open charm production at
DESCRIPTION
Open Charm Production at. Andrew Glenn University of Tennessee. July 7, 2004. Outline. Motivation (Experimental and Theoretical) Single muon Au+Au analysis Other charm data at PHENIX and STAR Summary and Outlook. Why is Charm Interesting (in A+A)?. Thermal. Pre-thermal. - PowerPoint PPT PresentationTRANSCRIPT
Open Charm ProductionOpen Charm Productionatat . .
Andrew Glenn
University of Tennessee
July 7, 2004
Andrew Glenn2
OutlineOutline
• Motivation (Experimental and Theoretical)
• Single muon Au+Au analysis• Other charm data at PHENIX and STAR
• Summary and Outlook
Andrew Glenn3
Why is Charm Interesting (in A+A)?Why is Charm Interesting (in A+A)?Hadronic
Vs.
QGPCan charm help show the difference?
Pre-thermal
Thermal
Initial production
Andrew Glenn4
d[A+BX] =
ij f
i/Af
j/B d [ijcc+X] D
cH + ...
J.C.Collins,D.E.Soper and G.Sterman, Nucl. Phys. B263, 37(1986)
Factorization theorem for charmed hadron production
fi/A,
fj/B
: distribution fuction for parton i,jD
cH : fragmentation function for c
d [ijcc+X] : parton cross section
+ ... : higher twist (power suppressed by
QCD/m
c, or
QCD/p
t if p
t ≫m
c ) :
e.g. "recombination" PRL, 89 122002 (2002)
Charm production at RHIC is dominated by gluon fusion
Charm ProductionCharm Production
B. L. Combridge et al. Nuc. Phys., B151:429–456, 1979
Andrew Glenn5
Measure Thermalization Time?Measure Thermalization Time?
Initial estimates showed pre-equilibrium charm production to be similar to the initial productionin a QGP at RHIC energy.
Berndt Muller and Xin-Nian Wang. Phys. Rev. Lett., 68:2437–2439, 1992.
Andrew Glenn6
Probably not.Probably not.Refined estimates showed thepost initial production to be small.
Most charm is made via gluon fusion in the initial stage.
Peter L´evai, Berndt Muller, and Xin-Nian Wang. Phys. Rev., C51:3326–3335, 1995.
Zi-wei Lin and M. Gyulassy. Nucl. Phys., A590:495c–498c, 1995.
Andrew Glenn7
Charm Enhancement?Charm Enhancement?
One early interpretation of the NA45 electron pair enhancement was a large charm enhancement
P. Braun-Munzinger, D. Miskowiec, A. Drees, and C. Lourenco. Eur. Phys. J., C1:123–130, 1998.
Andrew Glenn8
Quite Possibly (but less)Quite Possibly (but less)
NA50 Muon pair data showed that charm was not so largely enhanced. BUT there was still a significant excess which may be due to charm enhacement
Open CharmEnhancement ?
M. C. Abreu et al. Eur. Phys. J., C14:443–455, 2000.
Andrew Glenn9
Centrality DependenceCentrality Dependence
Enhancement up to 3.5 in central Pb+Pb
NA50
M. C. Abreu et al. Eur. Phys. J., C14:443–455, 2000.
Andrew Glenn10
HadronizationHadronization
fragmenting parton:ph = z p, z<1
recombining partons:p1+p2=ph
Fragmentation Vs. Coalescence
Quarks can combine with unrelated
Quarks can combine with unrelated quarks. Observed since ’77 as ‘leading particle effect’ (recombination). How much larger of a role might this play at RHIC; especially in a ‘quark soup’ (coalescence).
Andrew Glenn11
Enhancement at RHIC Vs. SPSEnhancement at RHIC Vs. SPS
Estimates show that RHIC will has a lower fraction of c quark pairs below 2mD threshold to contribute to enhancement via coalescence.
This region can’t contributeto open charm throughfragmentation.
Ma
xim
um
En
ha
nc
em
en
t
A. P. Kostyuk, M. I. Gorenstein, and W. Greiner. Phys. Lett., B519:207–211, 2001.
Andrew Glenn12
D RatiosD Ratios
• The ratios of different D mesons will differ in hadron vs. QGP scenario.
• Free relativistic fermion quark gas at T=200 MeV and a baryon chemical potential, µ = 0: D−
s / D− = 0.94
• A equilibrated hadronic bose gas at T=180 MeV: D−
s / D− = 0.610
• Final state interactions such as D± + K± → D±s +
π± could modify the ratios and need to be corrected for.
Cheuk-YinWong. Nucl. Phys., A630:487–498, 1998. and private communication
Andrew Glenn13
Other Information from CharmOther Information from CharmElectrons from charm
Transverse momentum spectra and flow parameters are sensitive to QGP.
V. Greco, C. M. Ko, and R. Rapp. Quark coalescence for charmed mesons in ultrarelativistic heavy-ion collisions. 2003.
Andrew Glenn14
Cronin
Nuclear effects such as shadowing, energy loss, kT broadening, cronin enhancement, and gluon saturation (Color Glass) need to be considered
Nuclear EffectsNuclear Effects
CGC
Shadowing
Dmitri Kharzeev and Kirill Tuchin. hep-ph/0310358, 2003.B. Z. Kopeliovich, J. Nemchik, A. Schafer, and A. V. Tarasov. Phys. Rev. Lett., 88:232303, 2002.R. Vogt. Int. J. Mod. Phys., E12:211–270, 2003.Jens Ole Schmitt et al. Phys.Lett., B498:163–168, 2001.
Andrew Glenn15
Charmonium ReferenceCharmonium ReferenceIn the past, J/ψ production (supression) has been measured relative to Drell-Yan. In order to minimize nuclear effects, such as gluon shadowing, open charm will be a better reference.
SPS/AGSRHIC
J/Psi to DY
Charmonium has a much different production mechanism than Drell-Yan.
J/Psi to Open Charm
H. Satz and K. Sridhar. Phys. Rev., D50:3557–3559, 1994.
Andrew Glenn16
The ApparatusThe ApparatusDetector (Iarocci Tubes)
Steel Absorber
Andrew Glenn17
Run II Au+Au Data SampleRun II Au+Au Data Sample• RHIC Run II Au+Au
(The first muon capable run)• Start With 7.7M Minimum-Bias Events
(Cleanest section of running period)
• Cuts on:• Vertex (-20 to 38cm)
• Track Quality (2/DOF < 7, NTrHits >=12) (-1.51 to -1.79 or = 155 -161o)
Uniform acceptance in event vertex.• Azimuthal Cut
Andrew Glenn18
Run IV Au+AuRun IV Au+Au
• Better Shielding (Tunnel and MuID Hole)
• Better Statistics (~1.5 Billion Min-bias!)
• Better Hardware Acceptance (stable HV..)
Run II
Run III
Andrew Glenn19
Sources of Muon CandidatesSources of Muon Candidates
• D (B) meson semi-leptonic decays(D K …) Prompt Signal
• Decay muons from hadron decays (±± , K±± )
• ‘Hadron’ Punch Through(±, K±, p)
• Decays from J/, , Drell-Yan…(Small Contribution)
PH
MuID
Bac
kgro
un
d
Gap 0 1 2 3 4
Steel absorber
Andrew Glenn20
Muon Identification Muon Identification
Main muon identification is from momentum/depth matchingPHMuID
ste
el
Last Gap = 2Centrality > 20%
Long tail from interacting hadrons(more evidence to come)
Sharp Muon Peak
Data –RedSimulation –Black
Gap (Plain) 0 1 2 3 4
3 GeV
1 GeV
3 GeV
Andrew Glenn21
Run IV Stopping PeaksRun IV Stopping Peaks
Muon Peaks
NorthSouth
Andrew Glenn22
We want to separate the contribution from prompt muon production and /K decays
Collision Point
nosecone
magnet
Muon trackerMuon ID
40 cm
• D c = 0.03 cm Decays before absorber• c = 780 cm Most are absorbed, but some decay first • K c = 371 cm Most are absorbed, but some decay firstγcτ >> 80cm → Decay Probability nearly constant between nosecones
Collisions occurring closer to the absorber will have fewer decay contributions. Should see a linear increase in decay background with increasing vertex.
Decay ContributionDecay Contribution
X
Z
Andrew Glenn23
Vertex DependenceVertex Dependence
=Centrality > 20%
Very Linear Shape Due to Decays
Not due to vertex detector resolution Centrality > 20%
Centrality > 20%
1 < pT > 3 GeV/c
Andrew Glenn24
Interacting Hadron Vertex Interacting Hadron Vertex
Interacting Hadrons: Last Gaps 2 and 3, Pz St3 tail. Flat shape indicates little to no decay (hence muon) component
Last Gap = 2
Centrality > 20%
Centrality > 20%
Andrew Glenn25
From simple (event vertex corrected) subtraction of near muons from far muons
(Hence NOT NORMALIZED, also NOT ACCEPTANCE/EFFICIENCY CORRECTED)
Free Decay pFree Decay pTT Distribution Distribution
Centrality > 20%
Region II – Region I
Z vertex
Muon Vertex
Region I Region II
Decays
prompt decay + punchthrough +??
Z absorber
Scaled
Andrew Glenn26
SimulationsSimulations
• With the availability of BRAHMS and K data at Muon Arm rapidities, we can examine a data driven simulation approach.
• An accurate modeling of K and (and p) production for simulation input is required for punchthrough estimations.
Decays Z dependence, simulation
Punch thoughPz Tails (extrapolation to Gap4), simulations
Promt Signal Simulations for acc*eff
Andrew Glenn27
Data Driven Particle GeneratorData Driven Particle Generator
Use scaled PHENIX central arm data to for basis of event generator. BRAHMS preliminary data helps with scaling and justification ( P(y,pT) ≈ P(y)P(pT) ). Only measurements for 5% most central events are available from BRAHMS.
5% Most Central Events
BRAHMS data extractedfrom Djamel Ouerdane’s thesis
BRAHMS5% most central
Provides scaling
Andrew Glenn28
Early Simulation ResultsEarly Simulation Results• 900K Single K’s and ’s thrown with BRAHMS (preliminary, 5% most
central) pT and dN/dy shapes. pT > 1 GeV required. Passed through full simulation/reconstruction.
Last Gap Reached Reconstructed Decay Muons Reconstructed non-muons
2 161 250
3 297 169
4 712 74
Last Gap = 4Same cut as data
Decays Punchthrough (non-muons)
Projected decay contribution ends at ~-73cm
Last Gap = 4Same cut as data
Andrew Glenn29
Rough Component BreakdownRough Component Breakdown
Free Decays
Other Decays
Prompt muons + unresolved background (combinatoric …)
Punch Through
z=-40cm nose cone
Z=-73cm decay sim.
Andrew Glenn30
Completing the AnalysisCompleting the Analysis
• Complete large statistics simulations to more accurately estimate punch though and background.
• Complete a more accurate estimate of combinatory background.
• Bin analysis in pT to determine prompt muon spectra.
• Finish acceptance*efficiency corrections.
Andrew Glenn31
Green band = systematic uncertainty.Blue dotted line = expectation.
Blue line = statistical uncertainty.
μ -
No absolute value yet; final efforts in progress
Measured decay muons with the expectation
Prompt muons
p+p Muon Open Charmp+p Muon Open Charm
Y. Kwon et. al
Andrew Glenn32
p+p Muon Open Charm IIp+p Muon Open Charm II
Work in progressestimates for backgroundsas a function of pT
Max BG
Min BG
Y. Kwon et. al
Andrew Glenn33
Has J/Has J/ψψ Muon Data Muon Data
Andrew Glenn34
J/J/ψψ Visible in Run IV Au+Au Data Visible in Run IV Au+Au Data
South ArmCentrality >40
Andrew Glenn35
PHENIX PRELIMINARY
Electron MeasurementsElectron Measurements
p+pAu+Au
consistant with binary scaling
Andrew Glenn36
.. Electron Measurements II Electron Measurements II
(e++e–)/2sys. error
Min. bias at Au+Au sNN=200GeV
PHENIX
• Fully corrected spectrum– Acceptance & eID efficiencies– 2.5M and 2.2M events
analyzed with and without the converter
• Backgrounds from KeX (less than 5%) and , , ee (1%) decays subtracted
• Systematic error is 13% at high pT
eID, acc, etc 11.8%K- >eX, VM- >ee 2.0%Signal extraction 5.0%
Andrew Glenn37
Mass plots from dAu data using event-mixing technique
D±
7.4<pt<9.3 GeV/c
D0+D0
0 < pT < 3 GeV/c, |y| < 1.0
d+Au minbias
8.5< pt<11.0 GeV/c
00 DD
STAR has measured charm in d+AuSTAR has measured charm in d+AuQM 2004
STAR also has a single electron charm measurement.
Andrew Glenn38
Summary and OutlookSummary and Outlook• Open (and hidden) charm measurements are
very important to RHIC HI/QGP physics.• PHENIX is capable of making charm
measurements via semileptonic decays (at forward and central rapidity).
• Electron measurments exhist, and muon measurements are close.
• Quicker simulations (using staged cloning) are being tested to aid in estimating punch through.
• Future upgrades may enhance our ability to do these measurements. (displaced vertex detection, pad chambers …)
Andrew Glenn39
Additional Slides
Andrew Glenn40
Peripheral Data Vs SimulationPeripheral Data Vs Simulation
Simulation: Muons From Central Hijing Data: Centrality > 60 (For cleaner events)
Falsely extended tracksLast Gap = 2
Last Gap = 3
Last Gap = 4
No clear peak or tailsince last gap.
Andrew Glenn41
Hadronization AnimationsHadronization Animations
C
U
UCUC