Salvatore Fazio (BNL) on behalf of Matthew Posik(Temple ... · 1 Gas Tracking R&D EIC User Meeting:...
Transcript of Salvatore Fazio (BNL) on behalf of Matthew Posik(Temple ... · 1 Gas Tracking R&D EIC User Meeting:...
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Gas Tracking R&D
EIC User Meeting: Jan 6-9, 2016
Constraining the Sea Quark Distributions Through W± Cross Section Ratio
Measurements at STAR
DIS 2017 University of Birmingham
April 3-7 2017
SalvatoreFazio(BNL) onbehalfofMatthewPosik (TempleUniversity)
STARCollaboration
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Motivation
o PartonDistributionFunctions(PDFs)probetheinternalstructureoftheproton.
o Thex-dependence ofthesePDFsallowyoutodistinguishbetweentheintrinsicpropertiesoftheprotonandQCDradiation.
o Severalglobalanalyses(CT14,MMHT14,BS15,etc.)haveextractedPDFsusingvariousdataandfunctionalfit assumptions.
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non-lineardynamicRegime
110-310-4 10-2 10-1
Few-body/ valence quark
Regime
x(proton)
Many-body Regime
QCD radiationdominated
Regime
10-5
arXiv:1412.3989
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Motivation
o E-866 suggestsatrendwherethedbar/ubar ratioappearstobedecreasingatlarge-x.
o Unpolarizeddbar/ubar distributioncanbeprobedviaDrell-Yanproduction.
B.Kernsetal.(SeaQuest Collaboration),APSAprilMeeting2016.
o Thepreliminary SeaQuest trendappearsleveloutathigherx.Howeverpreliminarydatahavelargeerrorbarsatlarge-x.Stillawaitingfullstatisticalsample.
o Moredirect andindirect dataareneededathigh-x tohelpconstrain theseaquarkdistributions.
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o NewmeasurementsfromdifferentexperimentscanprovidedataatdifferentQ2 andfromdifferentscatteringprocesses.
§ Thiswillallowfordifferentsystematiceffects andalsoserveasacrosscheckofourunderstandingofthephysics.
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W Boson Production Through p+p Collisions
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�W+
�W�=
✓N+
O �N+B
N�O �N�
B
◆✓✏�
✏+
◆ o +/- ispositron/electronfromWleptonicdecayo NO isnumberofobservedWeventso NB isnumberofbackgroundeventso ε isthemeasuredWefficiency
o Wbosonsaresensitive toquark/anti-quarkdistributions.TheycanbeaccessedviatheWleptonicdecaychannelsinproton+protoncollisions
u+ d ! W+ ! e+ + ⌫
d+ u ! W� ! e� + ⌫
Ø
Ø
o ThechargedWcross-sectionratio
Ø isproportionaltothedbar/ubar ratio
Ø canbeusedtoconstrain theseaquarkdistributions
�W+
�W�⇡ u(x1)d(x2) + d(x1)u(x2)
u(x1)d(x2) + d(x1)u(x2)
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Relativistic Heavy Ion Collider
o OverthepastseveralyearsluminosityatRHIChassteadilyincreased
o RHIC istheworld’sfirstpolarizedhadroncollider
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Solenoidal Tracker At RHIC𝛈 =-1 𝛈 =0
𝛈 =1
𝛈 =2
o Calorimetrysystemwith2𝜋 coverageØ Barrelelectromagneticcalorimeter
(BEMC),-1<𝜂 <1Ø Endcapelectromagneticcalorimeter
(EEMC),1.1<𝜂 <2
o Timeprojectionchamber(TPC),|𝜂|<1.3
Year ~Luminosity(pb-1)2011 25(sampled)2012 75(sampled)2013 250(sampled)2017 400(delivered)
Combined 750
o The2017 (transversep+p √s=510GeV)runisexpectedtodeliver~400pb-1 moredata
Productionrunsat√s=500/510GeV
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STAR Kinematics
RHICBOS-CT10pT >25GeV/c
e+/- pseudo-rapidity
x1x2<x>
o ApproximatekinematicrangeatSTARmid-rapidity (TPC+BEMC)
Ø 0.1<x<0.3for-1<𝜂 <1
o Forcollisionenergiesof√s=500GeVand𝜂 =0,(x1 ≈x2)Ø x=MW/√s=0.16
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STAR Kinematics
o ApproximatekinematicrangeatSTARmid-rapidity (TPC+BEMC)
Ø 0.1<x<0.3for-1<𝜂 <1
o Forcollisionenergiesof√s=500GeVand𝜂 =0,(x1 ≈x2)Ø x=MW/√s=0.16
o InSTARtheEEMC couldbeusedtoobtainamoreforwardeta-bin(1.1<𝜂 <2)whichwouldextendthexreachofSTARØ 0.06<x<0.4for-2<𝜂 <2
o AnalysisofthisforwardEEMCeta-biniscurrentlyunderway
RHICBOS-CT10pT >25GeV/c
e+/- pseudo-rapidity
x1x2<x>
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Selecting W Candidates
o Mid-rapiditySTARWselectioncriteria
Ø Isolationratio1/Isolationratio2
Ø pT-balancecut
Ø MatchpT >10GeV/ctracktoBEMCcluster
W+
W-
TPCtrackextrapolatedtoBEMCtowergrid
Ø Leadstogoodchargediscrimination
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Reconstruction W bosons
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TheSTARdetector@RHIC
Ingredientsfortheanalysis• Isolatedelectron• neutrino(notmeasureddirectly)• Hadronic recoil
q SelecteventswiththeW-signature(STEP1)Ø IsolatedhighPT electron
qNeutrinotransversemomentumisreconstructedfrommissingPT(Step2)
qNeutrino’slongitudinalmomentumisreconstructedfromthedecaykinematics(Step3)
€
! P Tν ≈ −
! P T
i
i∈clusterstracks
∑
€
MW2 = Ee + Eν( )2 − ! p e +
! p ν( )2
WbosonmomentumreconstructiontechniquewelltestedatFermiLab andLHC
[CDF:PRD70,032004(2004);ATLAS:JHEP1012(2010)060]
BarrelEMCAL(|η|<1)TPC (|η|<1.4)
FirstdevelopedatSTARforrun11transversesingle-spinasymmetrymeasurementofWbosonsPhys.Rev.Lett.116(2016)
(GeV)T E10 20 30 40 50 60 700
50
100
150
200
250
300
350
400Data Run-12
Total Sum
MCν e →W
Data-Driven QCD
Second EEMC
MCν τ →W
ee MC→Z
Background Contributions+Run-12: W
(GeV)T E10 20 30 40 50 60 700
2040
6080
100
120140
160
180200
220240
Data Run-12Total Sum
MCν e →WData-Driven QCDSecond EEMC
MCν τ →W ee MC→Z
Background Contributions-Run-12: W
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Mid-Rapidity W+/- Backgrounds
o Data-drivenQCDbackgroundssatisfye+/- isolationcuts
o SecondEEMCbackgroundsresultfrombackward(“Jet”)atnon-existingcalorimetercoveragefor-2<<-1.1𝜂
o SecondEEMCbackgroundsareestimatedfromEEMClocatedat1.1<<2𝜂
o Electro-weakbackground fromZdecayisdonewithPYTHIA/MCsimulations.
o SmallbackgroundcontributionfromZdecay.
W+
Run12
W-
Run12
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W+/- Efficiencies (Runs 11 and 12)
Eta-Bin1 2 3 4 5 6 7 8
Effic
ienc
y
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
Run-12
W+ Efficiency
W- Efficiency
Eta-Bin1 2 3 4 5 6 7 8
Effic
ienc
y
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
Run-11
W+ Efficiency
W- Efficiency
Run11 Run12
o 2012 running hadlowerW+/- efficienciesduetohigherluminosityrunning.
o Thisleadstomorepile-upintheTPC,whichresultedinlessefficient trackreconstruction.
o MinimalchargedependenceleadstosmallcontributiontothechargedWcross-sectionratio
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Charged W Cross Section Ratios
Run11+12preliminaryresult (~100pb-1)
o ChargeWcross-sectionratiovs.lepton pseudo-rapidity precisionisdominatedbystatistics.
o Run13shouldaddanother~250pb-1 ofdata
o WhileRun17isprojectedtodeliver~400pb-1
Run11+12Preliminary
𝝶e
W+ /W
-
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Charged W Cross Section Ratios
Run11+12preliminaryresult (~100pb-1)
o TheWbosonrapiditycannowalsobereconstructedatSTARviaitsrecoil.(Neededforrun11transversesingle-spinasymmetrymeasurement,Phys.Rev.Lett.116(2016))
o WorkisongoingtoimprovethesystematicuncertaintyassociatedwiththereconstructedWbosonrapidity.
W+ /W
-
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yW
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STAR Run 13 Statistical Impact
o Run13willsignificantlyimprovethestatisticalprecisionoftheSTARmeasuredW+/W- crosssectionratio.
o FurtherimprovementisexpectedfromRun17p+p 510GeVrun,whichisexpectedtodeliver~400pb-1.
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Run 13 Analysis Update
Ø W+andW- efficienciesforrun13showsimilarbehaviorasthosemeasuredinrun12
1) Run13 recentlyswitchedovertoanewtrackingalgorithmwhichresultedin
Ø Highertrackreconstructionefficiencyatlargeluminosity
2) TheBEMCwascalibratedusingrun13p+p 510GeVdataandisnowappliedtotheongoingrun13analysis(usedinSTAR2013WAL Prelim.ResultsshownatINPCandSPIN2016).
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o TheseanalysisupdateswereincludedintheSTAR2013mid-rapidityWAL preliminaryresultfirstshownatINPCandSPIN2016.
o PreliminaryWAL resultsintheforwardregionwillbeshownatthisconferenceduringthetalkonWed.17:00intheWG6session!
o Overthepastyearorso,therun13datasethashadsomeupdates/calibrationsimplemented.
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W+/- Efficiencies (Run 13)
Eta-Bin-0.8 -0.6 -0.4 -0.2 0 0.2 0.4 0.6 0.8
Effic
ienc
y
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
Run-13 Period 2
W+ Efficiency
W- Efficiency
Eta-Bin-0.8 -0.6 -0.4 -0.2 0 0.2 0.4 0.6 0.8
Effic
ienc
y
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
Run-13 Period 1
W+ Efficiency
W- Efficiency
Run13(Day76-126)
Run13(Day129-161)
o W+andW- efficienciesforrun13showsimilarbehaviorasthosemeasuredinrun12Ø Averageefficiency~50%Ø SmalltonegligibledifferencebetweenW+andW- efficiency
o Efficiencydip seendays129-161isduetoinsertionofanewsubdetector (HFT).
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𝜂 𝜂
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Summaryo STARmeasuredcross-sectionratiousingWproduction
Ø AcomplimentarymeasurementtoSeaQuest andE-866Ø Shouldhelpfurtherconstrain theseaquarkPDFs
o Preliminaryresultsofmeasuredcross-sectionratiosusingRun11and12datasetshavebeenreleasedasafunctionofleptonpseudo-rapidityandWbosonrapidity
o Run13analysisnowtakesadvantageofrecentlyimplemented
o Run13dataset(~250pb-1 )tobeincludedintothecross-sectionratiomeasurementsoon
Ø BarrelelectromagneticcalorimetercalibrationØ Trackingalgorithm
o Long510GeVrunin2017attransversespinpolarizationisexpectedtodeliver400pb-1 whichshouldfurtherimprove thechargedWcross-sectionratioprecision.
o Moreforward eta-bin(1.1– 2.0)lookingtobeaddedtothecrosssectionratioviatheelectromagneticendcap
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