highlights from phenix ii: photons and leptons
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Highlights from PHENIX II: Photons and Leptons. Terry Awes, ORNL For the PHENIX collaboration. Photons and Leptons. Penetrating probes that carry information about their production. Rare processes Need large data samples Large backgrounds Need precise background determination - PowerPoint PPT PresentationTRANSCRIPT
Highlights from PHENIX II:Photons and Leptons
Terry Awes, ORNLFor the PHENIX collaboration
Terry Awes, ORNL - QM08, Jaipur India Slide:2
Photons and Leptons• Penetrating probes that carry
information about their production.
• Rare processes– Need large data samples
• Large backgrounds– Need precise background
determination • Background from decays of and • Electrons from conversions • Combinatorial Backgrounds
• Theme: Towards Higher Accuracy
Terry Awes, ORNL - QM08, Jaipur India Slide:3
• Improved Statistical errors – Au+Au
Statistics: • 30 : 10 : 1 ( Runs 7 : 4 : 2 )
• Improved Systematic errors– More statistics– Two EMCals
More Precise Measurements
arXiv:0801.4020
Au+Au 200 GeV (Run 4)
Terry Awes, ORNL - QM08, Jaipur India Slide:4
Improved p+p Reference Data
• PHENIX 62 GeV p+p cross section approx. 2 times higher than ISR average.
• 200 GeV p+p data 10x (with Run5)
J.Phys.G31:S491 (2005)
p+p 62 GeV (Run 6)
Terry Awes, ORNL - QM08, Jaipur India Slide:5
Nuclear Suppression Dependence on:
Cu+Cu 22,62,200 GeV (Run 5)
• Model calculations indicate quenching expected at sNN = 22 GeV, but Cronin effect dominates
• Species dependence to probe space/time of suppression
arXiv:0801.4555
Energy Particle Species Au+Au 200 GeV (Run 4)
Terry Awes, ORNL - QM08, Jaipur India Slide:6
Dependence of Nuclear Suppression
• RAA scales with Npart at same sNN– Some indication for “higher order” effects
• Approximate scaling with <L>• Use RAA(Npart, sNN, Species, Pathlength) to illuminate models
Session I: Klaus Reygers
PHENIX PRC 76 034904
NPart Pathlength
Direct Photons
Terry Awes, ORNL - QM08, Jaipur India Slide:8
Towards inclusive ( contribution)
• Universal mT-scaling – Independent of centrality in Au+Au
Poster: B.Sahlmuller
Au+Au 200 GeV
p+p systematics
PRC 75, 024909 (2007)
PHENIX Preliminary
PRC 75, 024909 (2007)
Terry Awes, ORNL - QM08, Jaipur India Slide:9
• Run 4 (QM06): High pT suppression
– Isospin (PDF) effect (+ ?)
PHENIX Preliminary
Direct Au+Au: Direct = Inclusive-Decay
• Run 2: No suppression -> Jet quenching (PRL 94, 232301 (2005)).
Terry Awes, ORNL - QM08, Jaipur India Slide:10
Direct RAA ResultsCentral Cu+Cu 200 GeV (Run 5) Direct RAA vs Npart
Session VIII: Takao Sakaguchi
PHENIX Preliminary
PHENIX PreliminaryMin Bias Au+Au 62 GeV (Run 4)
• Direct RAA 1• Is there other evidence for nuclear effects?
– Reduced/enhanced radiation due to jet quenching
Terry Awes, ORNL - QM08, Jaipur India Slide:11
Direct v2 : Au+Au 200 GeV
• Interested in sign of direct v2 (at high pT): – Positive == parton emission quenched– Negative == parton emission (Brems.) enhanced
• Results suggest positive v2
1* _
2.
2.2 −
−=
RvvR
votonBGotoninc
otondi
Session XV: Kentaro Miki
Direct v2 Min Bias Au+Au 200 GeV (Run 4)
Terry Awes, ORNL - QM08, Jaipur India Slide:12
-h Correlations
“measures” recoil parton momentum– Measure fragmentation function D(Z)
-h p+p 200 GeV (Run 5)
~D(z)
2triggerT
triggerT
partnerT
Ep
ppx ⋅−≡
Session XV: Matthew Nguyen
Poster: A.Hanks
Use Near Side peak to determine direct associated with h, I.e. fragmentation photons
J/ Production
Terry Awes, ORNL - QM08, Jaipur India Slide:14
J/ d+Au: Cold Nuclear Matter• Increased Run 5 p+p statistics (x10 Run
3)• Improved & consistent p+p and dAu
analysis– Improved alignment, resolution, yield
extraction,… – Cancellation of systematic errors in RdAu
• Result: CNM = Shadowing(EKS) + Breakup = 2.8 mb– Consistent within errors with previous
results– and with Breakup=4.2+/-0.5mb (SPS result)
J/ RdAu 200 GeV
Session VI: Matthew WysockiarXiv:0711.3917
+1.7-1.4
Terry Awes, ORNL - QM08, Jaipur India Slide:15
J/ Au+Au: CNM Effects
• Large errors still (need Run 8 d+Au, Run 7 Au+Au)– Comparison suggests more forward suppression beyond CNM than at
mid-rapidity– BUT models shown don’t describe RdAu impact parameter dependence
J/ RAuAu 200 GeV (Run4)
arXiv:0711.3917
|y| < 0.35 1.2 < |y| < 2.2
Terry Awes, ORNL - QM08, Jaipur India Slide:16
J/ RAA Cu+Cu and Au+Au• Approx 2x more J/ in Cu+Cu
sample than Au+Au sample– More precise Npart<100 info
• Curves show RAA prediction from ad hoc CNM fit to RdAu separately at y=0 and y > 1.2
• CNM from RdAu fit describes suppression for Npart < 100.
J/ RAA 200 GeV
Session XVIII: Susumu Oda
arXiv:0801.0220
RdAu constraints are not sufficient to say if suppression beyond cold nuclear matter is stronger at forward rapidity
Terry Awes, ORNL - QM08, Jaipur India Slide:17
J/ <pT2> Cu+Cu and Au+Au
• No (or modest) pT broadening of J/ – Conspiracy of low pT suppression and recombination? Session XVIII:
Susumu Oda
arXiv:0801.0220
Low Mass e+e-
Terry Awes, ORNL - QM08, Jaipur India Slide:19
Electron Pair Mass Spectrum p+p
• Combinatorial Bkground subtraction error 0.25%– Confirmed with special
convertor runs• Correlated unlike (and
like) pairs due to jet and Dalitz photon pair conversions
Mee p+p 200 GeV (Run5)
Unlike sign
Like sign
arXiv:0801.0220
Terry Awes, ORNL - QM08, Jaipur India Slide:20
Hadronic Cocktail to Calculate Mee • Based on PHENIX
measurements– (Light VM See
Session XXIII Y. Nakamiya)
• Fit to pion spectrum provides excellent fit to all other mesons with MT-scaling assumption– MT-scaling works very
well
arXiv:0802.0050
Terry Awes, ORNL - QM08, Jaipur India Slide:21
Measured p+p Mee compared to Cocktail
• Cocktail filtered in PHENIX acceptance
• Charm, Bottom, DY contributions from PYTHIA
• Excellent agreement!
arXiv:0802.0050
Terry Awes, ORNL - QM08, Jaipur India Slide:22
Heavy Quarks in p+p from e+e-
c dominant
b dominant
After subtraction of Cocktail -Fit to a*charm+ b*bottom (with PYTHIA shape)
arXiv:0802.0050
• Good agreement with single e results
• Also new analyses via e-h coincidences, single muons, and direct charm measurement– See talks:
Session XIV: Yuhei MorinoDonny Hornback
Terry Awes, ORNL - QM08, Jaipur India Slide:23
Bottom Measurement
• Charm and bottom spectra both x above FONLL calculations– But ratio is in good agreement with FONLL
Session XIV: Yuhei Morino
p+p 200 GeV Charm and bottom extracted via e-h mass analysis
Terry Awes, ORNL - QM08, Jaipur India Slide:24
Heavy Flavor via non-photonic Electrons• HF strongly suppressed, Significant v2
– Implies high density, small diffusion coefficient
– Estimate /s = (1.3-2)/4– Very close to conjectured limit
PHENIX : PRL98, 172301 (2007)
Session XIV: Ralf Averbeck
Poster: A.DionPreliminary Run 7 HF v2 result:
Terry Awes, ORNL - QM08, Jaipur India Slide:25
Au+Au Mee compared to Cocktail• Data and Cocktail
absolutely normalized
– Cocktail normalized to Au+Au measurements
• Except ccbar• Low mass excess
– 150 < Mee < 750– X 3.4±0.2(stat.)
±1.3(syst.)±0.7(model)
• Intermediate mass agreement
arXiv:0706.3034
– Thermal contribution perhaps if ccbar mass spectrum softened by rescatt.
Terry Awes, ORNL - QM08, Jaipur India Slide:26
PT Dependence of Au+Au Mee
• Low Mass excess is a low pT enhancement– Huge excess at
lowest pT– Late Phase info
0 < pT < 8 GeV/c 0 < pT < 0.7 GeV/c
0.7 < pT < 1.5 GeV/c 1.5 < pT < 8 GeV/c
Session XI: Alberica Toia
PHENIX Preliminary • Still significant at high pT
Terry Awes, ORNL - QM08, Jaipur India Slide:27
High pT Direct Yield from *• Virtual with pT >> mee should
be produced directly with a rate and mass distrib. that follows a “Dalitz” form fdir with MHad->oo
• Extract Direct * “excess” as fraction r of fdir needed to describe low mass excess
• That direct * fraction of inclusive * (mostly and ) should be the same as the real fraction of inclusive (mostly and )
Terry Awes, ORNL - QM08, Jaipur India Slide:28
Direct via * for p+p, Au+Au• New p+p result with *
method agrees with NLO pQCD predictions, and with statistical method at high pT– Confirmation of the
method• For Au+Au (QM05 result)
there is a significant low pT excess above p+p expectations– Interpreted as thermal
emission -> Initial T
Session XV: Torsten DahmsarXiv:0801.xxxx
Terry Awes, ORNL - QM08, Jaipur India Slide:29
Summary• More precise studies
of sQGP matter – Systematics of RAA -h correlations
– Dilepton excess
• Initial T and evolution– Low pT direct excess
– Heavy Flavor– J/ |y| < 0.35
Terry Awes, ORNL - QM08, Jaipur India Slide:30
PHENIX Data SetsYear Species √s [GeV ] ∫Ldt Ntot (sampled) Data Size
Run1 2000 Au - Au 130 1 µb-1 10 M 3 TB
Run2 2001/02 Au - Au 200 24 µb-1 170 M 10 TB
Au - Au 19 < 1 M
p - p 200 0.15 pb-1 3.7 B 20 TB
Run3 2002/03 d - Au 200 2.74 nb-1 5.5 B 46 TB
p - p 200 0.35 pb-1 6.6 B 35 TB
Run4 2003/04 Au - Au 200 241 µb-1 1.5 B 270 TB
Au - Au 62.4 9 µb-1 58 M 10 TB
Run5 2005 Cu - Cu 200 3 nb-1 8.6 B 173 TB
Cu - Cu 62.4 0.19 nb-1 0.4 B 48 TB
Cu - Cu 22.4 2.7 µb-1 9 M 1 TB
p - p 200 3.8 pb-1 85 B 262 TB
Run-6 2006 p - p 200 10.7 pb-1 233 B 310 TB
p - p 62.4 0.1 pb-1 10 B 25 TB
Run-7 2007 Au - Au 200 725 µb-1 4.6 B 570 TB
Run-8 2007/08 d - Au 200
p - p 200/500