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Perturbative photons in pp (and AA) collisions at RHIC energies. Monique Werlen (LAPTH). Why are direct photons interesting?. Photons produced in the partonic interaction probe QCD dynamic without hadronic complications γ – quark: coupling precisely known (QED)

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slide1

Perturbative photons in pp

(and AA) collisions

at RHIC energies

Monique Werlen (LAPTH)

slide2

Why are direct photons interesting?

  • Photons produced in the partonic interaction probe QCD dynamic without hadronic complications
  • γ – quark: coupling precisely known (QED)
  • Two processes at lowest order:
  • QCD Compton : sensitive to gluon distribution in the hadron
  • Annihilation: sensitive to the QCD running coupling constant αs

αs

αs

α

α

α

αs

α

αs

slide3

O(ααs)

O(αs2α(1/αs+g))

Important at high √s and low pt

(NLO ACFGP NPB399,34)

O(ααs2)

slide4

Direct photon production

O(ααs)

“Direct” γ

O(ααs2)

Fragmentation

Only the sum σ(D) + σ(F) is a physical observable

slide6

World Data vs NLO QCD

INCNLO

23 GeV ≤√s≤ 63 GeV

Aurenche, Fontannaz, Guillet, Kniehl,

Pilon, M.W. Eur. Phys. JC9,107 (1999)

slide7

But NLO QCD has been proved correct!

including for direct photon

at least for the measurement of αs

(UA6 Phys.Lett. B452,201)

See Bethke plots (hep-ex/0407021)

on next slide

slide9

Additional contributions

to solve the Pb? NNLres

slide10

New PHENIX data

INCNLO

NLO QCD fine

fig. 4.34 from hep-ph/0311131 CERN YR

slide11

Theoretical uncertainties at RHIC energy

Fragmentation BFGI/BFGII

Scales uncertainty

slide12

Aurenche et al Eur. Phys. JC9,10(1999)

Updated with PHENIX prelim. K.Odaka et al.

hep-ex/0501066

Stat. Err. only

Phenix data clarifies the data/theory puzzle

slide13

Remark:

Fragmentation vs direct depends on scales (specially M_F)

One cannot evaluate

“the fraction due to fragmentation”!

slide14

The PHOX Family

NLO event generators (parton level)

for large ptPHOton (hadron ou jet) X-sections

http://www.lapp.in2p3.fr/lapth/PHOX_FAMILY/main.html

P.Aurenche, T.Binot, M.Fontannaz, J.Ph.Guillet, G.Heindrich, E.Pilon, M.W.

DIPHOX:

h1 h2→γγ+X

h1 h2→γh3+X

h1 h2→h3 h4+X

slide15

DIPHOX vs CDF data azimuthal angle

Remark: resummation needed near π

slide16

Photon Isolation

K.Odaka hep-ex/0501066

in a cone around photon with:

=0.5

R=

ET (parton) ≤ ET max =0.1Eγ

Isolated/Non-isolated

JETPHOX NLO

CTEQ6M BFG II M=MF=μ=pT

Isolated vs non-isolated: not much difference in data and in theory

prompt photons in aa collisions
Prompt Photons in AA collisions

hep-ph/0311131 CERN YR

Includes:

- EKS98 : Structure Function modification

in heavy nucleus (anti-)shadowing in Au

- parton energy loss

slide19

γ/π0

hep-ph/0311131 CERN YR

slide21

hep-ph/0311131 CERN YR

Not complete… for example:

no photon emission through Compton and Annihilation of partons in the plasma (jet-thermal in next slide)

no induced bremsstrahlung by the medium (next slide)

slide22

Induced γ

bremsstrahlung

All scales pt, CTEQ5M,

LO with k-factors from NLO

for direct and bremss

N-N:direct

---Without gluon suppression

slide23

Summary

  • Direct photon production
  • pp collisions:
  • PHENIX preliminary data seems to favor the NLO QCD theory (like most of ISR and fixed target data)
  • Isolation criteria induce only small effects
  • AA collisions:
  • A lot of small effects to take into account… Work in progress
slide26

Production of pions E706 data vs NLO theory

u(KKP)/u(BKK )

Gluon(KKP)/Gluon(BKK)

MF=3 GeV

M=MF=μ=pT/3

Better fit with fragmentation

functions KKP than BKK

<z> 0.75-0.9

Binoth,Guillet,Pilon,M.W. EPJC24,245

slide31

Fragmentation function BFGW

PHENIX:PRL 91,072303

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