As a preliminary step, the radiation produced by a classical charged current
coupled to a quantized Aμ is solved. To each order in α, all
infrared divergences cancel between the virtual γ's and the real
γ's absorbed from the plasma or emitted into the plasma. When all orders
of perturbation theory are summed, the finite answer predicts a suppression of
radiation with ω<αT. The analysis of QED then consists of two
steps. First, a general probability at T=0 is organized so that all the
virtual e±,γ are in the amplitudes and all the real
e±,γ are in the phase space integrations. Next, the cancellations
of IR divergences between virtual and real are demonstrated.Comment: 6 pages, (Talk presented at Quark Matter '93