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Damping of energetic gluons and quarks in high-temperature QCD

Journal Article · · Physical Review, D (Particles Fields); (United States)
;  [1]
  1. Department of Physics, McGill University, 3600 University Street, Montreal, Quebec, H3A2T8 (Canada)

When a gluon or a quark is sent through the hot QCD plasma it acquires a damping rate that is given by {gamma}({bold p})={ital cg}{sup 2} ln(1/{ital g}){ital T}+{ital O}({ital g}{sup 2}{ital T}) for {vert bar}{bold p}{vert bar}{much gt}{ital gT}. We show that very simple arguments suffice to fix the numerical coefficient {ital c} in this expression and to show that the {ital O}({ital g}{sup 2}{ital T}) contributon is incalculable in perturbation theory without further assumptions. For QCD with {ital N}{sub {ital c}} colors we find {ital c}{sub {ital g}}=+{ital N}{sub {ital c}}/4{pi} for gluons and {ital c}{sub {ital q}}=+({ital N}{sub {ital c}}{sup 2}{minus}1)/8{pi}{ital N}{sub {ital c}} for quarks, in agreement with more detailed calculations of Pisarski {ital et} {ital al}. but not with those of Lebedev {ital et} {ital al}. The simplicity of the calculation permits a direct verification of the gauge invariance and the physical sign of the result.

OSTI ID:
5135948
Journal Information:
Physical Review, D (Particles Fields); (United States), Journal Name: Physical Review, D (Particles Fields); (United States) Vol. 45:1; ISSN PRVDA; ISSN 0556-2821
Country of Publication:
United States
Language:
English

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