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

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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 Presentation

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Page 1: Highlights from PHENIX II: Photons and Leptons

Highlights from PHENIX II:Photons and Leptons

Terry Awes, ORNLFor the PHENIX collaboration

Page 2: Highlights from PHENIX II: Photons and Leptons

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

Page 3: Highlights from PHENIX II: Photons and Leptons

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)

Page 4: Highlights from PHENIX II: Photons and Leptons

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)

Page 5: Highlights from PHENIX II: Photons and Leptons

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)

Page 6: Highlights from PHENIX II: Photons and Leptons

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

Page 7: Highlights from PHENIX II: Photons and Leptons

Direct Photons

Page 8: Highlights from PHENIX II: Photons and Leptons

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)

Page 9: Highlights from PHENIX II: Photons and Leptons

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)).

Page 10: Highlights from PHENIX II: Photons and Leptons

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

Page 11: Highlights from PHENIX II: Photons and Leptons

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)

Page 12: Highlights from PHENIX II: Photons and Leptons

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

Page 13: Highlights from PHENIX II: Photons and Leptons

J/ Production

Page 14: Highlights from PHENIX II: Photons and Leptons

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

Page 15: Highlights from PHENIX II: Photons and Leptons

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

Page 16: Highlights from PHENIX II: Photons and Leptons

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

Page 17: Highlights from PHENIX II: Photons and Leptons

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

Page 18: Highlights from PHENIX II: Photons and Leptons

Low Mass e+e-

Page 19: Highlights from PHENIX II: Photons and Leptons

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

Page 20: Highlights from PHENIX II: Photons and Leptons

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

Page 21: Highlights from PHENIX II: Photons and Leptons

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

Page 22: Highlights from PHENIX II: Photons and Leptons

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

Page 23: Highlights from PHENIX II: Photons and Leptons

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

Page 24: Highlights from PHENIX II: Photons and Leptons

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:

Page 25: Highlights from PHENIX II: Photons and Leptons

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.

Page 26: Highlights from PHENIX II: Photons and Leptons

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

Page 27: Highlights from PHENIX II: Photons and Leptons

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 )

Page 28: Highlights from PHENIX II: Photons and Leptons

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

Page 29: Highlights from PHENIX II: Photons and Leptons

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

Page 30: Highlights from PHENIX II: Photons and Leptons

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