Thermal photons and lepton pairs from quark gluon plasma and hot hadronic matter

被引:64
作者
Alam, J [1 ]
Sarkar, S
Roy, P
Hatsuda, T
Sinha, B
机构
[1] Kyoto Univ, Dept Phys, Kyoto 6068502, Japan
[2] Ctr Variable Energy Cyclotron, Kolkata 700064, W Bengal, India
[3] Saha Inst Nucl Phys, Kolkata 700064, W Bengal, India
[4] Kyoto Univ, Dept Phys, Kyoto 6068502, Japan
[5] Ctr Variable Energy Cyclotron, Kolkata 700064, W Bengal, India
[6] Saha Inst Nucl Phys, Kolkata 700064, W Bengal, India
基金
日本学术振兴会;
关键词
D O I
10.1006/aphy.2000.6091
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
The formulation of the real and virtual photon production rate from strongly interacting matter is presented in the framework of finite temperature field theory. Th changes in the hadronic spectral function induced by temperature are discussed within the ambit of the Walecka type model, gauged linear and non-linear sigma models. hidden local symmetry approach, and QCD sum rule approach. The possibility of observing the direct thermal photon and lepton pairs from quark gluon plasma has been contrasted with those from hot hadronic matter with and without medium effects Ibr various mass variation scenarios. At SPS energies, in-medium effects of different magnitude on the hadronic properties for the Walecka model. Brown-Rho scaling. and Nambu scaling scenarios are conspicuously visible through the low invariant mass distribution of dileptons and transverse momentum spectra of photons. However at RHIC energies the thermal photon (dilepton) spectra originating from quark gluon plasma overshines those from hadronic matter for large transverse momentum (invariant mass) irrespective of the models used for evaluating the finite temperature effects on the hadronic pn,properties. It is thus expected that at both RHIC and LHC energies the formation of quark gluon plasma in the initial stages may indeed turn out to be a realistic scenario. (C) 2000 Academic Press.
引用
收藏
页码:159 / 248
页数:90
相关论文
共 139 条
[1]  
ABRIKOSOV AA, 1959, ZH EKSP TEOR FIZ, V9, P636
[2]   Electromagnetic probes of quark gluon plasma [J].
Alam, J ;
Raha, S ;
Sinha, B .
PHYSICS REPORTS-REVIEW SECTION OF PHYSICS LETTERS, 1996, 273 (5-6) :243-362
[3]   Unstable particles in matter at a finite temperature:: The ρ and ω mesons [J].
Alam, JE ;
Sarkar, S ;
Roy, P ;
Dutta-Roy, B ;
Sinha, B .
PHYSICAL REVIEW C, 1999, 59 (02) :905-913
[4]   SUCCESSIVE EQUILIBRATION IN QUARK-GLUON PLASMA [J].
ALAM, JE ;
RAHA, S ;
SINHA, B .
PHYSICAL REVIEW LETTERS, 1994, 73 (14) :1895-1898
[5]   Limits on the production of direct photons in 200A GeV S-32+Au collisions [J].
Albrecht, R ;
Antonenko, V ;
Awes, TC ;
Barlag, C ;
Berger, F ;
Bloomer, M ;
Blume, C ;
Bock, D ;
Bock, R ;
Bohne, EM ;
Bucher, D ;
Claesson, G ;
Claussen, A ;
Clewing, G ;
Debbe, R ;
Dragon, L ;
Dubovik, Y ;
Eklund, A ;
Fokin, S ;
Franz, A ;
Garpman, S ;
Glasow, R ;
Gustafsson, HA ;
Gutbrod, HH ;
Hansen, O ;
Holker, G ;
Idh, J ;
Ippolitov, M ;
Jacobs, P ;
Kampert, KH ;
Karadjev, K ;
Kolb, BW ;
Lebedev, A ;
Lohner, H ;
Lund, I ;
Manko, V ;
Moskowitz, B ;
Nikolaev, S ;
Nystrand, J ;
Obenshain, FE ;
Oskarsson, A ;
Otterlund, I ;
Peitzmann, T ;
Plasil, F ;
Poskanzer, AM ;
Purschke, M ;
Ritter, HG ;
Roters, B ;
Saini, S ;
Santo, R .
PHYSICAL REVIEW LETTERS, 1996, 76 (19) :3506-3509
[6]   Hard-thermal-loop resummation of the thermodynamics of a hot gluon plasma [J].
Andersen, JO ;
Braaten, E ;
Strickland, M .
PHYSICAL REVIEW D, 2000, 61 (01)
[7]   RHO MESON IN DENSE HADRONIC MATTER [J].
ASAKAWA, M ;
KO, CM ;
LEVAI, P ;
QIU, XJ .
PHYSICAL REVIEW C, 1992, 46 (04) :R1159-R1162
[8]   What thermodynamics tells us about the QCD plasma [J].
Asakawa, M ;
Hatsuda, T .
PHYSICAL REVIEW D, 1997, 55 (07) :4488-4491
[9]   A COMPARISON OF THE REAL-TIME AND THE IMAGINARY-TIME FORMALISMS OF FINITE-TEMPERATURE FIELD-THEORY FOR 2-POINT, 3-POINT AND 4-POINT GREEN-FUNCTIONS [J].
AURENCHE, P ;
BECHERRAWY, T .
NUCLEAR PHYSICS B, 1992, 379 (1-2) :259-303
[10]   Bremsstrahlung and photon production in thermal QCD [J].
Aurenche, P ;
Gelis, F ;
Zaraket, H ;
Kobes, R .
PHYSICAL REVIEW D, 1998, 58 (08)