Physics Letters B 768 (2017) 103–129
Contents lists available atScienceDirect
Physics
Letters
B
www.elsevier.com/locate/physletb
Multiplicity
and
rapidity
dependence
of
strange
hadron
production
in pp,
pPb,
and
PbPb
collisions
at
the
LHC
.
The
CMS
Collaboration
CERN,Switzerland
a
r
t
i
c
l
e
i
n
f
o
a
b
s
t
r
a
c
t
Articlehistory: Received21May2016
Receivedinrevisedform10December2016 Accepted16January2017
Availableonline20February2017 Editor:M.Doser Keywords: CMS Physics Heavyion Spectra Radialflow
Measurements ofstrange hadron (K0
S,+,and−+
+)transverse momentumspectrain pp,pPb, andPbPb collisionsarepresentedoverawiderangeofrapidityandeventcharged-particlemultiplicity. The data werecollectedwiththe CMS detectoratthe CERN LHCinpp collisions at√s=7TeV,pPb collisions at√sN N=5.02TeV,and PbPb collisions at√sN N=2.76TeV.Theaveragetransverse kinetic
energyisfoundtoincreasewithmultiplicity,atafasterrate forheavierstrange particlespeciesinall systems.Atsimilar multiplicities,thedifferenceinaveragetransverse kineticenergybetweendifferent particlespeciesisobservedtobelargerforpp andpPb eventsthanforPbPb events.InpPb collisions, theaveragetransversekineticenergyisfoundtobeslightlylargerinthePb-goingdirectionthaninthe p-goingdirectionforeventswithlarge multiplicity.Thespectraarecomparedtomodels motivatedby hydrodynamics.
©2017TheAuthor(s).PublishedbyElsevierB.V.ThisisanopenaccessarticleundertheCCBYlicense (http://creativecommons.org/licenses/by/4.0/).FundedbySCOAP3.
1. Introduction
Studiesofstrange-particle productioninhighenergycollisions ofprotonsandheavy ionsprovideimportantmeanstoinvestigate thedynamics ofthe collision process. Earlier studies of relativis-ticheavy ion collisions at the BNL RHIC and CERN SPS colliders indicatedanenhancementofstrangenessproductionwithrespect toproton–proton(pp)collisions[1,2],whichwashistorically inter-pretedto bedueto the formationofa high-densityquark–gluon medium[3].Theabundanceofstrangeparticlesatdifferent center-of-massenergiesisinlinewithcalculationsfromthermal statisti-cal models [4–6]. In gold–gold (AuAu) collisions at RHIC, strong azimuthal correlationsof final-statehadronswere observed, sug-gestingthattheproducedmediumbehaveslikeanear-perfectfluid undergoingapressure-drivenanisotropicexpansion[2].Studiesof strangenessandlightflavorproductionanddynamicsinheavyion collisions have provided further insight into the medium’s fluid-likenatureandevidenceforitspartoniccollectivity[2,7].
In recent years, the observation of a long-range “ridge” at smallazimuthalseparations intwo-particlecorrelationsin pp [8]
andproton-lead(pPb) [9–11] collisions withhighevent-by-event charged-particle multiplicity (referred to hereafter as “multiplici-ty”)hasprovidedanindicationforcollectiveeffectsinsystemsthat areanorderofmagnitudesmallerinsizethanheavyioncollisions.
E-mailaddress:cms-publication-committee-chair@cern.ch.
Thenatureoftheobservedlong-rangeparticlecorrelationsinhigh multiplicitypp andpPb collisionsisstillunderintensedebate[12]. Whilethe collectiveflowofa fluid-likemedium providesa natu-ral interpretation[13–16],other modelsattributethisbehaviorto theinitialcorrelationofgluons[17–21],ortheanisotropic escape ofparticles[22].
Studies of identified particle production and correlations in highmultiplicity pp and pPb collisionsprovide detailed informa-tion abouttheunderlying particleproductionmechanism. Identi-fiedparticle(includingstrange-hadron)transversemomentum(pT)
spectra andazimuthal anisotropies in lead–lead (PbPb) collisions attheCERNLHC havebeenstudied[23,24]anddescribed by hy-drodynamicmodels[25,26].Similarmeasurementshavebeen per-formed in pPb collisions as a function of multiplicity, where an indication of acommon velocity boostto the produced particles, knownas“radial flow”[27,28],andforamassdependenceofthe anisotropicflow[29,30]havebeenobserved.WhencomparingpPb andPbPb systemsatsimilarmultiplicities,a strongerradial veloc-ityboostisseen inthesmallerpPb collision system[27,30].This couldberelatedtoamuchhigherinitialenergydensityinahigh multiplicitybutsmallersystem,resultinginalargerpressure gra-dientoutwardalongtheradialdirection, aspredictedinRef.[31]. Toperform a quantitative comparison, a common average radial-flowvelocityfromdifferentcollisionsystemscanbeextractedfrom asimultaneousfittothespectraofvariousparticlespecies, based on the blast-wave model [32]. Inspired by hydrodynamics, the blast-wavemodelassumesa commonkinetic freeze-out
tempera-http://dx.doi.org/10.1016/j.physletb.2017.01.075
0370-2693/©2017TheAuthor(s).PublishedbyElsevierB.V.ThisisanopenaccessarticleundertheCCBYlicense(http://creativecommons.org/licenses/by/4.0/).Fundedby SCOAP3.
pp events represent an even smaller system than pPb events, a strongerradial-flowboostmightbepresentcomparedtopPb and PbPb events ata comparable multiplicity [31]. Furthermore, ina pPb collision,thesystemisnotsymmetricinpseudorapidity(
η
).If afluid-likemediumisformed,itsenergydensitycouldbedifferent onthep- and Pb-goingsides, whichcouldlead toan asymmetry inthecollectiveradial-floweffectasafunctionofη
. Hydrodynam-icalmodelspredictthattheaveragepT(or, equivalently,theaver-agetransversekineticenergy
KET,whereKET≡
mT−
m,with mT=
m2
+
p2T and m the particle mass) of produced particles
is larger in the Pb-goingdirection than in the p-going direction, whilethistrendcould bereversedinmodelsbasedongluon sat-uration [37]. Measurement of identified particle pT spectra as a
functionof
η
couldthushelptoconstraintheoreticalmodels. ThisLetterpresentsmeasurementsofstrange-particle pTspec-trainpp,pPb,andPbPb collisionsasafunctionofthemultiplicity inthe events.Specifically, we examine thespectra ofK0
S,
, and
− particles, where the inclusion of the charge-conjugate states isimplied for
and
− particles. The data were collected with theCMSdetectorattheLHC.Withtheimplementationofa ded-icated high-multiplicitytrigger, thepp and pPb datasamples ex-hibitmultiplicitiescomparabletothatobservedinperipheralPbPb collisions,where “peripheral”refers to
∼
50–100% centrality, with centralitydefinedasthefractionofthetotalinelasticcrosssection. Themostcentralcollisionshave0%centrality.Thisoverlapinmean multiplicityallowsthethreesystems,withdrasticallydifferent col-lisiongeometries, tobe compared.The largesolid-angle coverage oftheCMSdetectorpermitsthestrange-particle pT spectratobestudiedindifferentrapidityranges,andthusthestudyofpossible asymmetrieswithrespecttothep- andPb-goingdirectionsinpPb collisions.
2. Detectoranddatasamples
Thecentralfeature oftheCMSapparatusisasuperconducting solenoid of 6 m internal diameter, which provides an axial field of3.8T.Withinthesolenoidvolume area siliconpixelandstrip tracker(with13and14layers inthecentralandendcapregions, respectively), alead tungstatecrystalelectromagnetic calorimeter (ECAL), and a brass and scintillator hadron calorimeter (HCAL), each composed ofa barrel andtwo endcapsections. The tracker covers the pseudorapidity range
|
η
|
<
2.
5. Reconstructed tracks with 1<
pT<
10GeV typically have resolutions of 1.5–3% in pTand 25–90 (45–150) μm in the transverse (longitudinal) impact parameter [38]. The ECAL and HCAL each cover
|
η
|
<
3.
0 while forwardhadron calorimeters(HF) cover 3<
|
η
|
<
5.Muons with|
η
|
<
2.
4 aremeasuredwithgas-ionizationdetectorsembeddedin the steel flux-return yoke outside the solenoid. A more detailed descriptionoftheCMSdetector,together withadefinitionofthe coordinate system and the relevant kinematic variables, can be foundinRef. [39].The MonteCarlo(MC) simulationoftheparti-ingthedatafromthetworunperiods.Becauseoftheasymmetric beam conditions,the nucleon–nucleoncenter-of-mass inthe pPb collisions moves with speed
β
=
0.
434 in the laboratory frame, corresponding to a rapidity of 0.465. As a consequence, the ra-pidity ofa particle in thenucleon–nucleon center-of-mass frame ( ycm)isdetectedinthelaboratoryframe( ylab)withashift, ylab=
ycm+
0.
465.ThepPb particleyieldsreportedinthisLetterarepre-sentedintermsof ycm,ratherthan ylab,forbettercorrespondence
withtheresultsfromthepp andPbPb collisions.
3. Selectionofeventsandtracks
The triggers, eventreconstruction,andeventselection are the sameasthosediscussedforpp,pPb,andPbPb collisionsinRefs.[8, 41]. Theyare briefly outlined inthe following paragraphs for pp andpPb collisions,whicharethemainfocusofthisLetter.A sub-setofperipheralPbPb datacollectedin2011withaminimum-bias triggerisreprocessedusingthesameeventselectionandtrack re-construction algorithmasforthepresentpPb andpp analyses,in order to more directly compare the three systems at the same multiplicity. Details of the 2011 PbPb analysis can be found in Refs.[41,42].
Minimum-bias pPb events are triggered by requiring at least one trackwith pT
>
0.
4GeV tobe found inthepixeltracker.Be-cause of hardware limitations in the data acquisition rate, only a small fraction
(
∼
10−3)
of triggered minimum-bias events are recorded.Inordertocollectalargesampleofhigh-multiplicitypPb collisions,adedicatedhigh-multiplicitytriggerisimplemented us-ingtheCMSLevel-1(L1)andhigh-leveltrigger(HLT)systems[43]. AtL1,thetotaltransverseenergysummedovertheECALandHCAL isrequiredtoexceedeither20or40GeV,dependingonthe mul-tiplicityrequirementasspecified below.Charged particlesare re-constructedattheHLTlevelusingthepixeldetectors.Itisrequired that these tracks originate within a cylindrical region (30 cm in length along thedirectionofthe beamaxisand0.
2 cm in radius inthedirectionperpendicularto thataxis)centered onthe nom-inalinteraction point. Foreach event,the numberofpixel tracks (Nonlinetrk ) with
|
η
|
<
2.
4 and pT>
0.
4GeV isdetermined for eachreconstructed vertex. Only tracks with a distance of closest ap-proach0
.
4 cm orlesstooneoftheverticesareincluded.TheHLT selectionrequiresNonlinetrk forthevertexwiththelargestnumberof tracks to exceeda specific value. Data are collected in pPb colli-sionswiththresholds Nonlinetrk
>
100 and130foreventswithanL1transverseenergythresholdof20GeV,and Nonlinetrk
>
160 and190 forevents withan L1thresholdof 40GeV. Whileall eventswith Nonlinetrk
>
190 areaccepted,onlyafractionoftheeventsfromtheotherthresholdsareretained.Thisfractionisdependentonthe in-stantaneous luminosity.Datafromboththeminimum-biastrigger and the high-multiplicitytrigger are retained foroffline analysis. Similar high-multiplicity triggers, with differentthresholds, were developedforpp collisions,withdetailsgiveninRef.[8].
The CMS Collaboration / Physics Letters B 768 (2017) 103–129 105
In the subsequent analysis of all collision systems, hadronic eventsare selectedby requiring thepresence ofatleast one en-ergydepositlargerthan3GeV ineachofthetwoHFcalorimeters. Eventsarealsorequiredtocontainaprimaryvertexwithin 15 cm ofthenominalinteractionpointalong thebeamaxisand0
.
15 cm in the transverse direction, where the primary vertex is the re-constructedvertexwiththelargesttrackmultiplicity.Atleasttwo reconstructed tracks are required to be associated with this pri-maryvertex,acondition thatisimportantonlyforminimum-bias events.Beam-relatedbackgroundissuppressedbyrejectingevents inwhichlessthan25%ofallreconstructedtrackssatisfythe high-purityselectiondefinedinRef.[38].InthepPb datasample,there is a 3% probability to haveat least one additional interaction in the same bunch crossing (pileup). The procedure used to reject pileupeventsinpPb collisionsisdescribedinRef.[41].Itisbased onthenumberoftracksassociatedwitheachreconstructedvertex andthe distancebetweendifferentvertices.Apurityof99.8%for single pPb collision events is achieved for the highest multiplic-itypPb range studiedin thisLetter. Forthepp data, theaverage numberofcollisionsper bunchcrossingis1.2.However,pp inter-actions thatare well separated fromeach other do not interfere. Thus,amongeventsidentifiedascontainingpileup,theeventis re-tainediftheseparationbetweentheprimaryvertexandanyother vertexexceeds 1 cm.Insuch events,onlytracksfromthehighest multiplicityvertexareused.Withtheabovecriteria,97%(98%)ofthesimulatedpPb events generatedwith the epos lhc [44] (hijing 2.1 [45]) programs are selected.Similarly,94% (96%)ofthepp eventssimulatedwiththe pythia6Tune Z2[46] (pythia 8Tune4C [47]) programs are se-lected.
Theevent-by-event charged-particle multiplicity Ntrkoffline is de-finedusingprimary tracks,i.e., tracksthat satisfy thehigh-purity criteria of Ref. [38] and, in addition, the following criteria de-signed to improve track quality and ensure the tracks emanate fromtheprimaryvertex.Theimpactparametersignificanceofthe trackwithrespecttotheprimaryvertexinthedirectionalongthe beamaxis,dz
/
σ
(
dz)
,is requiredto be lessthan 3,asis thecor-responding impact parameter in the transverse plane, dT
/
σ
(
dT)
.Therelative pT uncertainty,
σ
(
pT)/
pT,must belessthan 10%.Toensure high tracking efficiency and to reduce the rate of mis-reconstructed tracks, the tracks are required to satisfy
|
η
|
<
2.
4 and pT>
0.
4GeV. Based on simulated samples generated withthe hijing program, the efficiency for primary track reconstruc-tion is found to be greater than 80% for charged particles with pT
>
0.
6GeV and|
η
|
<
2.
4.For the multiplicity rangestudied inthisLetter, nodependenceofthe trackingefficiencyon multiplic-ityisfoundandtherateofmisreconstructedtracksis1–2%.
Thepp, pPb, andPbPb dataare divided intoclasses basedon Nofflinetrk . The quantity Ncorrectedtrk is the corresponding multiplicity corrected for detector and algorithm inefficiencies in the same kinematicregion (
|
η
|
<
2.
4 andpT>
0.
4GeV).The fractionofthetotalmultiplicity found ineach interval and the averagenumber oftracksboth beforeandafteraccountingforthecorrectionsare listedin
Table 1
forthe pp dataandinRef. [41]forthepPb and PbPb data.TheuncertaintyintheaveragevalueNcorrectedtrk is eval-uatedfromtheuncertaintyinthetrackingefficiency,whichis3.9% fora single track[48]. Forthe pp data,six multiplicity intervals, indicatedinTable 1
,aredefined,whichareinclusiveforthelower boundsandexclusivefortheupperbounds,asindicatedinTable 1
. TheaverageNtrkofflinevalueofminimum-biaseventsissimilartothat forthemultiplicity rangeNofflinetrk<
35.ForthepPb andPbPb data, eightintervalsaredefined.Theseeightintervalsareindicated,e.g., inthe legend ofFig. 2.Note that, unlike pp and PbPb collisions, Nofflinetrk forpPb collisions isnotdetermined inthe center-of-mass frame. However, the difference in the Nofflinetrk definition between
Table 1
Fractionof the fullevent sample ineach multiplicity interval and the average multiplicity perintervalfor pp data.Themultiplicities Noffline
trk and Ncorrectedtrk are determinedfor|η|
<
2.4 and pT>0.4GeV beforeandafterefficiencycorrections, respectively.Thethirdandfourthcolumnslistthe averagevaluesofNofflinetrk and Ncorrectedtrk .
Multiplicity interval (Noffline
trk ) Fraction Noffline trk Ncorrected trk [0,35) 0.93 12 14±1 [35,60) 0.06 43 50±2 [60,90) 6×10−3 68 79±3 [90,110) 2×10−4 97 112±4 [110,130) 1×10−5 116 135±5 [130,∞) 7×10−7 137 158±6
thelaboratoryandthecenter-of-massframesisfoundtobe min-imal andso thisdifferenceisignored. Thedetectorcondition has beencheckedtobestableforeventswithdifferentmultiplicities.
4. TheK0
S,
,and
−reconstructionandyields
ThereconstructionandselectionproceduresforK0S,
,and
− candidatesarepresentedinRefs.[30,49].Toincreasetheefficiency for trackswith low momenta andlarge impact parameters, both characteristicofthestrange-particledecayproducts,theloose se-lection of tracks, asdefined in Ref. [38], is used. The K0
S and
candidates(generically referred toas“V0s”) arereconstructed,by
combiningoppositelychargedparticlestodefine asecondary ver-tex.Eachofthetwotracksmusthavehitsinatleastfourlayersof thesilicontracker,andtransverseandlongitudinalimpact parame-tersignificanceswithrespecttotheprimaryvertexgreaterthan1. Thedistanceofclosestapproachofthepairoftrackstoeachother is required to be less than 0
.
5 cm. The fitted three-dimensional vertex of the pair of tracks is required to have aχ
2 valuedi-vided by thenumber of degreesoffreedom lessthan 7.Each of thetwo tracksis assumedtobe apioninthe caseoftheK0
S
re-construction. As the proton carries nearly all of the momentum in the
decay, the higher-momentum trackis assumedto be a protonandtheothertrackapioninthecaseofthe
reconstruc-tion.Toreconstruct
−particles,a
candidateiscombinedwith anadditionalchargedparticlecarryingthecorrectsign,todefinea commonsecondaryvertex.Thisadditionaltrackisrequiredtohave hitsinatleastfourlayersofthesilicontracker,andboththe trans-verseandlongitudinalimpactparametersignificanceswithrespect totheprimaryvertexarerequiredtoexceed 3.
Due to the long lifetime of the K0
S and
particles, the
sig-nificance of the V0 decay length, whichis the three-dimensional
distancebetweentheprimaryandV0verticesdividedbyits uncer-tainty,isrequiredtoexceed5.ToremoveK0
S candidates
misiden-tified as
particles and vice versa, the
(K0S) candidate mass assuming both tracksto be pions(the lower-momentumtrackto beapionandthehigher-momentumtrackaproton)mustdifferby morethan 20
(
10)
MeV fromthe nominal[50]K0S()massvalue. To remove photon conversions to an electron–positron pair, the massofaK0Sor
candidateassumingbothtrackstohavethe elec-tron massmust exceed15MeV. The angle
θ
point betweenthe V0 momentumvector andthevectorconnectingtheprimary andV0 vertices is requiredto satisfy cosθ
point>
0.
999.This reduces the contributions ofparticlesfromnuclearinteractions, random com-binationsoftracks,andsecondaryparticlesoriginatingfromthe weakdecaysof
and
particles.
To optimize the reconstruction of
− particles, requirements onthethree-dimensionalimpactparametersignificanceofits de-cay productswithrespectto theprimary vertexare applied.This significancemustbe largerthan3 (4)fortheproton(pion)tracks
Fig. 1. InvariantmassdistributionofK0
S(left),
(middle),and
−(right)candidatesinthepTrange1–3GeV for220≤Nofflinetrk <260 inpPb collisions.Theinclusionof thecharge-conjugatestatesisimpliedfor
and
−particles.Thesolidlinesshowtheresultsoffitsdescribedinthetext.Thedashedlinesindicatethefittedbackground component.
from the
decay, and larger than 5 for the direct pion candi-datefrom the
− decay. Tofurther reduce thebackground from randomcombinationsoftracks,thecorresponding impact param-etersignificance of
− candidates cannot exceed 2.5. The three-dimensionaldecaylengthsignificance,withrespecttotheprimary vertex,ofthe
− candidateandtheassociated
candidatemust exceed3and12,respectively.
The K0
S,
, and
− reconstruction efficiencies are about 15,
5, and 0.7% for pT
≈
1GeV, and 20, 10, and2% for pT>
3GeV,averaged over
|
η
|
<
2.
4. These efficiencies account for the ef-fectsof acceptance,and forthe branching fractions of the decay modes in which the strange particles are reconstructed. The in-variantmassdistributions ofreconstructedK0S,, and
− candi-dateswith1
<
pT<
3GeV areshowninFig. 1
forpPb eventswith220
≤
Nofflinetrk<
260.Prominentmasspeaksare visible,withlittle background.Thesolidlines showtheresultofamaximum likeli-hoodfit.Inthisfit,thestrange-particlepeaksaremodeled asthe sumoftwoGaussian functionswithacommonmean.The “aver-ageσ
”valuesinFig. 1
arethesquarerootoftheweightedaverage ofthevariancesofthetwoGaussian functions.Thebackgroundis modeledwithaquadraticfunctionfortheK0Sresults,withthe ana-lyticformAq1/2+
Bq3/2withq=
m− (
mπ+
mp)
fortheresults,
andwiththeformCqDwithq
=
m−(
m+
mπ)
forthe−results,
whereA,B,C ,andD arefittedparameters.Thesefitfunctionsare foundtoprovideagooddescriptionofthesignalandbackground with relatively few free parameters. The fits are performedover therangesof strange-particleinvariant massesindicatedin
Fig. 1
toobtaintherawstrange-particleyields Nraw K0
S//−
.
Therawstrange-particleyieldsarecorrectedtoaccountforthe branching fraction ofthe reconstructed decay mode, and forthe acceptanceandreconstructionefficiencyofthestrangeparticle, us-ing simulatedeventsamplesbased on the pythia 6(pp) or epos (pPb and PbPb)eventgeneratorand Geant4 modeling ofthe de-tector: Ncorr K0 S//−
=
Nraw K0 S//− Rcorr,
(1)where Rcorr is a correction factor from simulation given by the
ratiooftherawreconstructedyieldtothetotalgeneratedyieldfor therespectivestrangeparticle,withNcorr
K0 S//−
thecorrectedyield. Theraw
particleyieldincludescontributionsfromthedecays of
− and
particles. This “nonprompt” contribution is largely determined by the relative
− to
yield (because the contri-butionfrom
particlesis negligible).Thestringentrequirements placed on cos
θ
point remove a large fraction ofthe nonpromptcomponentbut, fromsimulation, up to 10% of the
candidates
at high pT are nonprompt.If the relative
− to
yieldin
sim-ulation is modeled precisely, the contamination from nonprompt
particleswillberemovedbythecorrectionprocedureofEq.(1). Otherwise,anadditionalcorrectiontoaccountfortheresidual con-tamination is necessary. As the
− particle yields are explicitly measured in this analysis, this residual correction factor can be determineddirectlyfromthedataas:
f,residualnp
=
1+
f,rawnp,MC Ncorr−/
Ncorr NMC−/
NMC−
1,
(2)where f,rawnp,MC denotes the fractionof nonprompt
particles in the raw reconstructed
sample asdetermined fromsimulation, while Ncorr−
/
Ncorr and NMC −
/
NMC
are the
−-to-
yield ratios
from thedata afterapplying thecorrectionsof Eq.(1),andfrom generator-level simulation, respectively. The final prompt
par-ticle yield is given by Ncorr
/
f,residualnp . Based on epos MC studies, which has a similar−/
ratio to the data, the residual non-prompt contributions to the
yields are found to be negligible in pPb and PbPb collisions, while in pp collisions the correction is 1–3% depending on the pT value of the
particle. Note that Ncorr
inEq.(2)isderivedusingEq.(1),whichinprinciplecontains
theresidualnonprompt
contributions.Nonetheless,byapplying Eq.(2) inan iterativefashion, we expect Ncorr to approacha re-sultcorresponding toprompt
particles only.Asecond iteration ofcorrectionisfoundtohaveaneffectoflessthan0.1%onthe
particle yield.As a cross-checkwe treat the sample ofsimulated eventsgeneratedwiththeHIJINGprogramlikedataandverifythat we obtain thecorrectyields atthe generatorlevel afterapplying thecorrectionproceduredescribedabove.
5. Systematicuncertainties
Table 2 summarizes thedifferentsources ofsystematic uncer-tainty intheyieldsofeach strangeparticlespecies. Thevaluesin parenthesescorrespondtothesystematicuncertaintiesinthe for-ward rapidity regions (
−
2.
4<
ycm<
−
1.
5 and 0.
8<
ycm<
1.
5)for pPb data, ifthey differfromthose atmid-rapidity. The dom-inant sources of systematic uncertainty are associated with the strange-particlereconstruction,especiallytheefficiency determina-tion.
The systematicuncertainty in determining the efficiency of a single track is 3.9% [48]. The tracking efficiency is strongly cor-related with the lifetime of a particle because when and where a particle decaysdetermine how efficientlythe detectorcaptures its decayproducts. Weobserve agreementofthe K0S lifetime dis-tribution (c
τ
) betweendataandsimulation,andsimilarly fortheThe CMS Collaboration / Physics Letters B 768 (2017) 103–129 107
Table 2
SummaryofsystematicuncertaintiesforthepTspectraofKS0,
,and
−particlesinthecenter-of-massrapidityrange |ycm|<1.0 (forpPb events,atforwardrapidities,ifdifferent)forthethreecollisionsystems.
Source K0 S(%) (%) −(%) pT(GeV) <1.5 >1.5 <1.5 >1.5 Single-track efficiency 7.8 7.8 7.8 7.8 11.7 Yield extraction 2 (3) 2 (3) 2 (4) 2 (4) 3 Selection criteria 3.6 (3.6) 2.2 (3.6) 3.6 (6.4) 2.2 (6.4) 7 Momentum resolution 2 2 2 2 2 Nonpromptcorrection 2 2 Pileup (pp only) 3 1 3 1 3
Proton direction (pPb only) 3 (3) 3 (3) 3 (5) 3 (5) 4
Rapidity binning 1 (2) 1 (2) 1 (3) 1 (3) 2
Efficiency correction 5
Total (pp) 9.6 8.7 9.8 8.9 15.4
Total (pPb) 9.6 (10.0) 9.2 (10.0) 9.8 (12.6) 9.4 (12.6) 15.6
Total (PbPb) 9.1 8.6 9.3 8.9 15.1
and
−,whichprovidesacross-check ofthesystematic uncer-tainty.Thistranslatesinto a systematicuncertaintyin the recon-structionefficiencyof7.8% forthe K0S and
particles,and11.7% forthe
−particles.Differentbackgroundfitfunctionsand meth-ods to extract the yields for the KS0,
, and
− are compared. The background fit function is varied to a fourth-order polyno-mialfortheK0S and
studies,andtoalinearfunctionforthe
− study.Theyields areobtainedbyintegratingover aregionthatis
±
5timestheaverageresolutionandcenteredatthemean,rather thanoverthe entirefittedmass range.Possible contamination by residualmisidentified V0 candidates(i.e.,a K0S particle
misidenti-fiedasa
particle, orvice versa) isinvestigatedby varying the invariant mass range used to reject misidentified V0 candidates. Onthe basis of thesestudies we assign systematicuncertainties of2–4% to the yields. Systematic effects related to the selection ofthestrange-particlecandidatesareevaluatedbyvaryingthe se-lectioncriteria,resultinginanuncertaintyof1–7%.Theimpactof finitemomentumresolutiononthespectraisestimatedusingthe eposeventgenerator.Specifically,thegenerator-levelpTspectraof the strange particles are smeared by the momentum resolution, which is determined through comparison of the generator-level andmatched reconstructed-level particle information. The differ-ence betweenthe smeared and original spectra is less than 2%. Thesystematic uncertaintyassociated withnonprompt
correc-tions to the
spectra is evaluated through propagation of the systematic uncertainty in the Ncorr−
/
Ncorr ratio in Eq. (2) to thefresidual
,np factor,andisfoundto belessthan2%.Systematic
uncer-taintiesintroduced bypossibleresidual pileupeffectsforpp data are estimated to be 1–3%. This uncertainty is evaluated through bothtightening(only onereconstructedvertexallowedperevent) andloosening (no eventrejectionon the basis ofthe numberof vertices)thepileuprejectioncriteria[41].Theuncertainty associ-atedwithpileupisnegligibleforthepPb andPbPb datasincethere arevery feweventsinthose sampleswithmore thanone recon-structed vertex. In pPb collisions, the direction of the p and Pb beamswerereversedduringcourseofthedatacollection,as men-tioned in Section 2. Comparison of the particle pT spectra with
andwithoutthe beamreversalyields an uncertaintyof 2–5%for all particletypes. The effectof the choice ofthe rapidity bins is assessedbydividingeachbinintotwo,therebydoublingthe num-berof bins,resultingin a systematicuncertaintyof1–3% forthe pT spectra.Forthe
−,the reconstructionefficiencycorrectionis
smoothedby averaging adjacent bins inorder tocompensate for thelimitedstatisticalprecisionoftheMCsample.Variationsinthe smoothingprocedureleadtoasystematicuncertaintyof5%forthe pTspectraofthe
−.
All sources of systematic uncertainty are uncorrelated and summedinquadraturetodefinethetotalsystematicuncertainties inthe pTspectraofeachstrangeparticle.Thetotalsystematic
un-certaintiesbetweenthepp,pPb,andPbPb systemsaresimilarand largelycorrelated.When calculatingratiosofparticleyields,most ofthesystematicuncertaintiespartiallyorentirelycancel.For ex-ample,thesystematicuncertaintiesduetotrackingefficiencyand pileupforthe
/2K0S ratioarenegligible.
6. Results
6.1. Multiplicitydependenceatmid-rapidity
The pT spectra of K0S,
, and
− particles with
|
ycm|
<
1 inpp collisions at
√
s=
7TeV (top),pPb collisionsat√
s=
5.
02TeV (middle),andPbPb collisionsat√
sN N=
2.
76TeV (bottom)arepre-sentedin
Fig. 2
,fordifferentmultiplicity intervals. Duetodetails in the implementation of the dedicated high-multiplicity trigger thresholdsused toselectthe pp events,themultiplicity intervals forpp eventsdiffer slightlyfromthosefor pPb andPbPb events. The pTdifferential yieldisdefinedasdN2/(
2π
pT)
dpTd y.Forthepurposeofbetter visibility,the dataare scaledby factors of2−n,
as indicated in the figure legend. A clear evolution of the spec-tral shapewithmultiplicity can be seenforeach particle species ineach collision system. Forhighermultiplicity events,the spec-tratendtobecomeflatter(i.e.,“harder”),indicatingalarger
KETvalue.Withineachcollisionsystem,heavierparticles(e.g.,
−) ex-hibit a harder spectrum than lighter particles (K0S), especially for high-multiplicityevents.
To examine the differences in the multiplicity dependence of the spectra in greater detail, the ratios
/2K0
S and
−/
of the
yields areshownin
Fig. 3
asa functionof pT fordifferentmulti-plicityrangesinthepp,pPb,andPbPb systems.Theresultsforthe
/2K0
S ratioare showninFig. 3(top).For pT
2GeV,the/2K0S
ratioisseentobesmallerinhigh-multiplicityeventsthanin low-multiplicity eventsforagiven pT value.In pp andpPb collisions,
thistrendissimilartowhathasbeenobservedbetweenperipheral andcentralPbPb collisions[23];thistrendisnotasevidentforthe PbPb datain Fig. 3 (topright)because inthe presentstudyonly PbPb events of 50–100% centrality are considered. At higher pT,
this multiplicity ordering of the
/2K0S ratio is reversed. In hy-drodynamic modelssuch asthose presentedinRefs. [51,52],this behaviorcanbeinterpretedastheeffectofradialflow.Astronger radialflowisdevelopedinhigher-multiplicityevents,whichboosts heavierparticles(e.g.,
) tohigher pT,resultingina suppression
ofthe
/2K0S ratioatlow pT.Comparingthevariouscollision
low-Fig. 2. ThepTspectraofK0S,
,and
−particlesinthecenter-of-massrapidityrange|ycm|<1 inpp collisionsat√s=7TeV (top),pPb collisionsat√s=5.02TeV (middle), andPbPb collisionsat√sN N=2.76TeV (bottom)fordifferentmultiplicityintervals.Theinclusionofthecharge-conjugatestatesisimpliedfor
and
−particles.The
datainthedifferentmultiplicityintervalsarescaledbyfactorsof2−nforbettervisibility.Thestatisticaluncertaintiesaresmallerthanthemarkersandthesystematic
uncertaintiesarenotshown.
andhigh-multiplicity eventsisseen tobelargestforthepp data. Inthehydrodynamic modelofRef. [31],smallercollisionsystems likepp producealargerradial-floweffectthanlargersystemslike pPb or PbPb, for similar multiplicities, which could explain this observation.ForpT
>
2GeV,thebaryonenhancementcouldbeex-plainedbyrecombinationmodels,inwhichfreequarksrecombine to form hadrons [53]. In previous studies (e.g., Ref. [54]), it has beenshownthat theaverage pT value ofvariousparticle species
hasonlya slightcenter-of-massenergydependence(10% athigh multiplicity).Thisdependenceisnot sufficientto explainthe dif-ferencesobservedin
Fig. 3
betweenthevarioussystems.Foreach multiplicity interval,the
/2K0S ratio reachesa max-imum that has a similar value for all three collision processes, and then decreases at higher pT. The location of the maximum
increaseswithmultiplicityfromaround pT
=
2 to 3GeV.The results forthe
−/
ratio are shown in Fig. 3 (bottom). Inthiscase,thedifferencebetweenthelow- andhigh-multiplicity eventsismuchsmallerthanforthe
/2K0S ratio,forallthree col-lisionssystems.Forallsystems,the
−/
ratioincreaseswithpT
andreachesaplateauataround pT
=
3GeV.Duetothelargesys-tematic uncertainty, it isnot possibleto draw a conclusion with respecttotheradial-flowinterpretation.
Motivatedby thehydrodynamicmodel,weperforma simulta-neous fit of a blast-wave function [32] to the K0S and
spectra in Fig. 2. The fits are restricted to low pT because that is the
region in which the blast-wave model is valid. The blast-wave model is strictly appropriate only fordirectly produced particles, while about1/3 oftheK0S mesonsmaybe fromhighermass res-onances [55]. The
− particle isnot used in thefit asthere are not many
−atlow pT.Thefitsareperformedforeach collision
systemseparately.Thefitrangesare0
.
1<
pT<
1.
5GeV fortheK0Sand0
.
6<
pT<
3.
0GeV forthe.Thefittedfunctionis: 1 pT dN dpT
∼
R 0 r dr mTI0 pTsinhρ
TkinK1 mTcosh
ρ
Tkin,
(3)where
ρ
=
tanh−1β
T=
tanh−1β
s(
r/
R)
nis the velocity profile, R is the radius of the medium (set to unity in the fit), r is the radial distancefrom the centerof the medium in the transverse plane,n istheexponentofthevelocityprofile,
β
TisthetransverseThe CMS Collaboration / Physics Letters B 768 (2017) 103–129 109
Fig. 3. RatiosofpTspectrafor
/2KS0(top)and
−/(bottom)inthecenter-of-massrapidityrange|ycm|
<
1.0 forpp collisionsat√s=7TeV (left),pPb collisionsat √s=5.02TeV (middle),andPbPb collisionsat√sN N=2.76TeV (right).Two(forpp)orthree(forpPb andPbPb)representativemultiplicityintervalsarepresented.The
inclusionofthecharge-conjugatestatesisimpliedfor
and
− particles.Theerrorbarsrepresentthestatisticaluncertainties,whiletheboxesindicatethesystematic uncertainties.
expansionvelocity (also known asthe radial-flow velocity),
β
s is thetransverse expansion velocity on the surface of the medium, Tkin isthekineticfreeze-outtemperature,andI0andK1 aremod-ifiedBesselfunctions.Thefittedparametersthatgoverntheshape aren,
β
s,andTkin.Inthe blast-wave model,common values of Tkin andaverage
radial-flow velocity
β
T are assumed for all particle species, asisexpected ifthe systemis locally thermalizedand undergoes a radial-flowexpansion.Itisusefultodirectlycomparetheextracted values of Tkin and
β
T fromthe different systems to study thesystem-sizedependenceatsimilarmultiplicities.
TheextractedvaluesofTkinand
β
TareshowninFig. 4
forthesixpp andfortheeightpPb andPbPb multiplicityintervals.Inthis figure,themultiplicityincreasesfromlefttoright.Theellipses cor-respondtoone standard deviationstatisticaluncertainties, which forpp collisionsaresmalleratlowandhighmultiplicityduetothe useofevents collected withminimumbias andhigh-multiplicity triggers. Systematicuncertainties, which are evaluated by propa-gatingthe systematicuncertaintiesfromthe spectratothe blast-wave fits and altering the fit ranges, are on the order of a few percentandarenotshown.Examplesofthefitsareshownin
Fig. 5
foralow- andhigh-multiplicityrangeinpPb collisions.Ingeneral, thefit quality is goodfor high-multiplicity eventsexcept forthe lowest pT range,while for low-multiplicityevents there are
dis-crepanciesontheorderof5%.However,thediscrepanciesbetween thefitanddataliewithinthesystematicuncertainty.
Theprecisemeaningofthe Tkin and
β
Tparametersismodeldependent,andthey shouldnot beinterpreted literallyasthe ki-netic freeze-out temperature andradial-flow velocity of the sys-tem. The mainpurpose ofFig. 4 is toprovide a qualitative com-parisonofthespectralshapesinthethreesystems.Inthecontext
Fig. 4. Theextractedkineticfreeze-outtemperature,Tkin,versustheaverage radial-flowvelocity,βT,fromasimultaneousblast-wavefittotheK0Sand
pTspectra at|ycm|<1 fordifferentmultiplicityintervalsinpp,pPb,andPbPb collisions.The sixpp andeightpPb andPbPb multiplicityintervalsareindicatedinthelegendof Fig. 2.Fortheresultsinthisplot,themultiplicityincreasesfromlefttoright.The correlationellipsesrepresentthestatisticaluncertainties.Systematicuncertainties, whichareevaluatedtobeontheorderofafewpercent,arenotshown.
oftheblast-wavemodel,whencomparingatsimilarmultiplicities, theTkinparameterhasthesamevaluewithin15%amongthethree
systems, while the
β
T parameter is larger when the system issmaller, i.e.,
β
Tpp>
β
TpPb>
β
TPbPb. Thisis qualitativelycon-sistent withthe predictionofRef. [31].The results ofblast-wave fitsare knowntodependontheparticlespecies. Duetothe lim-ited setofparticlesinthisanalysis,futurestudieswillbe needed tofurthersubstantiatetheconclusions.
Theevolution ofthe pT spectra withmultiplicity canbe
com-paredmoredirectlybetweenthethreesystemsthrough examina-tion ofthe
KET value. The KETvalues at|
ycm|
<
1 for K0S,,
Fig. 5. Examplesofsimultaneousblast-wavefitsofthepTspectraofKS0and
particlesinlow- andhigh-multiplicitypPb events.Theinclusionofthecharge-conjugatestates isimpliedfor
particles.TheratiosofthefitstothedataasafunctionofpTareshowninthebottompanels.Theuncertaintiesarestatisticalonlyandaretoosmalltobe visibleformostofthepoints.
Fig. 6. Theaveragetransversekineticenergy,KET,at|ycm|<1 forK0S,
,and
− particlesasafunctionofmultiplicityinpp,pPb,andPbPb collisions.Theinclusionof thecharge-conjugatestatesisimpliedfor
and
−particles.Forthe
−,onlyresultsfrompPb collisionsareshown.Theerrorbarsrepresentthestatisticaluncertainties, whiletheboxesindicatethesystematicuncertainties.
and
− particlesasafunctionofmultiplicityareshownin
Fig. 6
. Extrapolation ofthe pT spectra down to pT=
0GeV is a crucialstepinextractingthe
KETvalues,whiletheimpactoftheextrap-olationupto pT
≈ ∞
isnegligible,bothonthevalueofKETandits uncertainty.Forthe
− particle,onlyresultsin pPb collisions are shown due to the limitation of the low-pT reach in pp and
PbPb collisions,ascan beseen fromFig. 2.Blast-wavefits tothe individual spectra, which only consider the spectrum shape but donot impose anyphysics constraint, areused to obtainthe ex-trapolation.The fractionoftheextrapolatedyieldwithrespectto thetotal yield is about1.2–2.5%forthe K0
S, 5.8–15.1%forthe
,
and5.4–20.4% forthe
− particles, depending on the multiplic-ity.Alternativemethods toperform theextrapolationare usedto evaluateasystematicuncertainty,includinguseofthepredictions fromthesimultaneousblast-wavefittotheK0
S and
pT spectra,
anda linear extrapolation fromthe yields ina low range of pT.
Thesystematicuncertaintiesfrom
Table 2
arealsoincludedinthe evaluationoftheKETuncertainties.Forthelowestmultiplicityrange,the
KETvaluesforeachpar-ticlespecies areseen to besimilar. Forall particle species,
KETincreases with increasing multiplicity. However, the slope of the increase differs for different particles, with the heavier particles exhibiting a faster growth in
KET for all systems. For a givenmultiplicity range,the
KETvalue isroughly proportional to theparticle’s mass. In PbPb collisions, this can be understood to be dueto theonsetofradial flow [2,7].The observeddifference be-tween particlespeciesathighmultiplicity isseentobelargerfor pp andpPb eventsthanforPbPb events.Note,however,the differ-enceinthecenter-of-massenergiesbetweenthethreesystems. 6.2. RapiditydependenceinpPb events
The rapidity dependence of the pT spectra of the K0S and
particlesisstudiedinthepPb data.Noresultsfor
−particlesare presentedduetostatisticallimitations.AsapPb collisionis asym-metric in rapidity, it is interesting to compare the spectra along thePb-going( ycm
<
0) andp-going( ycm>
0)directions[37].TheThe CMS Collaboration / Physics Letters B 768 (2017) 103–129 111
Fig. 7. ThepTspectraofK0S and
particlesindifferent ycm rangesfor pPb collisionsat √s=5.02TeV.Theinclusionofthecharge-conjugatestatesisimpliedfor
andparticles.Resultsareshownforthreemultiplicityranges:0≤Noffline
trk <35 (top),120≤N offline
trk <150 (middle),and220≤N offline
trk <260 (bottom).Withineachpanel, thecurvesontoprepresentPb-goingeventsandthecurvesonbottomp-goingevents.Thedatainthedifferentrapidityintervalsarescaledbyfactorsof2−2n forbetter visibility.Thestatisticaluncertaintiesaresmallerthanthemarkersandthesystematicuncertaintiesarenotshown.
pTspectraofK0S and
particlesindifferentycmrangesareshown
in
Fig. 7
forsmall(top),intermediate(middle),andlarge(bottom) averagemultiplicities.The
/2K0S ratios fromthe
−
1.
5<
ycm<
−
0.
8 (Pb-going) and0
.
8<
ycm<
1.
5 (p-going)rapidityregions are comparedinFig. 8
formultiplicity ranges 0
≤
Nofflinetrk<
35 and 220≤
Nofflinetrk<
260. Forboththelow-multiplicityandthehigh-multiplicityevents,the/2K0SratiofromthePb-goingdirectionliesabovetheresultsfrom thep-goingdirection,withthelargestdifferenceobservedathigh pT inthehigh-multiplicitysample.
Asafurtherstudy,wecalculate
KET,followingtheprocedureoutlined inSection 6.1, andexamine its dependence on ycm for
K0S and
particlesinthepPb collisions.Theresultsareshownin
Fig. 8. RatiosofpTspectra,
/2K0S,fromthe−1.5<ycm<−0.8 (Pb-going)and0.8
<
ycm<1.5 (p-going)rapidityregionsinpPb collisionsat√s=5.02TeV.Theinclusion ofthecharge-conjugatestatesisimpliedforparticles.Resultsarepresentedfortwomultiplicityranges0≤Noffline
trk <35 (left)and220≤Ntrkoffline<260 (right).Theerror barsrepresentthestatisticaluncertainties,whiletheboxesindicatethesystematicuncertainties.
Fig. 9. Theaveragetransversekineticenergy,KET,asafunctionofycmfortheK0S and
particlesinthreerangesofmultiplicityinpPb collisionsat √
s=5.02TeV.The inclusionofthecharge-conjugatestatesisimpliedfor
particles.Theerrorbarsrepresentthestatisticaluncertainties,whiletheboxesindicatethesystematicuncertainties.
arelarge,the
KETvaluesareseentobecomeslightlyasymmetricasmultiplicity increases. At low multiplicities (0
≤
Nofflinetrk<
35), theratiosofKETbetweenthePb-goingside(−
1.
5<
ycm<
−
0.
8)andthep-going side(0
.
8<
ycm<
1.
5) are 1.
01±
0.
01 (syst.) forK0
S particlesand1
.
04±
0.
05 (syst.)forparticles,both ofwhich
areconsistentwithunitywithin thesystematicuncertainties (the statistical uncertainties are negligible). However, in the highest multiplicity range,220
≤
Nofflinetrk<
260,theratios become 1.
06±
0.
01 (syst.)forK0S particlesand1.
12±
0.
06 (syst.)forparticles, suggestingthatan asymmetry inKETisdeveloped betweenthe
Pb-going andp-going sides. This trend is qualitatively consistent withthehydrodynamicpredictionforpPb collisions[37].
7. Summary
Measurements of strange hadron (K0S,
+
, and−
+
+) transversemomentumspectrainpp, pPb,andPbPb collisionsare presentedoverawiderangeofeventcharged-particlemultiplicity andparticle rapidity.The studyis basedon samples of pp colli-sionsat√
s=
7TeV,pPb collisionsat√
s=
5.
02TeV,andPbPb col-lisionsat√
sN N=
2.
76TeV,collectedwiththeCMSdetectorattheLHC.Inthecontextofhydrodynamic models,themeasured parti-clespectraarefittedwitha blastwave function,which describes anexpandingfluid-likesystem.Whencomparingatasimilar mul-tiplicity,theextractedradial-flowvelocityparametersarefoundto belargerinpp andpPb collisionsthanthatinPbPb collisions.The averagetransverse kinetic energy
KETof strangehadronsisob-served to increase with multiplicity,with a strongerincrease for
heavier particles.At similar multiplicities, thedifference in
KETbetweenthestrange-particlespeciesislargerinthesmallerpp and pPb systemsthaninthePbPb system.ForpPb collisions,
KETinthePb-goingdirectionforK0S(
+
)is6%(12%)largerthaninthe p-goingdirectionforeventswiththehighestparticlemultiplicities.Acknowledgements
WecongratulateourcolleaguesintheCERNaccelerator depart-ments for the excellent performance of the LHC and thank the technical andadministrativestaffs atCERNand atother CMS in-stitutes for their contributions to the success of the CMS effort. Inaddition,wegratefullyacknowledgethecomputingcentersand personneloftheWorldwideLHCComputingGridfordeliveringso effectively thecomputinginfrastructure essentialto our analyses. Finally, we acknowledge the enduring support for the construc-tion andoperationofthe LHCandtheCMSdetectorprovided by thefollowingfundingagencies:BMWFWandFWF(Austria);FNRS and FWO (Belgium); CNPq, CAPES, FAPERJ, and FAPESP (Brazil); MES (Bulgaria); CERN; CAS, MoST, and NSFC (China); COLCIEN-CIAS (Colombia); MSES and CSF (Croatia); RPF (Cyprus); MoER, ERC IUT andERDF (Estonia); Academy of Finland, MEC, andHIP (Finland); CEA and CNRS/IN2P3 (France); BMBF, DFG, and HGF (Germany);GSRT(Greece);OTKAandNIH(Hungary);DAEandDST (India);IPM(Iran); SFI(Ireland);INFN (Italy);MSIP andNRF (Re-public ofKorea);LAS(Lithuania);MOE andUM(Malaysia);BUAP, CINVESTAV, CONACYT, LNS, SEP, and UASLP-FAI (Mexico); MBIE (New Zealand); PAEC (Pakistan); MSHE and NSC (Poland); FCT (Portugal); JINR(Dubna); MON,RosAtom, RASandRFBR (Russia);
The CMS Collaboration / Physics Letters B 768 (2017) 103–129 113
MESTD(Serbia); SEIDIandCPAN(Spain); SwissFundingAgencies (Switzerland); MST (Taipei); ThEPCenter, IPST, STAR and NSTDA (Thailand);TUBITAKandTAEK(Turkey);NASUandSFFR(Ukraine); STFC(UnitedKingdom);DOEandNSF(USA).
Individuals have received support from the Marie-Curie pro-gramandtheEuropeanResearchCouncilandEPLANET(European Union); the Leventis Foundation; the A.P. Sloan Foundation; the AlexandervonHumboldt Foundation;theBelgianFederal Science Policy Office; the Fonds pour la Formation à la Recherche dans l’Industrie et dans l’Agriculture (FRIA-Belgium); the Agentschap voor Innovatie door Wetenschap en Technologie (IWT-Belgium); theMinistryofEducation, YouthandSports (MEYS)ofthe Czech Republic;theCouncilofScienceandIndustrialResearch,India;the HOMING PLUSprogram ofthe Foundation forPolish Science, co-financed from European Union, Regional Development Fund; the MobilityPlusprogramoftheMinistryofScienceandHigher Edu-cation(Poland);theOPUSprogramoftheNationalScienceCenter (Poland);the Thalis andAristeia programs cofinancedby EU-ESF andtheGreek NSRF;the NationalPrioritiesResearch Programby Qatar National Research Fund; the Programa Clarín-COFUND del Principado de Asturias; the Rachadapisek Sompot Fund for Post-doctoralFellowship,ChulalongkornUniversity(Thailand);the Chu-lalongkorn Academic into Its 2nd Century Project Advancement Project(Thailand);andtheWelchFoundation,contractC-1845.
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M. Van De Klundert,
H. Van Haevermaet,
P. Van Mechelen,
N. Van Remortel,
A. Van Spilbeeck
UniversiteitAntwerpen,Antwerpen,BelgiumS. Abu Zeid,
F. Blekman,
J. D’Hondt,
N. Daci,
I. De Bruyn,
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C. Caillol,
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M. Musich,
C. Nuttens,
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L. Quertenmont,
M. Selvaggi,
M. Vidal Marono,
S. Wertz
UniversitéCatholiquedeLouvain,Louvain-la-Neuve,Belgium
N. Beliy,
G.H. Hammad
UniversitédeMons,Mons,Belgium
W.L. Aldá Júnior,
F.L. Alves,
G.A. Alves,
L. Brito,
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M. Hamer,
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4,
A. Vilela Pereira
UniversidadedoEstadodoRiodeJaneiro,RiodeJaneiro,BrazilS. Ahuja
a,
C.A. Bernardes
b,
A. De Souza Santos
b,
S. Dogra
a,
T.R. Fernandez Perez Tomei
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E.M. Gregores
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P.G. Mercadante
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C.S. Moon
a,
5,
S.F. Novaes
a,
Sandra S. Padula
a,
D. Romero Abad
b,
J.C. Ruiz Vargas
aUniversidadeEstadualPaulista,SãoPaulo,Brazil bUniversidadeFederaldoABC,SãoPaulo,Brazil
A. Aleksandrov,
R. Hadjiiska,
P. Iaydjiev,
M. Rodozov,
S. Stoykova,
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M. Vutova
InstituteforNuclearResearchandNuclearEnergy,Sofia,BulgariaA. Dimitrov,
I. Glushkov,
L. Litov,
B. Pavlov,
P. Petkov
UniversityofSofia,Sofia,BulgariaW. Fang
6BeihangUniversity,Beijing,China
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J.G. Bian,
G.M. Chen,
H.S. Chen,
M. Chen,
T. Cheng,
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F. Romeo,
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A. Spiezia,
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Y. Ban,
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S.J. Qian,
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A. Cabrera,
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D. Lelas,
I. Puljak,
P.M. Ribeiro Cipriano
UniversityofSplit,FacultyofElectricalEngineering,MechanicalEngineeringandNavalArchitecture,Split,Croatia
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M. Kovac
UniversityofSplit,FacultyofScience,Split,Croatia
V. Brigljevic,
D. Ferencek,
K. Kadija,
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S. Micanovic,
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M. Kadastik,
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J. Pekkanen,
M. Voutilainen
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V. Karimäki,
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T. Lampén,
K. Lassila-Perini,
S. Lehti,
T. Lindén,
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J. Tuominiemi,
E. Tuovinen,
L. Wendland
HelsinkiInstituteofPhysics,Helsinki,Finland
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T. Tuuva
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F. Couderc,
M. Dejardin,
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B. Fabbro,
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J. Andrea,
A. Aubin,
D. Bloch,
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E.C. Chabert,
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X. Coubez,
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D. Gelé,
U. Goerlach,
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K. Skovpen,
P. Van Hove
InstitutPluridisciplinaireHubertCurien,UniversitédeStrasbourg,UniversitédeHauteAlsaceMulhouse,CNRS/IN2P3,Strasbourg,France
S. Gadrat
CentredeCalculdel’InstitutNationaldePhysiqueNucleaireetdePhysiquedesParticules,CNRS/IN2P3,Villeurbanne,France
S. Beauceron,
C. Bernet,
G. Boudoul,
E. Bouvier,
C.A. Carrillo Montoya,
R. Chierici,
D. Contardo,
B. Courbon,
P. Depasse,
H. El Mamouni,
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M. Gouzevitch,
B. Ille,
F. Lagarde,
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M. Lethuillier,
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J.D. Ruiz Alvarez,
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P. Verdier,
S. Viret
UniversitédeLyon,UniversitéClaudeBernardLyon1,CNRS-IN2P3,InstitutdePhysiqueNucléairedeLyon,Villeurbanne,France