Dilepton measurement in H.I.C.

22
Dilepton measurement Dilepton measurement in H.I.C. in H.I.C. 小小小 小小小 小小 小小

description

Dilepton measurement in H.I.C. 小沢恭一郎 東大・理. Lepton pair measurements. p T [GeV/ c ]. φ. ω. J/ y. ρ. As a function of Energy Species Centrality Rapidity. 2. Heavy Flavor. Thermal Radiation. 1. Drell Yan. g*. 1. 2. 3. Mass [GeV/ c 2 ]. ● Au + Au ● p+p. J/ y. φ. ω. - PowerPoint PPT Presentation

Transcript of Dilepton measurement in H.I.C.

Page 1: Dilepton  measurement in H.I.C.

Dilepton measurement in Dilepton measurement in H.I.C.H.I.C.

小沢恭一郎 小沢恭一郎 東大・理 東大・理

Page 2: Dilepton  measurement in H.I.C.

●   Au + Au ●   p+pω φ

J/

Lepton pair measurementsLepton pair measurements

9/15/20079/15/2007 Heavy Ion Cafe @ HongoHeavy Ion Cafe @ Hongo 22

Mass[GeV/c2]

pT

[GeV/c]

1 2 3

2

ω φ J/ρ

Thermal

Radiation

Heavy

Flavor

Drell

Yan

As a function of

Energy

Species

Centrality

Rapidity

Page 3: Dilepton  measurement in H.I.C.

φφ ・・ ωω

Page 4: Dilepton  measurement in H.I.C.

9/15/20079/15/2007 Heavy Ion Cafe @ HongoHeavy Ion Cafe @ Hongo 44

Chiral Symmetry in Hadronic matterChiral Symmetry in Hadronic matter

Mass shiftMass shift and/or and/or modificationmodification of vector of vector mesons are expectedmesons are expected

Lepton decaysLepton decays become good probes become good probes Not interacting “strongly.”Not interacting “strongly.” However, we only see However, we only see integrated informationintegrated information

from all stages of collisions.from all stages of collisions. Energy and Centrality dependenceEnergy and Centrality dependence

QGPHadron gas

AfterFreeze Out

Integrated information

T.Hatsuda and S.Lee

(Phys.Rev.C46-R34-38, 1992)

Line shapeLine shape Direct measurementsDirect measurements

YieldYield Q value of Q value of → → KK is smallKK is small

( )

( )

BR ee

BR KK

Page 5: Dilepton  measurement in H.I.C.

9/15/20079/15/2007 Heavy Ion Cafe @ HongoHeavy Ion Cafe @ Hongo 55

hadron and lepton decayshadron and lepton decays

Main issue:

K+K- and e+e-

seem not consistent

Many efforts are on-going to understand the difference btw K and e.

We have to prove that the difference is not made artificially.We have to prove that the difference is not made artificially.

Analysis in d+Au and p+p data is important as baseline. Analysis in d+Au and p+p data is important as baseline.

Page 6: Dilepton  measurement in H.I.C.

9/15/20079/15/2007 Heavy Ion Cafe @ HongoHeavy Ion Cafe @ Hongo 66

p+p p+p

d/dy

Extracted by integrationOMEGA:

3.50037 +/- 0.175942 (stat) +/- 0.875 (sys)

4.37554 (upper sys) 2.62521 (lower sys)

PHI:

0.369182 +/- 0.0195987 (stat) +/- 0.0894 (sys)

0.458564 (upper sys) 0.2798 (lower sys)

omega

phi

Page 7: Dilepton  measurement in H.I.C.

9/15/20079/15/2007 Heavy Ion Cafe @ HongoHeavy Ion Cafe @ Hongo 77

spectraspectra Spectra of Spectra of meson are measured in several collision meson are measured in several collision

systems.systems.p+p Au+Aud+Au

Results are mainly obtained using hadron decays. Analysis for electron decay mode is underway.

Page 8: Dilepton  measurement in H.I.C.

Lepton pair continuumLepton pair continuum(ρ(ρ ? ?  ThermalThermal ?? ))

Page 9: Dilepton  measurement in H.I.C.

9/15/20079/15/2007 Heavy Ion Cafe @ HongoHeavy Ion Cafe @ Hongo 99

Lepton pair continuumLepton pair continuum

Broadening of Broadening of meson makes meson makes continuum on the invariant continuum on the invariant mass of electron-positron pairmass of electron-positron pair

In addition,In addition, thermal radiation thermal radiation by by the system via quark anti-quark the system via quark anti-quark annihilation also makes annihilation also makes continuum and it carries direct continuum and it carries direct information from the matter.information from the matter. Matter is formedMatter is formed DeconfinementDeconfinement ThermalizedThermalized

Experimentally, Experimentally, combinatorial combinatorial background is very largebackground is very large and and must be subtracted properly.must be subtracted properly.

Also, useful for charm Also, useful for charm measurementsmeasurements

A prediction

R. Rapp, nucl-ex 0204003

Page 10: Dilepton  measurement in H.I.C.

9/15/20079/15/2007 Heavy Ion Cafe @ HongoHeavy Ion Cafe @ Hongo 1010

@SPS - NA60@SPS - NA60 and and : : fix yields such fix yields such

as to get, after as to get, after subtraction, a subtraction, a smoothsmooth underlying continuumunderlying continuum

: : (()) set upper limit, set upper limit, defined by “defined by “saturatingsaturating” ” the measured yield in the measured yield in the mass region close to the mass region close to 0.2 GeV/c0.2 GeV/c22 ( (lower limit lower limit for excessfor excess).).

(() use yield measured ) use yield measured for pfor pTT > 1.4 GeV/c > 1.4 GeV/c

Page 11: Dilepton  measurement in H.I.C.

9/15/20079/15/2007 Heavy Ion Cafe @ HongoHeavy Ion Cafe @ Hongo 1111

What’s this?What’s this?

• absolute norm., melting • M>0.9GeV: “4”→and • baryon effects essential

[van Hees+RR ‘06]

Page 12: Dilepton  measurement in H.I.C.

9/15/20079/15/2007 Heavy Ion Cafe @ HongoHeavy Ion Cafe @ Hongo 1212

@RHIC@RHIC

Clear enhancement is observed Clear enhancement is observed in the mass region below in the mass region below ..

submitted to Phys. Rev. Lett

arXiv:0706.3034

Page 13: Dilepton  measurement in H.I.C.

9/15/20079/15/2007 Heavy Ion Cafe @ HongoHeavy Ion Cafe @ Hongo 1313

pp pp –– AuAu comparison AuAu comparison

p+p NORMALIZED TO mee<100 MeVp+p MULTIPLIED by Ncoll

Page 14: Dilepton  measurement in H.I.C.

9/15/20079/15/2007 Heavy Ion Cafe @ HongoHeavy Ion Cafe @ Hongo 1414

Centrality DependenceCentrality Dependence

• 0 production scales with Npart

• If in-medium enhancement from or qq annihilationyield should increase faster than proportional to Npart

LOW MASS

INTERMEDIATE MASS

• 0 production scales with Npart

• charm follows binary scaling yield should increase proportional to Ncoll

Page 15: Dilepton  measurement in H.I.C.

photonphoton

9/15/20079/15/2007 Heavy Ion Cafe @ HongoHeavy Ion Cafe @ Hongo 1515

Page 16: Dilepton  measurement in H.I.C.

9/15/20079/15/2007 Heavy Ion Cafe @ HongoHeavy Ion Cafe @ Hongo 1616

Thermal photonThermal photon Direct photonDirect photon

Directly emitted from the Directly emitted from the medium medium

Not from hadron decaysNot from hadron decays Hard photonHard photon

Initial pQCDInitial pQCD Thermal photonThermal photon

Hadron gasHadron gasQGPQGP

Turbide, Rapp, Gale, Phys. Rev. C 69 (014903), 2004

Window for thermal photons from QGP in this calculation: Window for thermal photons from QGP in this calculation: ppTT = 1 - 3 GeV/ = 1 - 3 GeV/cc

pQCD calculation should be confirmed in High ppQCD calculation should be confirmed in High pTT region region

After subtraction of large After subtraction of large background from hadron background from hadron decays, decays,

Page 17: Dilepton  measurement in H.I.C.

9/15/20079/15/2007 Heavy Ion Cafe @ HongoHeavy Ion Cafe @ Hongo 1717

Idea - Idea - ** e e++ee--

Compton

q

g q

0

0

e+

e-

q

g q

e+

e-

Any  source of real  emits virtual  with very low mass

Dalitz decay Use lepton pairs to measure virtual 

 and extrapolate to real  

PHENIX can measure low mass e+e- pairs

hadron decays and

direct photon

*incl.

*directcan be measured.

*In the analysis, Mee distribution for Dalitz and direct photon is calculated theoretically. Therefore, the ratio of Nee in two different mass region is converted to the ratio between direct and inclusive photons. The systematic error is reduced.

Page 18: Dilepton  measurement in H.I.C.

9/15/20079/15/2007 Heavy Ion Cafe @ HongoHeavy Ion Cafe @ Hongo 1818

**directdirect / / **

inclusiveinclusive

Significant 10% excess of Significant 10% excess of very-low-massvery-low-mass virtual direct photons virtual direct photons

Results agrees well with Results agrees well with Conventional resultConventional result

*incl.

*direct

One can extract the direct photon yield from the inclusive photon yield.

incl.

direct=

Page 19: Dilepton  measurement in H.I.C.

9/15/20079/15/2007 Heavy Ion Cafe @ HongoHeavy Ion Cafe @ Hongo 1919

Direct photon yieldDirect photon yield

Direct photon yield is calculated from Direct photon yield is calculated from the inclusive photon yield.the inclusive photon yield.

Page 20: Dilepton  measurement in H.I.C.

9/15/20079/15/2007 Heavy Ion Cafe @ HongoHeavy Ion Cafe @ Hongo 2020

Direct photon yieldDirect photon yield

Direct photon yield is calculated from Direct photon yield is calculated from the inclusive photon yield.the inclusive photon yield.

Compare to NLO pQCD Compare to NLO pQCD L.E.Gordon and W. VogelsangL.E.Gordon and W. Vogelsang

Phys. Rev. D48, 3136 (1993) Phys. Rev. D48, 3136 (1993)

Excess above the calculation

It might include contribution from thermal photons

Reference measurement needed

pp and dAu

Using same analysis method

Page 21: Dilepton  measurement in H.I.C.

9/15/20079/15/2007 Heavy Ion Cafe @ HongoHeavy Ion Cafe @ Hongo 2121

Comparison of R* btw p+p and Au+Au

PHENIX Preliminary

Au+Au

p+p

Page 22: Dilepton  measurement in H.I.C.

9/15/20079/15/2007 Heavy Ion Cafe @ HongoHeavy Ion Cafe @ Hongo 2222

SummarySummary

So many interesting analysis topics are on-So many interesting analysis topics are on-going at PHENIXgoing at PHENIX Such as, Heavy flavor measurements, J/Such as, Heavy flavor measurements, J/, , , and , and

lepton pair continuumlepton pair continuum Measurement for chiral symmetry is Measurement for chiral symmetry is

underway.underway. First result will publish soon.First result will publish soon.

Enhancement is observed in eEnhancement is observed in e++ee-- continuum!continuum!

Interesting results in Direct photon Interesting results in Direct photon measurements.measurements.