2001
DOI: 10.1088/1126-6708/2001/12/009
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Photon emission from quark-gluon plasma: complete leading order results

Abstract: We compute the photon emission rate of an equilibrated, hot QCD plasma at zero chemical potential, to leading order in both α EM and the QCD coupling g s (T ). This requires inclusion of near-collinear bremsstrahlung and inelastic pair annihilation contributions, and correct incorporation of Landau-Pomeranchuk-Migdal suppression effects for these processes. Analogous results for a QED plasma are also included.

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Cited by 485 publications
(761 citation statements)
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“…When τ −1 f λ q ≫ 1 the photons decohere early from the parent quark and our result reduces to incoherent emission from individual scattering centers. Our result differs from previous findings [7,9] in several important ways: first, it treats the case of finite L/λ q ∼ few, relevant to heavy ion physics. Second, we find that the most significant contribution to the LPM effect for photons comes from the interference of the medium-induced photon radiation with the hard emission from the large Q 2 scattering of the parent quark.…”
Section: Differential Photon Bremsstrahlung Spectrum To All Ordecontrasting
confidence: 99%
“…When τ −1 f λ q ≫ 1 the photons decohere early from the parent quark and our result reduces to incoherent emission from individual scattering centers. Our result differs from previous findings [7,9] in several important ways: first, it treats the case of finite L/λ q ∼ few, relevant to heavy ion physics. Second, we find that the most significant contribution to the LPM effect for photons comes from the interference of the medium-induced photon radiation with the hard emission from the large Q 2 scattering of the parent quark.…”
Section: Differential Photon Bremsstrahlung Spectrum To All Ordecontrasting
confidence: 99%
“…This mechanism is quite similar to that for the photon radiation from hard quarks [16] and to the induced gluon radiation from fast partons [41]. The data analyses based on the standard formulas of [39] calculated for the fixed QCD coupling constant awaken a lively interest in such calculations with the running coupling constant (and changing the thermal quark mass). It looks like a quite relevant task, at least for the energy range covered by RHIC and LHC where the QGP, as we know, is strongly coupled.…”
Section: Prethermal and Thermal Photon Spectramentioning
confidence: 53%
“…Moreover, in our present calculations we are handling iHKM with the same set of parameters as used for describing almost all bulk hadron observables in the past (see [3]). Thus, in estimating the thermal emission from the QGP phase we draw attention to the expression of [39] with the number of quarks n f = 3 as for the LHC data…”
Section: Prethermal and Thermal Photon Spectramentioning
confidence: 99%
“…(3.21) is well known and can be expressed in terms of a path integral in the transverse plane, leading to 22) where U (x + , y + ; [r]) is defined in eq. (3.14) and the boundary conditions are r(y + ) = y and r(x + ) = x.…”
Section: Jhep01(2013)031mentioning
confidence: 99%