Abstract
Electron-electron bremsstrahlung in a weakly ionized uniform non-stationary plasma is investigated. The respective problem is solved analytically for two initial electron-distributions: maxwellian with the temperatureT0, and the delta distribution. In the case of initial maxwellian distribution the radiation intensity is proportional toΘ3/2, whereΘ=T+(T0−T) exp (−s),s=2mv1t/M,v1 is the momentum transfer frequency, and the other symbols are standard. In the case of initial delta distribution the radiation intensity is proportional to [1 -exp (−s)]3/2. The proportionality factors are known, and are expressed in terms of mathematical and physical constants.
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