The gluon collisional width in hot QCD plasmas is discussed with emphasis on temperatures near Tc, where the coupling is large. Considering its effect on the entropy, which is known from lattice calculations, it is argued that the width, which in the perturbative limit is given by γ~g²ln(1/g)T, should be sizeable at intermediate temperatures but has to be small close to Tc. Implications of these results for several phenomenologically relevant quantities, such as the energy loss of hard jets, are pointed out.
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A. Peshier (2004) studied this question.
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