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Direct photons at low pt
measured in PHENIX
D.Peressounko RRC “Kurchatov institute”
for the PHENIX collaboration
QM2006 D.Peressounko 2
Outline
Physics of direct photons at small pt
p+p collisionsTaggingSubtraction
d+Au collisionsTagging Subtraction Internal conversion
Au+Au collisionsSubtractionExternal conversionDirect photon HBT
Comparison of binary scaled d+Au and Au+Au Conclusions
QM2006 D.Peressounko 3
Direct photons at small pt
1/ptn
pt~5 GeV~3 GeV
e-pt/T
Prompt photons: control the initial state of the collision, modification of structure functions etc.
Jet-matter interaction: test matter density
Thermal photons: temperature and equation of state of the hot matter
d3N
/dyd
2p
t
Goal: extract thermal photon spectrum in A+A collisions and measure (effective) temperature.
Need a baseline from p+p and p+A collisions.
Jet-matter
See talk of TadaAki Isobe (Parallel session 3.3) for high pt photon review.
QM2006 D.Peressounko 4
Subtraction and Tagging methods
Measure photon spectrum and remove those photons which make 0 mass with any otherCorrect direct photon candidate sample for contribution from 0 decay photons with missing partner and for direct photons with fake partnersSubtract contribution from , etc. decays
Measure yield of inclusive photons corrected for hadron contaminations, conversion, efficiency and acceptance.Measure spectrum of 0, , etc.Calculate yield of decay photons and subtract it from the inclusive yield.
Ndir = N
incl - Ndecay
Subtraction Tagging
QM2006 D.Peressounko 5
Direct photon spectrum in p+p collisions
Submitted to Phys.Rev.Lett., hep-ex/0609031
PbGlPbScNLO pQCD CTEQ6M PDF µ=pT/2, pT, 2pT
(by W. Vogelsang)
GeV 200s at pp
Tagging
Data agrees with pQCD predictions in entire pt range
More data from Run-5 are coming (already available for pt>5 GeV)
Subtraction
QM2006 D.Peressounko 6
Direct photon spectrum in d+Au collisions
Data agrees with pQCD predictions in entire pt range
=> No indication for nuclear effects
NLO pQCD calculations from W.Vogelsang
Run-3 d+Au
Subtraction (pt<5 GeV) and tagging (pt>5 GeV) methods
QM2006 D.Peressounko 7
Internal conversion: idea
N.M.Kroll and W.Wada, Phys. Rev. 98 (1955) 1355
Number of real photons e+e- pair mass Mass (√s) of the
emitting system
Formfactor (~1)
Part common for all processes
Phase space
Due to phase-space factor we can measure direct photons in the region where e.g. 0 contribution is reduced (Mee>m) and thus increase Signal/Background ratio ~10 times
QM2006 D.Peressounko 8
Internal conversion: implementation
Fit measured mass spectrum with function
a - absolute normalization
b – proportion of direct photons:
decay
dir
N
Nb
QM2006 D.Peressounko 9
d+Au collisions: Double ratio
• Internal conversion method provides smaller systematic errors • But not as small as in the case of Au+Au collisions in Run-4 (Large background of external conversion on MVD detector in Run-3)
QM2006 D.Peressounko 10
d+Au collisions: Spectrum
Internal conversion extends range of significant points to pt > 2 GeV
Data agrees with pQCD predictions in full pt range
=> No indication for nuclear effects
QM2006 D.Peressounko 11
Au+Au collisions: External conversion
Combining this photon with others measured in EMCAL with loose PID cut, estimate proportion of photons coming from 0 decaysCorrect for missing 0 decay partnersSubtract , , ’ decay photonsCalculate ratio N
all/Ndecay
Use very tight PID cut on EMCAL photons to produce very clean photon sample
Use external photon conversion in beam pipe to produce very clean photon sample
External conversion Tagging
no pair cutwith pair cut
Dalitz
Conversion
Uses very pure photon sample
avoid explicit calculation of 0 spectrum=>reduce systematic errors
QM2006 D.Peressounko 12
Au+Au collisions, different methods
All three methods produce consistent resultsand comparable systematic errors.
(QM05)
See posters (#87) of Hijiang Gong and (#88) of TakaoSakagutchi
QM2006 D.Peressounko 13
Comparison: Au+Au Minimum Bias
Direct photon spectrum measured in d+Au collisions and scaled with <Ncoll> agrees pretty well with spectrum measured in Au+Au at high pt
=>Systematic errors are still too big to extract thermal photons.=>There is room for thermal photons
QM2006 D.Peressounko 14
Comparison: Au+Au, central collisions
Spectra agree within errors in entire pt range
Systematic errors are still too large to extract thermal photons.There is room for thermal photons
This is consistent with excess above pQCD reported previously
QM2006 D.Peressounko 15
Direct photon HBT
Only direct photon correlation matters (R
decay~108 fm)Size of emitting region can
be extractedProportion of direct photons can be evaluated from the correlation strength parameter:
Distortion of two-photon correlation function:Apparatus effects;Contamination by (correlated?) hadronsContamination by photon conversion on detector materialBackground photon correlations
See poster (#111) of Dmitri Peressounko for details
2
2
1
all
dir
N
N
1
3/2
1/Rdecay ~ 1 eV
q
QM2006 D.Peressounko 16
Two-photon correlations
1
2
1
2rec
e-
e+
External conversion:• No close cluster interference• No hadron contamination
C2 calculated in EMCAL and converted+EMCAL agree =>both effects are under control
QM2006 D.Peressounko 17
Conclusions
Measurement of direct photon yield at small pt is very interesting but extremely complicated taskPHENIX has developed a variety of methods for direct photon extraction in p+p, d+Au and Au+Au collisions producing consistent resultsBecause of the large systematic errors comparison of binary scaled d+Au spectrum with Au+Au does not allow to make a statement on the origin of the excess above pQCD observed in Au+Au. More precise data are coming…
QM2006 D.Peressounko 18
Backup slides
QM2006 D.Peressounko 19
Internal conversion: implementation
QM2006 D.Peressounko 20
Comparison to Subtraction Au+Au results