Prague,CzechRepublic
Y. Assran9, A. Ellithi Kamel10,M.A. Mahmoud11, A. Radi12,13
AcademyofScientificResearchandTechnologyoftheArabRepublicofEgypt,EgyptianNetworkofHighEnergyPhysics,Cairo,Egypt
M. Kadastik, M. Murumaa, M. Raidal, A. Tiko
NationalInstituteofChemicalPhysicsandBiophysics,Tallinn,Estonia
P. Eerola, M. Voutilainen
DepartmentofPhysics,UniversityofHelsinki,Helsinki,Finland
J. Härkönen,V. Karimäki, R. Kinnunen, M.J. Kortelainen, T. Lampén, K. Lassila-Perini,S. Lehti, T. Lindén, P. Luukka, T. Mäenpää,T. Peltola, E. Tuominen, J. Tuominiemi,E. Tuovinen, L. Wendland
HelsinkiInstituteofPhysics,Helsinki,Finland
J. Talvitie, T. Tuuva
LappeenrantaUniversityofTechnology,Lappeenranta,Finland
M. Besancon, F. Couderc,M. Dejardin, D. Denegri, B. Fabbro,J.L. Faure, C. Favaro,F. Ferri, S. Ganjour, A. Givernaud, P. Gras, G. Hamel de Monchenault, P. Jarry,E. Locci, J. Malcles,J. Rander, A. Rosowsky, M. Titov
DSM/IRFU,CEA/Saclay,Gif-sur-Yvette,France
S. Baffioni,F. Beaudette, P. Busson, E. Chapon, C. Charlot,T. Dahms, M. Dalchenko, L. Dobrzynski, N. Filipovic, A. Florent,R. Granier de Cassagnac, L. Mastrolorenzo, P. Miné, I.N. Naranjo, M. Nguyen, C. Ochando, G. Ortona,P. Paganini, S. Regnard, R. Salerno, J.B. Sauvan, Y. Sirois, C. Veelken,Y. Yilmaz, A. Zabi
LaboratoireLeprince-Ringuet,EcolePolytechnique,IN2P3-CNRS,Palaiseau,France
J.-L. Agram14, J. Andrea, A. Aubin, D. Bloch,J.-M. Brom, E.C. Chabert,C. Collard, E. Conte14, J.-C. Fontaine14,D. Gelé, U. Goerlach, C. Goetzmann,A.-C. Le Bihan, K. Skovpen, P. Van Hove
InstitutPluridisciplinaireHubertCurien,UniversitédeStrasbourg,UniversitédeHauteAlsaceMulhouse,CNRS/IN2P3,Strasbourg,France
S. Gadrat
CentredeCalculdel’InstitutNationaldePhysiqueNucleaireetdePhysiquedesParticules,CNRS/IN2P3,Villeurbanne,France
S. Beauceron,N. Beaupere, C. Bernet7,G. Boudoul2, E. Bouvier, S. Brochet, C.A. Carrillo Montoya, J. Chasserat, R. Chierici,D. Contardo2,B. Courbon, P. Depasse, H. El Mamouni, J. Fan, J. Fay, S. Gascon, M. Gouzevitch, B. Ille, T. Kurca, M. Lethuillier, L. Mirabito,A.L. Pequegnot, S. Perries, J.D. Ruiz Alvarez, D. Sabes,L. Sgandurra, V. Sordini,M. Vander Donckt, P. Verdier,S. Viret, H. Xiao
UniversitédeLyon,UniversitéClaudeBernardLyon1,CNRS-IN2P3,InstitutdePhysiqueNucléairedeLyon,Villeurbanne,France
Z. Tsamalaidze8
InstituteofHighEnergyPhysicsandInformatization,TbilisiStateUniversity,Tbilisi,Georgia
C. Autermann, S. Beranek,M. Bontenackels, M. Edelhoff,L. Feld, A. Heister, K. Klein,M. Lipinski, A. Ostapchuk, M. Preuten,F. Raupach, J. Sammet, S. Schael, J.F. Schulte, H. Weber, B. Wittmer, V. Zhukov5
M. Ata, M. Brodski,E. Dietz-Laursonn, D. Duchardt, M. Erdmann,R. Fischer, A. Güth, T. Hebbeker, C. Heidemann,K. Hoepfner,D. Klingebiel, S. Knutzen,P. Kreuzer, M. Merschmeyer,A. Meyer, P. Millet, M. Olschewski, K. Padeken,P. Papacz, H. Reithler,S.A. Schmitz,L. Sonnenschein, D. Teyssier,S. Thüer
RWTHAachenUniversity,III.PhysikalischesInstitutA,Aachen,Germany
V. Cherepanov, Y. Erdogan,G. Flügge, H. Geenen, M. Geisler, W. Haj Ahmad, F. Hoehle,B. Kargoll, T. Kress,Y. Kuessel, A. Künsken, J. Lingemann2,A. Nowack, I.M. Nugent,C. Pistone, O. Pooth,A. Stahl
RWTHAachenUniversity,III.PhysikalischesInstitutB,Aachen,Germany
M. Aldaya Martin,I. Asin, N. Bartosik, J. Behr, U. Behrens,A.J. Bell, A. Bethani,K. Borras, A. Burgmeier, A. Cakir,L. Calligaris, A. Campbell,S. Choudhury, F. Costanza, C. Diez Pardos,G. Dolinska,S. Dooling, T. Dorland,G. Eckerlin, D. Eckstein, T. Eichhorn, G. Flucke, J. Garay Garcia, A. Geiser, A. Gizhko, P. Gunnellini, J. Hauk, M. Hempel15,H. Jung, A. Kalogeropoulos, O. Karacheban15, M. Kasemann, P. Katsas, J. Kieseler, C. Kleinwort,I. Korol, D. Krücker,W. Lange, J. Leonard, K. Lipka,A. Lobanov, W. Lohmann15,B. Lutz, R. Mankel, I. Marfin15, I.-A. Melzer-Pellmann,A.B. Meyer, G. Mittag, J. Mnich, A. Mussgiller,S. Naumann-Emme, A. Nayak,E. Ntomari, H. Perrey,D. Pitzl, R. Placakyte, A. Raspereza, P.M. Ribeiro Cipriano,B. Roland, E. Ron, M.Ö. Sahin,J. Salfeld-Nebgen, P. Saxena,T. Schoerner-Sadenius, M. Schröder,C. Seitz, S. Spannagel, A.D.R. Vargas Trevino, R. Walsh, C. Wissing
DeutschesElektronen-Synchrotron,Hamburg,Germany
V. Blobel, M. Centis Vignali, A.R. Draeger,J. Erfle, E. Garutti,K. Goebel, M. Görner, J. Haller, M. Hoffmann,R.S. Höing,A. Junkes, H. Kirschenmann, R. Klanner, R. Kogler,T. Lapsien, T. Lenz,
I. Marchesini,D. Marconi, J. Ott, T. Peiffer, A. Perieanu, N. Pietsch,J. Poehlsen,T. Poehlsen, D. Rathjens, C. Sander,H. Schettler, P. Schleper, E. Schlieckau, A. Schmidt, M. Seidel, V. Sola,H. Stadie, G. Steinbrück, D. Troendle,E. Usai, L. Vanelderen, A. Vanhoefer
UniversityofHamburg,Hamburg,Germany
C. Barth,C. Baus, J. Berger,C. Böser, E. Butz, T. Chwalek, W. De Boer,A. Descroix, A. Dierlamm, M. Feindt,F. Frensch, M. Giffels, A. Gilbert,F. Hartmann2,T. Hauth, U. Husemann, I. Katkov5,
A. Kornmayer2, P. Lobelle Pardo, M.U. Mozer,T. Müller, Th. Müller, A. Nürnberg, G. Quast, K. Rabbertz, S. Röcker,H.J. Simonis, F.M. Stober,R. Ulrich, J. Wagner-Kuhr, S. Wayand, T. Weiler, R. Wolf
InstitutfürExperimentelleKernphysik,Karlsruhe,Germany
G. Anagnostou,G. Daskalakis, T. Geralis,V.A. Giakoumopoulou, A. Kyriakis, D. Loukas,A. Markou, C. Markou, A. Psallidas,I. Topsis-Giotis
InstituteofNuclearandParticlePhysics(INPP),NCSRDemokritos,AghiaParaskevi,Greece
A. Agapitos,S. Kesisoglou, A. Panagiotou,N. Saoulidou, E. Stiliaris, E. Tziaferi
UniversityofAthens,Athens,Greece
X. Aslanoglou,I. Evangelou, G. Flouris,C. Foudas, P. Kokkas, N. Manthos, I. Papadopoulos,E. Paradas, J. Strologas
UniversityofIoánnina,Ioánnina,Greece
G. Bencze,C. Hajdu, P. Hidas,D. Horvath16, F. Sikler,V. Veszpremi, G. Vesztergombi17, A.J. Zsigmond
WignerResearchCentreforPhysics,Budapest,Hungary
N. Beni,S. Czellar, J. Karancsi18,J. Molnar, J. Palinkas, Z. Szillasi
InstituteofNuclearResearchATOMKI,Debrecen,Hungary
A. Makovec,P. Raics, Z.L. Trocsanyi, B. Ujvari
S.K. Swain
NationalInstituteofScienceEducationandResearch,Bhubaneswar,India
S.B. Beri, V. Bhatnagar,R. Gupta, U. Bhawandeep, A.K. Kalsi, M. Kaur, R. Kumar,M. Mittal, N. Nishu, J.B. Singh
PanjabUniversity,Chandigarh,India
Ashok Kumar, Arun Kumar,S. Ahuja, A. Bhardwaj, B.C. Choudhary,A. Kumar, S. Malhotra,M. Naimuddin, K. Ranjan,V. Sharma
UniversityofDelhi,Delhi,India
S. Banerjee, S. Bhattacharya, K. Chatterjee,S. Dutta, B. Gomber, Sa. Jain, Sh. Jain,R. Khurana, A. Modak, S. Mukherjee,D. Roy, S. Sarkar, M. Sharan
SahaInstituteofNuclearPhysics,Kolkata,India
A. Abdulsalam, D. Dutta, V. Kumar, A.K. Mohanty2,L.M. Pant, P. Shukla, A. Topkar
BhabhaAtomicResearchCentre,Mumbai,India
T. Aziz, S. Banerjee, S. Bhowmik19,R.M. Chatterjee, R.K. Dewanjee, S. Dugad, S. Ganguly,S. Ghosh, M. Guchait,A. Gurtu20,G. Kole, S. Kumar, M. Maity19, G. Majumder, K. Mazumdar,G.B. Mohanty, B. Parida,K. Sudhakar, N. Wickramage21
TataInstituteofFundamentalResearch,Mumbai,India
S. Sharma
IndianInstituteofScienceEducationandResearch(IISER),Pune,India
H. Bakhshiansohi,H. Behnamian, S.M. Etesami22, A. Fahim23, R. Goldouzian, M. Khakzad,
M. Mohammadi Najafabadi, M. Naseri, S. Paktinat Mehdiabadi, F. Rezaei Hosseinabadi, B. Safarzadeh24, M. Zeinali
InstituteforResearchinFundamentalSciences(IPM),Tehran,Iran
M. Felcini,M. Grunewald
UniversityCollegeDublin,Dublin,Ireland
M. Abbresciaa,b, C. Calabriaa,b,S.S. Chhibraa,b, A. Colaleoa, D. Creanzaa,c,L. Cristellaa,b,
N. De Filippisa,c, M. De Palmaa,b,L. Fiorea,G. Iasellia,c,G. Maggia,c,M. Maggia, S. Mya,c, S. Nuzzoa,b, A. Pompilia,b,G. Pugliesea,c,R. Radognaa,b,2, G. Selvaggia,b, A. Sharmaa, L. Silvestrisa,2, R. Vendittia,b, P. Verwilligena
aINFNSezionediBari,Bari,Italy bUniversitàdiBari,Bari,Italy cPolitecnicodiBari,Bari,Italy
G. Abbiendia,A.C. Benvenutia,D. Bonacorsia,b, S. Braibant-Giacomellia,b, L. Brigliadoria,b, R. Campaninia,b, P. Capiluppia,b,A. Castroa,b,F.R. Cavalloa, G. Codispotia,b, M. Cuffiania,b,
G.M. Dallavallea,F. Fabbria, A. Fanfania,b, D. Fasanellaa,b,P. Giacomellia,C. Grandia,L. Guiduccia,b, S. Marcellinia, G. Masettia, A. Montanaria, F.L. Navarriaa,b,A. Perrottaa, A.M. Rossia,b,T. Rovellia,b, G.P. Sirolia,b,N. Tosia,b, R. Travaglinia,b
aINFNSezionediBologna,Bologna,Italy bUniversitàdiBologna,Bologna,Italy
S. Albergoa,b,G. Cappelloa, M. Chiorbolia,b, S. Costaa,b, F. Giordanoa,2,R. Potenzaa,b, A. Tricomia,b, C. Tuvea,b
aINFNSezionediCatania,Catania,Italy bUniversitàdiCatania,Catania,Italy cCSFNSM,Catania,Italy
G. Barbaglia,V. Ciullia,b,C. Civininia, R. D’Alessandroa,b, E. Focardia,b,E. Galloa, S. Gonzia,b, V. Goria,b, P. Lenzia,b, M. Meschinia, S. Paolettia,G. Sguazzonia,A. Tropianoa,b
aINFNSezionediFirenze,Firenze,Italy bUniversitàdiFirenze,Firenze,Italy
L. Benussi,S. Bianco, F. Fabbri, D. Piccolo
INFNLaboratoriNazionalidiFrascati,Frascati,Italy
R. Ferrettia,b,F. Ferroa,M. Lo Veterea,b,E. Robuttia, S. Tosia,b
aINFNSezionediGenova,Genova,Italy bUniversitàdiGenova,Genova,Italy
M.E. Dinardoa,b, S. Fiorendia,b, S. Gennaia,2, R. Gerosaa,b,2,A. Ghezzia,b, P. Govonia,b,M.T. Lucchinia,b,2, S. Malvezzia, R.A. Manzonia,b, A. Martellia,b, B. Marzocchia,b,2, D. Menascea,L. Moronia,
M. Paganonia,b,D. Pedrinia, S. Ragazzia,b, N. Redaellia,T. Tabarelli de Fatisa,b
aINFNSezionediMilano-Bicocca,Milano,Italy bUniversitàdiMilano-Bicocca,Milano,Italy
S. Buontempoa, N. Cavalloa,c,S. Di Guidaa,d,2, F. Fabozzia,c,A.O.M. Iorioa,b, L. Listaa,S. Meolaa,d,2, M. Merolaa, P. Paoluccia,2
aINFNSezionediNapoli,Napoli,Italy bUniversitàdiNapoli‘FedericoII’,Napoli,Italy cUniversitàdellaBasilicata(Potenza),Napoli,Italy dUniversitàG.Marconi(Roma),Napoli,Italy
P. Azzia, N. Bacchettaa, D. Biselloa,b, R. Carlina,b, P. Checchiaa,M. Dall’Ossoa,b, T. Dorigoa, F. Gasparinia,b, U. Gasparinia,b,A. Gozzelinoa,M. Gulminia,25,K. Kanishcheva,c,S. Lacapraraa, M. Margonia,b, A.T. Meneguzzoa,b,M. Passaseoa, J. Pazzinia,b, N. Pozzobona,b, P. Ronchesea,b, F. Simonettoa,b,E. Torassaa,M. Tosia,b,P. Zottoa,b,A. Zucchettaa,b,G. Zumerlea,b
aINFNSezionediPadova,Padova,Italy bUniversitàdiPadova,Padova,Italy cUniversitàdiTrento(Trento),Padova,Italy
M. Gabusia,b,S.P. Rattia,b, V. Rea,C. Riccardia,b,P. Salvinia,P. Vituloa,b
aINFNSezionediPavia,Pavia,Italy bUniversitàdiPavia,Pavia,Italy
M. Biasinia,b,G.M. Bileia,D. Ciangottinia,b,2,L. Fanòa,b, P. Laricciaa,b, G. Mantovania,b, M. Menichellia, A. Sahaa, A. Santocchiaa,b,A. Spieziaa,b,2
aINFNSezionediPerugia,Perugia,Italy bUniversitàdiPerugia,Perugia,Italy
K. Androsova,26,P. Azzurria,G. Bagliesia,J. Bernardinia,T. Boccalia,G. Broccoloa,c,R. Castaldia, M.A. Cioccia,26,R. Dell’Orsoa, S. Donatoa,c,2,G. Fedi, F. Fioria,c,L. Foàa,c,A. Giassia, M.T. Grippoa,26, F. Ligabuea,c,T. Lomtadzea,L. Martinia,b, A. Messineoa,b, C.S. Moona,27, F. Pallaa,2, A. Rizzia,b, A. Savoy-Navarroa,28,A.T. Serbana, P. Spagnoloa, P. Squillaciotia,26,R. Tenchinia,G. Tonellia,b, A. Venturia,P.G. Verdinia,C. Vernieria,c
aINFNSezionediPisa,Pisa,Italy bUniversitàdiPisa,Pisa,Italy
cScuolaNormaleSuperiorediPisa,Pisa,Italy
L. Baronea,b, F. Cavallaria,G. D’imperioa,b,D. Del Rea,b, M. Diemoza,C. Jordaa, E. Longoa,b,
F. Margarolia,b, P. Meridiania,F. Michelia,b,2,G. Organtinia,b, R. Paramattia,S. Rahatloua,b, C. Rovellia, F. Santanastasioa,b, L. Soffia,b,P. Traczyka,b,2
aINFNSezionediRoma,Roma,Italy bUniversitàdiRoma,Roma,Italy
N. Amapanea,b, R. Arcidiaconoa,c,S. Argiroa,b,M. Arneodoa,c,R. Bellana,b, C. Biinoa, N. Cartigliaa, S. Casassoa,b,2, M. Costaa,b, R. Covarelli,A. Deganoa,b, N. Demariaa,L. Fincoa,b,2, C. Mariottia, S. Masellia, E. Migliorea,b,V. Monacoa,b,M. Musicha, M.M. Obertinoa,c,L. Pachera,b,N. Pastronea, M. Pelliccionia,G.L. Pinna Angionia,b, A. Potenzaa,b,A. Romeroa,b, M. Ruspaa,c,R. Sacchia,b, A. Solanoa,b, A. Staianoa, U. Tamponia
aINFNSezionediTorino,Torino,Italy bUniversitàdiTorino,Torino,Italy
cUniversitàdelPiemonteOrientale(Novara),Torino,Italy
S. Belfortea,V. Candelisea,b,2, M. Casarsaa,F. Cossuttia, G. Della Riccaa,b,B. Gobboa,C. La Licataa,b, M. Maronea,b,A. Schizzia,b, T. Umera,b,A. Zanettia
aINFNSezionediTrieste,Trieste,Italy bUniversitàdiTrieste,Trieste,Italy
S. Chang, A. Kropivnitskaya,S.K. Nam
KangwonNationalUniversity,Chunchon,RepublicofKorea
D.H. Kim,G.N. Kim, M.S. Kim,D.J. Kong, S. Lee, Y.D. Oh,H. Park, A. Sakharov, D.C. Son
KyungpookNationalUniversity,Daegu,RepublicofKorea
T.J. Kim, M.S. Ryu
ChonbukNationalUniversity,Jeonju,RepublicofKorea
J.Y. Kim, D.H. Moon,S. Song
ChonnamNationalUniversity,InstituteforUniverseandElementaryParticles,Kwangju,RepublicofKorea
S. Choi, D. Gyun,B. Hong, M. Jo,H. Kim, Y. Kim,B. Lee, K.S. Lee, S.K. Park,Y. Roh
KoreaUniversity,Seoul,RepublicofKorea
H.D. Yoo
SeoulNationalUniversity,Seoul,RepublicofKorea
M. Choi,J.H. Kim, I.C. Park, G. Ryu
UniversityofSeoul,Seoul,RepublicofKorea
Y. Choi,Y.K. Choi, J. Goh,D. Kim, E. Kwon, J. Lee, I. Yu
SungkyunkwanUniversity,Suwon,RepublicofKorea
A. Juodagalvis
VilniusUniversity,Vilnius,Lithuania
J.R. Komaragiri, M.A.B. Md Ali,W.A.T. Wan Abdullah
NationalCentreforParticlePhysics,UniversitiMalaya,KualaLumpur,Malaysia
E. Casimiro Linares, H. Castilla-Valdez, E. De La Cruz-Burelo,I. Heredia-de La Cruz, A. Hernandez-Almada,R. Lopez-Fernandez, A. Sanchez-Hernandez
CentrodeInvestigacionydeEstudiosAvanzadosdelIPN,MexicoCity,Mexico
S. Carrillo Moreno, F. Vazquez Valencia
UniversidadIberoamericana,MexicoCity,Mexico
I. Pedraza, H.A. Salazar Ibarguen
A. Morelos Pineda
UniversidadAutónomadeSanLuisPotosí,SanLuisPotosí,Mexico
D. Krofcheck
UniversityofAuckland,Auckland,NewZealand
P.H. Butler,S. Reucroft
UniversityofCanterbury,Christchurch,NewZealand
A. Ahmad, M. Ahmad, Q. Hassan,H.R. Hoorani, W.A. Khan,T. Khurshid, M. Shoaib
NationalCentreforPhysics,Quaid-I-AzamUniversity,Islamabad,Pakistan
H. Bialkowska,M. Bluj, B. Boimska,T. Frueboes, M. Górski, M. Kazana, K. Nawrocki, K. Romanowska-Rybinska,M. Szleper, P. Zalewski
NationalCentreforNuclearResearch,Swierk,Poland
G. Brona,K. Bunkowski, M. Cwiok,W. Dominik,K. Doroba, A. Kalinowski,M. Konecki, J. Krolikowski, M. Misiura, M. Olszewski
InstituteofExperimentalPhysics,FacultyofPhysics,UniversityofWarsaw,Warsaw,Poland
P. Bargassa,C. Beirão Da Cruz E Silva, P. Faccioli, P.G. Ferreira Parracho,M. Gallinaro, L. Lloret Iglesias, F. Nguyen, J. Rodrigues Antunes,J. Seixas, J. Varela, P. Vischia
LaboratóriodeInstrumentaçãoeFísicaExperimentaldePartículas,Lisboa,Portugal
M. Gavrilenko,I. Golutvin, A. Kamenev, V. Karjavin, V. Konoplyanikov, V. Korenkov,G. Kozlov, A. Lanev, A. Malakhov,V. Matveev29,V.V. Mitsyn, P. Moisenz, V. Palichik,V. Perelygin, S. Shmatov, V. Smirnov, E. Tikhonenko, A. Zarubin
JointInstituteforNuclearResearch,Dubna,Russia
V. Golovtsov,Y. Ivanov, V. Kim30,E. Kuznetsova, P. Levchenko, V. Murzin, V. Oreshkin, I. Smirnov, V. Sulimov,L. Uvarov, S. Vavilov, A. Vorobyev,An. Vorobyev
PetersburgNuclearPhysicsInstitute,Gatchina(St.Petersburg),Russia
Yu. Andreev,A. Dermenev,S. Gninenko, N. Golubev, M. Kirsanov, N. Krasnikov, A. Pashenkov, D. Tlisov, A. Toropin
InstituteforNuclearResearch,Moscow,Russia
V. Epshteyn,V. Gavrilov, N. Lychkovskaya,V. Popov, I. Pozdnyakov,G. Safronov, S. Semenov, A. Spiridonov,V. Stolin, E. Vlasov,A. Zhokin
InstituteforTheoreticalandExperimentalPhysics,Moscow,Russia
V. Andreev,M. Azarkin31,I. Dremin31, M. Kirakosyan, A. Leonidov31,G. Mesyats, S.V. Rusakov, A. Vinogradov
P.N.LebedevPhysicalInstitute,Moscow,Russia
A. Belyaev,E. Boos,M. Dubinin32, L. Dudko,A. Ershov, A. Gribushin,V. Klyukhin, O. Kodolova,I. Lokhtin, S. Obraztsov,S. Petrushanko,V. Savrin, A. Snigirev
SkobeltsynInstituteofNuclearPhysics,LomonosovMoscowStateUniversity,Moscow,Russia
I. Azhgirey,I. Bayshev,S. Bitioukov, V. Kachanov, A. Kalinin, D. Konstantinov,V. Krychkine, V. Petrov, R. Ryutin, A. Sobol,L. Tourtchanovitch, S. Troshin, N. Tyurin, A. Uzunian,A. Volkov
P. Adzic33, M. Ekmedzic,J. Milosevic,V. Rekovic
UniversityofBelgrade,FacultyofPhysicsandVincaInstituteofNuclearSciences,Belgrade,Serbia
J. Alcaraz Maestre, C. Battilana,E. Calvo, M. Cerrada,M. Chamizo Llatas, N. Colino, B. De La Cruz, A. Delgado Peris,D. Domínguez Vázquez, A. Escalante Del Valle, C. Fernandez Bedoya,
J.P. Fernández Ramos,J. Flix, M.C. Fouz,P. Garcia-Abia,O. Gonzalez Lopez, S. Goy Lopez, J.M. Hernandez, M.I. Josa,E. Navarro De Martino, A. Pérez-Calero Yzquierdo, J. Puerta Pelayo, A. Quintario Olmeda, I. Redondo,L. Romero, M.S. Soares
CentrodeInvestigacionesEnergéticasMedioambientalesyTecnológicas(CIEMAT),Madrid,Spain
C. Albajar, J.F. de Trocóniz, M. Missiroli, D. Moran
UniversidadAutónomadeMadrid,Madrid,Spain
H. Brun, J. Cuevas,J. Fernandez Menendez, S. Folgueras, I. Gonzalez Caballero
UniversidaddeOviedo,Oviedo,Spain
J.A. Brochero Cifuentes, I.J. Cabrillo, A. Calderon, J. Duarte Campderros,M. Fernandez, G. Gomez, A. Graziano, A. Lopez Virto,J. Marco, R. Marco,C. Martinez Rivero, F. Matorras, F.J. Munoz Sanchez, J. Piedra Gomez, T. Rodrigo,A.Y. Rodríguez-Marrero,A. Ruiz-Jimeno, L. Scodellaro,I. Vila,
R. Vilar Cortabitarte
InstitutodeFísicadeCantabria(IFCA),CSIC-UniversidaddeCantabria,Santander,Spain
D. Abbaneo, E. Auffray, G. Auzinger, M. Bachtis,P. Baillon, A.H. Ball, D. Barney, A. Benaglia, J. Bendavid, L. Benhabib,J.F. Benitez, P. Bloch, A. Bocci, A. Bonato, O. Bondu,C. Botta, H. Breuker, T. Camporesi, G. Cerminara, S. Colafranceschi34,M. D’Alfonso, D. d’Enterria, A. Dabrowski, A. David,F. De Guio, A. De Roeck, S. De Visscher, E. Di Marco,M. Dobson, M. Dordevic, B. Dorney, N. Dupont-Sagorin, A. Elliott-Peisert, G. Franzoni, W. Funk, D. Gigi,K. Gill, D. Giordano, M. Girone,F. Glege, R. Guida, S. Gundacker, M. Guthoff,J. Hammer, M. Hansen,P. Harris,J. Hegeman, V. Innocente, P. Janot, K. Kousouris,K. Krajczar, P. Lecoq,C. Lourenço, N. Magini, L. Malgeri,M. Mannelli, J. Marrouche,
L. Masetti, F. Meijers, S. Mersi,E. Meschi, F. Moortgat, S. Morovic, M. Mulders, L. Orsini, L. Pape,E. Perez, A. Petrilli, G. Petrucciani,A. Pfeiffer, M. Pimiä, D. Piparo, M. Plagge, A. Racz,G. Rolandi35, M. Rovere, H. Sakulin, C. Schäfer, C. Schwick,A. Sharma,P. Siegrist, P. Silva,M. Simon, P. Sphicas36,D. Spiga,
J. Steggemann,B. Stieger, M. Stoye,Y. Takahashi, D. Treille, A. Tsirou, G.I. Veres17,N. Wardle, H.K. Wöhri, H. Wollny, W.D. Zeuner
CERN,EuropeanOrganizationforNuclearResearch,Geneva,Switzerland
W. Bertl,K. Deiters, W. Erdmann, R. Horisberger, Q. Ingram, H.C. Kaestli, D. Kotlinski,U. Langenegger, D. Renker, T. Rohe
PaulScherrerInstitut,Villigen,Switzerland
F. Bachmair, L. Bäni, L. Bianchini, M.A. Buchmann,B. Casal, N. Chanon, G. Dissertori, M. Dittmar, M. Donegà, M. Dünser,P. Eller, C. Grab,D. Hits, J. Hoss,G. Kasieczka, W. Lustermann,B. Mangano, A.C. Marini,M. Marionneau, P. Martinez Ruiz del Arbol,M. Masciovecchio, D. Meister, N. Mohr, P. Musella, C. Nägeli37, F. Nessi-Tedaldi, F. Pandolfi, F. Pauss,L. Perrozzi, M. Peruzzi,M. Quittnat, L. Rebane, M. Rossini,A. Starodumov38, M. Takahashi, K. Theofilatos,R. Wallny, H.A. Weber
InstituteforParticlePhysics,ETHZurich,Zurich,Switzerland
C. Amsler39, M.F. Canelli,V. Chiochia,A. De Cosa, A. Hinzmann, T. Hreus, B. Kilminster, C. Lange, J. Ngadiuba,D. Pinna, P. Robmann, F.J. Ronga,S. Taroni, Y. Yang
M. Cardaci,K.H. Chen, C. Ferro, C.M. Kuo, W. Lin, Y.J. Lu,R. Volpe, S.S. Yu
NationalCentralUniversity,Chung-Li,Taiwan
P. Chang, Y.H. Chang,Y. Chao, K.F. Chen, P.H. Chen, C. Dietz, U. Grundler,W.-S. Hou,Y.F. Liu, R.-S. Lu, M. Miñano Moya,E. Petrakou, Y.M. Tzeng,R. Wilken
NationalTaiwanUniversity(NTU),Taipei,Taiwan
B. Asavapibhop,G. Singh, N. Srimanobhas, N. Suwonjandee
ChulalongkornUniversity,FacultyofScience,DepartmentofPhysics,Bangkok,Thailand
A. Adiguzel, M.N. Bakirci40,S. Cerci41, C. Dozen,I. Dumanoglu, E. Eskut, S. Girgis, G. Gokbulut, Y. Guler, E. Gurpinar,I. Hos, E.E. Kangal42,A. Kayis Topaksu, G. Onengut43,K. Ozdemir44,S. Ozturk40, A. Polatoz, D. Sunar Cerci41, B. Tali41, H. Topakli40, M. Vergili, C. Zorbilmez
CukurovaUniversity,Adana,Turkey
I.V. Akin,B. Bilin, S. Bilmis, H. Gamsizkan45, B. Isildak46, G. Karapinar47,K. Ocalan48,S. Sekmen, U.E. Surat,M. Yalvac, M. Zeyrek
MiddleEastTechnicalUniversity,PhysicsDepartment,Ankara,Turkey
E.A. Albayrak49, E. Gülmez,M. Kaya50,O. Kaya51, T. Yetkin52
BogaziciUniversity,Istanbul,Turkey
K. Cankocak,F.I. Vardarlı
IstanbulTechnicalUniversity,Istanbul,Turkey
L. Levchuk,P. Sorokin
NationalScientificCenter,KharkovInstituteofPhysicsandTechnology,Kharkov,Ukraine
J.J. Brooke,E. Clement, D. Cussans,H. Flacher, J. Goldstein,M. Grimes, G.P. Heath, H.F. Heath,J. Jacob, L. Kreczko,C. Lucas, Z. Meng, D.M. Newbold53,S. Paramesvaran, A. Poll, T. Sakuma,S. Seif El Nasr-storey, S. Senkin,V.J. Smith
UniversityofBristol,Bristol,UnitedKingdom
K.W. Bell,A. Belyaev54,C. Brew, R.M. Brown, D.J.A. Cockerill, J.A. Coughlan, K. Harder,S. Harper, E. Olaiya,D. Petyt, C.H. Shepherd-Themistocleous, A. Thea,I.R. Tomalin, T. Williams, W.J. Womersley, S.D. Worm
RutherfordAppletonLaboratory,Didcot,UnitedKingdom
M. Baber,R. Bainbridge, O. Buchmuller, D. Burton,D. Colling, N. Cripps,P. Dauncey, G. Davies, M. Della Negra,P. Dunne, A. Elwood, W. Ferguson, J. Fulcher, D. Futyan,G. Hall, G. Iles, M. Jarvis, G. Karapostoli,M. Kenzie, R. Lane,R. Lucas53,L. Lyons, A.-M. Magnan, S. Malik,B. Mathias, J. Nash, A. Nikitenko38,J. Pela, M. Pesaresi, K. Petridis,D.M. Raymond, S. Rogerson, A. Rose,C. Seez, P. Sharp†, A. Tapper,M. Vazquez Acosta, T. Virdee,S.C. Zenz
ImperialCollege,London,UnitedKingdom
J.E. Cole, P.R. Hobson,A. Khan, P. Kyberd,D. Leggat, D. Leslie,I.D. Reid, P. Symonds, L. Teodorescu, M. Turner
BrunelUniversity,Uxbridge,UnitedKingdom
J. Dittmann, K. Hatakeyama,A. Kasmi, H. Liu, N. Pastika, T. Scarborough,Z. Wu
O. Charaf,S.I. Cooper, C. Henderson, P. Rumerio
TheUniversityofAlabama,Tuscaloosa,USA
A. Avetisyan, T. Bose,C. Fantasia, P. Lawson, C. Richardson, J. Rohlf, J. St. John,L. Sulak
BostonUniversity,Boston,USA
J. Alimena,E. Berry, S. Bhattacharya, G. Christopher, D. Cutts, Z. Demiragli, N. Dhingra, A. Ferapontov, A. Garabedian,U. Heintz, E. Laird, G. Landsberg, Z. Mao,M. Narain, S. Sagir,T. Sinthuprasith, T. Speer, J. Swanson
BrownUniversity,Providence,USA
R. Breedon,G. Breto, M. Calderon De La Barca Sanchez, S. Chauhan,M. Chertok, J. Conway,R. Conway, P.T. Cox, R. Erbacher,M. Gardner,W. Ko, R. Lander,M. Mulhearn, D. Pellett, J. Pilot, F. Ricci-Tam, S. Shalhout, J. Smith, M. Squires, D. Stolp, M. Tripathi, S. Wilbur,R. Yohay
UniversityofCalifornia,Davis,Davis,USA
R. Cousins,P. Everaerts,C. Farrell, J. Hauser, M. Ignatenko, G. Rakness, E. Takasugi, V. Valuev,M. Weber
UniversityofCalifornia,LosAngeles,USA
K. Burt, R. Clare,J. Ellison, J.W. Gary, G. Hanson,J. Heilman, M. Ivova Rikova, P. Jandir, E. Kennedy, F. Lacroix,O.R. Long, A. Luthra, M. Malberti, M. Olmedo Negrete, A. Shrinivas,S. Sumowidagdo, S. Wimpenny
UniversityofCalifornia,Riverside,Riverside,USA
J.G. Branson, G.B. Cerati,S. Cittolin,R.T. D’Agnolo, A. Holzner, R. Kelley, D. Klein, J. Letts, I. Macneill, D. Olivito, S. Padhi, C. Palmer,M. Pieri, M. Sani, V. Sharma,S. Simon, M. Tadel,Y. Tu, A. Vartak,C. Welke, F. Würthwein,A. Yagil, G. Zevi Della Porta
UniversityofCalifornia,SanDiego,LaJolla,USA
D. Barge, J. Bradmiller-Feld, C. Campagnari, T. Danielson, A. Dishaw,V. Dutta, K. Flowers,
M. Franco Sevilla,P. Geffert, C. George, F. Golf, L. Gouskos,J. Incandela, C. Justus,N. Mccoll, S.D. Mullin, J. Richman, D. Stuart,W. To,C. West, J. Yoo
UniversityofCalifornia,SantaBarbara,SantaBarbara,USA
A. Apresyan,A. Bornheim, J. Bunn, Y. Chen, J. Duarte,A. Mott, H.B. Newman, C. Pena, M. Pierini, M. Spiropulu, J.R. Vlimant,R. Wilkinson, S. Xie, R.Y. Zhu
CaliforniaInstituteofTechnology,Pasadena,USA
V. Azzolini,A. Calamba, B. Carlson, T. Ferguson, Y. Iiyama, M. Paulini,J. Russ, H. Vogel,I. Vorobiev
CarnegieMellonUniversity,Pittsburgh,USA
J.P. Cumalat, W.T. Ford,A. Gaz, M. Krohn, E. Luiggi Lopez,U. Nauenberg, J.G. Smith, K. Stenson, S.R. Wagner
UniversityofColoradoatBoulder,Boulder,USA
J. Alexander, A. Chatterjee, J. Chaves,J. Chu, S. Dittmer, N. Eggert, N. Mirman, G. Nicolas Kaufman, J.R. Patterson,A. Ryd, E. Salvati, L. Skinnari,W. Sun, W.D. Teo, J. Thom, J. Thompson, J. Tucker, Y. Weng, L. Winstrom,P. Wittich
CornellUniversity,Ithaca,USA
D. Winn
S. Abdullin,M. Albrow, J. Anderson, G. Apollinari, L.A.T. Bauerdick, A. Beretvas, J. Berryhill,P.C. Bhat, G. Bolla,K. Burkett,J.N. Butler, H.W.K. Cheung, F. Chlebana, S. Cihangir,V.D. Elvira, I. Fisk, J. Freeman, E. Gottschalk,L. Gray, D. Green, S. Grünendahl, O. Gutsche, J. Hanlon, D. Hare, R.M. Harris, J. Hirschauer, B. Hooberman, S. Jindariani, M. Johnson,U. Joshi, B. Klima, B. Kreis, S. Kwan†,J. Linacre, D. Lincoln, R. Lipton, T. Liu,R. Lopes De Sá, J. Lykken,K. Maeshima, J.M. Marraffino, V.I. Martinez Outschoorn, S. Maruyama,D. Mason, P. McBride, P. Merkel,K. Mishra, S. Mrenna, S. Nahn, C. Newman-Holmes, V. O’Dell,O. Prokofyev, E. Sexton-Kennedy, A. Soha,W.J. Spalding, L. Spiegel, L. Taylor,S. Tkaczyk, N.V. Tran,L. Uplegger, E.W. Vaandering, R. Vidal,A. Whitbeck, J. Whitmore, F. Yang
FermiNationalAcceleratorLaboratory,Batavia,USA
D. Acosta, P. Avery, P. Bortignon, D. Bourilkov, M. Carver, D. Curry,S. Das, M. De Gruttola,
G.P. Di Giovanni, R.D. Field, M. Fisher, I.K. Furic, J. Hugon, J. Konigsberg,A. Korytov, T. Kypreos, J.F. Low, K. Matchev,H. Mei, P. Milenovic55, G. Mitselmakher,L. Muniz, A. Rinkevicius, L. Shchutska, M. Snowball, D. Sperka,J. Yelton, M. Zakaria
UniversityofFlorida,Gainesville,USA
S. Hewamanage, S. Linn, P. Markowitz, G. Martinez, J.L. Rodriguez
FloridaInternationalUniversity,Miami,USA
J.R. Adams, T. Adams,A. Askew,J. Bochenek, B. Diamond, J. Haas, S. Hagopian,V. Hagopian, K.F. Johnson, H. Prosper,V. Veeraraghavan, M. Weinberg
FloridaStateUniversity,Tallahassee,USA
M.M. Baarmand,M. Hohlmann, H. Kalakhety, F. Yumiceva
FloridaInstituteofTechnology,Melbourne,USA
M.R. Adams,L. Apanasevich, D. Berry, R.R. Betts, I. Bucinskaite,R. Cavanaugh, O. Evdokimov, L. Gauthier, C.E. Gerber,D.J. Hofman,P. Kurt, C. O’Brien,I.D. Sandoval Gonzalez, C. Silkworth,P. Turner, N. Varelas
UniversityofIllinoisatChicago(UIC),Chicago,USA
B. Bilki56,W. Clarida, K. Dilsiz, M. Haytmyradov, J.-P. Merlo, H. Mermerkaya57,A. Mestvirishvili, A. Moeller, J. Nachtman, H. Ogul, Y. Onel,F. Ozok49, A. Penzo,R. Rahmat, S. Sen, P. Tan, E. Tiras, J. Wetzel,K. Yi
TheUniversityofIowa,IowaCity,USA
I. Anderson,B.A. Barnett, B. Blumenfeld, S. Bolognesi, D. Fehling, A.V. Gritsan, P. Maksimovic,C. Martin, M. Swartz,M. Xiao
JohnsHopkinsUniversity,Baltimore,USA
P. Baringer,A. Bean,G. Benelli, C. Bruner, J. Gray, R.P. Kenny III, D. Majumder, M. Malek,M. Murray, D. Noonan, S. Sanders,J. Sekaric, R. Stringer, Q. Wang,J.S. Wood
TheUniversityofKansas,Lawrence,USA
I. Chakaberia,A. Ivanov, K. Kaadze,S. Khalil, M. Makouski,Y. Maravin, L.K. Saini, N. Skhirtladze, I. Svintradze
KansasStateUniversity,Manhattan,USA
J. Gronberg,D. Lange, F. Rebassoo,D. Wright
A. Baden, A. Belloni,B. Calvert, S.C. Eno, J.A. Gomez, N.J. Hadley, S. Jabeen, R.G. Kellogg,T. Kolberg, Y. Lu, A.C. Mignerey, K. Pedro, A. Skuja, M.B. Tonjes,S.C. Tonwar
UniversityofMaryland,CollegePark,USA
A. Apyan,R. Barbieri, K. Bierwagen, W. Busza, I.A. Cali,L. Di Matteo, G. Gomez Ceballos, M. Goncharov, D. Gulhan, M. Klute,Y.S. Lai, Y.-J. Lee,A. Levin, P.D. Luckey, C. Paus,D. Ralph, C. Roland, G. Roland, G.S.F. Stephans, K. Sumorok, D. Velicanu,J. Veverka, B. Wyslouch,M. Yang, M. Zanetti,V. Zhukova
MassachusettsInstituteofTechnology,Cambridge,USA
B. Dahmes, A. Gude, S.C. Kao, K. Klapoetke, Y. Kubota,J. Mans, S. Nourbakhsh, R. Rusack, A. Singovsky, N. Tambe, J. Turkewitz
UniversityofMinnesota,Minneapolis,USA
J.G. Acosta,S. Oliveros
UniversityofMississippi,Oxford,USA
E. Avdeeva, K. Bloom, S. Bose,D.R. Claes, A. Dominguez,R. Gonzalez Suarez, J. Keller,D. Knowlton, I. Kravchenko, J. Lazo-Flores, F. Meier,F. Ratnikov, G.R. Snow, M. Zvada
UniversityofNebraska-Lincoln,Lincoln,USA
J. Dolen, A. Godshalk,I. Iashvili, A. Kharchilava, A. Kumar,S. Rappoccio
StateUniversityofNewYorkatBuffalo,Buffalo,USA
G. Alverson, E. Barberis, D. Baumgartel, M. Chasco, A. Massironi, D.M. Morse,D. Nash, T. Orimoto, D. Trocino, R.-J. Wang, D. Wood,J. Zhang
NortheasternUniversity,Boston,USA
K.A. Hahn, A. Kubik, N. Mucia,N. Odell, B. Pollack, A. Pozdnyakov, M. Schmitt,S. Stoynev, K. Sung, M. Velasco, S. Won
NorthwesternUniversity,Evanston,USA
A. Brinkerhoff, K.M. Chan,A. Drozdetskiy, M. Hildreth, C. Jessop,D.J. Karmgard, N. Kellams, K. Lannon, S. Lynch, N. Marinelli, Y. Musienko29, T. Pearson,M. Planer, R. Ruchti,G. Smith, N. Valls, M. Wayne, M. Wolf,A. Woodard
UniversityofNotreDame,NotreDame,USA
L. Antonelli, J. Brinson, B. Bylsma, L.S. Durkin, S. Flowers, A. Hart, C. Hill, R. Hughes,K. Kotov, T.Y. Ling, W. Luo, D. Puigh,M. Rodenburg, B.L. Winer,H. Wolfe, H.W. Wulsin
TheOhioStateUniversity,Columbus,USA
O. Driga,P. Elmer, J. Hardenbrook, P. Hebda,S.A. Koay, P. Lujan, D. Marlow,T. Medvedeva, M. Mooney, J. Olsen, P. Piroué, X. Quan, H. Saka,D. Stickland2,C. Tully, J.S. Werner, A. Zuranski
PrincetonUniversity,Princeton,USA
E. Brownson,S. Malik, H. Mendez, J.E. Ramirez Vargas
UniversityofPuertoRico,Mayaguez,USA
V.E. Barnes,D. Benedetti, D. Bortoletto,M. De Mattia, L. Gutay, Z. Hu, M.K. Jha, M. Jones, K. Jung, M. Kress, N. Leonardo,D.H. Miller, N. Neumeister, F. Primavera, B.C. Radburn-Smith, X. Shi, I. Shipsey, D. Silvers, A. Svyatkovskiy, F. Wang, W. Xie, L. Xu, J. Zablocki
N. Parashar,J. Stupak
PurdueUniversityCalumet,Hammond,USA
A. Adair,B. Akgun, K.M. Ecklund, F.J.M. Geurts, W. Li, B. Michlin, B.P. Padley,R. Redjimi, J. Roberts, J. Zabel
RiceUniversity,Houston,USA
B. Betchart,A. Bodek, P. de Barbaro, R. Demina, Y. Eshaq,T. Ferbel, M. Galanti, A. Garcia-Bellido,
P. Goldenzweig,J. Han, A. Harel, O. Hindrichs, A. Khukhunaishvili, S. Korjenevski, G. Petrillo,M. Verzetti, D. Vishnevskiy
UniversityofRochester,Rochester,USA
R. Ciesielski,L. Demortier, K. Goulianos, C. Mesropian
TheRockefellerUniversity,NewYork,USA
S. Arora,A. Barker, J.P. Chou, C. Contreras-Campana, E. Contreras-Campana,D. Duggan, D. Ferencek, Y. Gershtein,R. Gray, E. Halkiadakis, D. Hidas,S. Kaplan, A. Lath,S. Panwalkar, M. Park, S. Salur, S. Schnetzer, D. Sheffield, S. Somalwar, R. Stone,S. Thomas, P. Thomassen,M. Walker
Rutgers,TheStateUniversityofNewJersey,Piscataway,USA
K. Rose, S. Spanier,A. York
UniversityofTennessee,Knoxville,USA
O. Bouhali58, A. Castaneda Hernandez, S. Dildick,R. Eusebi,W. Flanagan, J. Gilmore, T. Kamon59, V. Khotilovich,V. Krutelyov, R. Montalvo, I. Osipenkov,Y. Pakhotin, R. Patel, A. Perloff,J. Roe, A. Rose, A. Safonov,I. Suarez,A. Tatarinov, K.A. Ulmer
TexasA&MUniversity,CollegeStation,USA
N. Akchurin, C. Cowden,J. Damgov, C. Dragoiu, P.R. Dudero, J. Faulkner, K. Kovitanggoon, S. Kunori, S.W. Lee, T. Libeiro, I. Volobouev
TexasTechUniversity,Lubbock,USA
E. Appelt,A.G. Delannoy, S. Greene,A. Gurrola, W. Johns, C. Maguire, Y. Mao,A. Melo, M. Sharma, P. Sheldon,B. Snook, S. Tuo, J. Velkovska
VanderbiltUniversity,Nashville,USA
M.W. Arenton, S. Boutle,B. Cox,B. Francis, J. Goodell, R. Hirosky, A. Ledovskoy, H. Li,C. Lin, C. Neu, E. Wolfe,J. Wood
UniversityofVirginia,Charlottesville,USA
C. Clarke, R. Harr, P.E. Karchin, C. Kottachchi Kankanamge Don,P. Lamichhane, J. Sturdy
WayneStateUniversity,Detroit,USA
D.A. Belknap,D. Carlsmith, M. Cepeda, S. Dasu, L. Dodd, S. Duric, E. Friis,R. Hall-Wilton, M. Herndon, A. Hervé,P. Klabbers, A. Lanaro, C. Lazaridis, A. Levine, R. Loveless,A. Mohapatra, I. Ojalvo, T. Perry, G.A. Pierro,G. Polese,I. Ross, T. Sarangi, A. Savin,W.H. Smith, D. Taylor,C. Vuosalo, N. Woods
UniversityofWisconsin,Madison,USA
E-mailaddress:cms-publication-committee-chair@cern.ch(G. Hamel de Monchenault).
† Deceased.
1 AlsoatViennaUniversityofTechnology,Vienna,Austria.