direct photon at rhic-phenix

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Direct photon at RHIC- PHENIX Kensuke Okada (RBRC) For the PHENIX collaboration Rencontres de Moriond March 13, 2012 3/13/2012 1 K.Okada

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Direct photon at RHIC-PHENIX. Kensuke Okada (RBRC) For the PHENIX collaboration Rencontres de Moriond March 13, 2012. Direct photon: a unique probe. high pT: Known source, Penetrating probe A good reference to jet quenching low pT : QGP production mechanism Spectra : A thermometer - PowerPoint PPT Presentation

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Page 1: Direct photon at RHIC-PHENIX

K.Okada 1

Direct photon at RHIC-PHENIX

Kensuke Okada (RBRC) For the PHENIX collaboration

Rencontres de Moriond March 13, 2012

3/13/2012

Page 2: Direct photon at RHIC-PHENIX

K.Okada 2

Direct photon: a unique probe

• high pT: Known source, Penetrating probe – A good reference to jet quenching

• low pT : QGP production mechanism – Spectra : A thermometer– Azimuthal dependence to the reaction plane :

Probe for the formation mechanism

3/13/2012

A new state of the matter (sQGP)Produced by HI collision.

Page 3: Direct photon at RHIC-PHENIX

K.Okada 3

PHENIX detector

3/13/2012

Fine segmented EMCalElectron identification, tracking +High DAQ rate Trigger

The central arm spectrometer

Page 4: Direct photon at RHIC-PHENIX

K.Okada 4

Reference data (p+p)

3/13/2012

Measured up to pT=25 GeV/c.

The pQCD NLO calculation is in good agreement with data.

Page 5: Direct photon at RHIC-PHENIX

K.Okada 5

xT scaling

3/13/2012

pp/p+pbar, inclusive/isolated

They are on a universal curveexcept one experiment, from LHC to fixed target experiments.

xT2pT/scross section scaled by s4.5

PHENIX e+e-

PHENIX

n=4.5 is in a range consistent with expectations from NLO pQCD.

Page 6: Direct photon at RHIC-PHENIX

K.Okada 6

Direct photon RAA

3/13/2012

There is a difficulty in high pT region in the measurement. (=0 merging BG, cosmic BG in p+p.)

Various checks are done.Final results will come out soon.

Nuclear modification factor (R_AA) Photon vs. hadron

high pT

PRL101,232301 (2008) PRC 82,011902(2010)

Page 7: Direct photon at RHIC-PHENIX

K.Okada 7

Photon = e++e-?

3/13/2012

They have the same quantum number. Kroll-Wada formula connects the real and (ee) yield.

Independent of the origin in the very low mass region (Mee < ~30MeV)No 0 Dalitz above the 0 mass. The key to improve the S/N ratio. Direct photon follows 1/Mee.

ProcedureCombinatorial and correlated pair subtractionCocktail and direct photon shapes Normalized in the very low mass regionFit and Extract the direct photon component

SdNMM

m

M

m

dM

Nd

eeee

e

ee

e

ee

121

41

3

22

2

2

22

22eeT Mp When , S=1 for photons.

m

q

g*

g q

e+

e-

low pT

Page 8: Direct photon at RHIC-PHENIX

8

Virtual photon spectra

3/13/2012

p+p: Already shown in the previous xT plot.d+Au: Consistent with scaled p+p. Little or no nuclear effects.

Au+Au

K.Okada

Au+Au: Large excess in low pT region. <T> is extracted from the inverse slope.

PRL 104,132301 (2010)

Page 9: Direct photon at RHIC-PHENIX

K.Okada 9

Tc~170MeV from lattice QCD

Initial temperature & formation time

3/13/2012

PRC 81, 034911 (2010)

They are all above the critical temperature. However Tinit depends on 0 in the theory calculations.

Need additional experimental constraints

Page 10: Direct photon at RHIC-PHENIX

K.Okada 10

Direct photon 2

3/13/2012

Hadron gas

sQGP

Parton+medium

Jet fragment

Hard scat.

pTThe ingredients are tuned by pT

v2 > 0

v2 < 0 Parton+medium

Jet fragment

q+gHard scatteringv2 = 0

sQGP Hadron gas

v2 0 Amplitude for 0, Relative ratio

(another knob)

Page 11: Direct photon at RHIC-PHENIX

K.Okada 11

Direct photon 2

3/13/2012

12

.2.

2

R

vvRv

BGincdir

inc2

BG2

Inclusive photon v2

BG photon v2 (From 0 and other mesons v2)

B

BSR

From virtual photon measurement

From real photon in the EMCal with virtual photon measurement

Page 12: Direct photon at RHIC-PHENIX

12

Direct photon 2

3/13/2012

At high pT, v2~0. It is consistent with the hard scattering source. At low pT (thermal region), an unexpectedly large v2 is observed!

It depends on the formation time.But theory predictions are too small.

early late small large

K.Okada

arXiv:1105.4126

MB (0-92%) 0-20% 20-40%

calculation from PRC 79, 021901(R)

Page 13: Direct photon at RHIC-PHENIX

K.Okada 13

Next step: 2 of virtual photon

3/13/2012

v2 from combinatorial BGand remaining Dalitz decaycan be well controlled.

virtual photon

real photonsys. uncertainty tablearXiv:1105.4126

Advantage (systematic)

Disadvantage (statistics)Total statistics goes down by a factor of ~200.Even in 1-3 GeV/c bin, it’s statistically challenging.

ee are induced in a strong magnetic field in HI collisions?PRC 83, 017901 (2011) Tuchin

If it is true, it affects the assumptionsin all virtual photon results. Anyway it is interesting.

Page 14: Direct photon at RHIC-PHENIX

K.Okada 14

Future sPHENIX project

3/13/2012

What can we add to the current RHIC detectors?Large acceptance with high /0 separation.More tracking layers, hope eID is still powerful.Hadron calorimeter for +Jet analysis.

A plan to upgrade the detector.

Page 15: Direct photon at RHIC-PHENIX

K.Okada 15

Summary

• Showed PHENIX (selected) photon results• p+p reference measurements are on the

universal curve of world’s measurements. • An unexpectedly large 2 was measured in the

low pT region. No theory explanation so far. • PHENIX upgrade discussion is on going.

3/13/2012

Page 16: Direct photon at RHIC-PHENIX

K.Okada 16

Backup

3/13/2012

Page 17: Direct photon at RHIC-PHENIX

K.Okada 17

Space time evolution

3/13/2012

Page 18: Direct photon at RHIC-PHENIX

K.Okada 18

Hadron contamination check

• Hadron contamination can be significant

• Check with an external conversion analysis– Identify photons via

conversion in material to dileptons

– No hadron contamination• Two measurements are

consistent• Hadron contamination in the

real photon (EMCal) measurement well understood

3/13/2012

Page 19: Direct photon at RHIC-PHENIX

K.Okada 19

STAR

3/13/2012

Page 20: Direct photon at RHIC-PHENIX

K.Okada 20

STAR vs PHENIX

3/13/2012

PHENIX has a little better S/B ratio. Acceptance STAR = 6*PHENIXDAQ STAR(~1kHz) vs PHENIX(~6kHz)

Page 21: Direct photon at RHIC-PHENIX

K.Okada 21

PHENIX Au+Au Statistics

3/13/2012

Run species AuAu200 intL comment

4 AuAu200, 64.4 1.5G (0.241/nb)

7 AuAu200, 5.1G(0.813/nb) RXN, HBD prototype

8 dAu, p+p

9 p+p500, 200

10 AuAu200, lowE (1.25/1.07/nb) for 30/20cm

RXN, HBD

11 pp500,AuAu19.6, 200 (0.913/0.788/nb) for 30/12cm

VTX

In Run10, 11, the integrated luminosity is comparable to Run7. Can we remove Dalitz decay to reduce the combinatorial? Then small Mee will be cut out. It needs some trick for the mass shape fit.

STAR has an advantage if their claim for the combinatorial BG is true.

Page 22: Direct photon at RHIC-PHENIX

K.Okada 22

RHIC advantage to LHC

3/13/2012

Page 23: Direct photon at RHIC-PHENIX

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System size dependence of g fraction

• g fraction = Yielddirect / Yieldinclusive

• Largest excess above pQCD is seen at Au+Au.– Moderately in Cu+Cu also.

3/13/2012 K.Okada

No excess in d+Au(no medium)

Excess also in Cu+Cu

Page 24: Direct photon at RHIC-PHENIX

• Later thermalization gives larger v2 (QGP photons)

• Large photon flow is not explained by models for QGP

3/13/2012 K.Okada 24

Comparison with models. No success..

Curves: Holopainen, Räsänen, Eskola., arXiv:1104.5371v1

thermal

diluted by prompt

Chatterjee, Srivastava PRC79, 021901 (2009)

Hydro after t0

QM: Quark MatterHM: Hadronic Matter