Photon emission from quark-gluon plasma: complete leading order results

Wecomputethephotonemissionrateofanequilibrated,hotQCDplasmaat zero chemical potential, to leading order in both fiEM and the QCD coupling gs(T). This requires inclusion of near-collinear bremsstrahlung and inelastic pair annihilation contri- butions, andcorrect incorporation of Landau-Pomeranchuk-Migdal suppressionefiects for these processes. Analogous resultsfor aQED plasmaare also included.

[1]  Greiner,et al.  Photons from strange-quark annihilation in a quark-gluon plasma. , 1986, Physical review. D, Particles and fields.

[2]  Laurence G. Yaffe,et al.  Photon Emission from Ultrarelativistic Plasmas , 2001 .

[3]  H. Weldon Effective Fermion Masses of Order gT in High Temperature Gauge Theories with Exact Chiral Invariance , 1982 .

[4]  H. Weldon Covariant Calculations at Finite Temperature: The Relativistic Plasma , 1982 .

[5]  B. G. Zakharov,et al.  Energy loss in perturbative QCD , 2003 .

[6]  Rudolf Baier,et al.  Induced gluon radiation in a QCD medium , 1995 .

[7]  R. Baier,et al.  THE LANDAU-POMERANCHUK-MIGDAL EFFECT IN QED , 1996 .

[8]  Yu.L. Dokshitzer,et al.  Medium-induced radiative energy loss; equivalence between the BDMPS and Zakharov formalisms , 1998 .

[9]  A. B. Migdal,et al.  Bremsstrahlung and pair production in condensed media at high-energies , 1956 .

[10]  B. Sinha Universal signals of a quark-gluon plasma , 1983 .

[11]  Seibert,et al.  High-energy photons from quark-gluon plasma versus hot hadronic gas. , 1991, Physical review. D, Particles and fields.

[12]  Enhanced photon production rate on the light cone. , 1996, Physical review. D, Particles and fields.

[13]  M. Neubert Photon production in ultrarelativistic heavy-ion collisions at 200 GeV/u , 1989 .

[14]  Y. Dokshitzer,et al.  Radiative energy loss of high-energy quarks and gluons in a finite volume quark - gluon plasma , 1997 .

[15]  Blankenbecler,et al.  Landau-Pomeranchuk-Migdal effect for finite targets. , 1996, Physical review. D, Particles and fields.

[16]  K. Redlich,et al.  Production rate of hard thermal photons and screening of quark mass singularity , 1992 .

[17]  F. Gelis,et al.  KLN theorem, magnetic mass, and thermal photon production , 1999 .

[18]  P. Ruuskanen,et al.  Shielding of quark mass singularities in photon emission from hot quark-gluon plasma , 1983 .

[19]  L. D. Landau,et al.  Limits of applicability of the theory of bremsstrahlung electrons and pair production at high-energies , 1953 .

[20]  E. Shuryak Quark-gluon plasma and hadronic production of leptons, photons and psions , 1978 .