The electrical conductivity is calculated for partially ionized Li, Na, K, Rb, and Cs plasmas starting from quantum kinetic equations which account for collision terms of free and bound particles including many body effects. The scattering cross sections entering the conductivity are calculated in T matrix approximation. The description of electron-atom scattering is based on the close coupling system of equations considered in the adiabatic exchange model. The plasma composition is determined from generalized mass action laws valid for nonideal plasmas.
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Starzyński et al. (1996) studied this question.
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