Abstract

The conductivity of nonideal, fully ionized plasma is calculated under the assumption that there are no straight sections of electron trajectory. The trajectory consists of pieces of parabolic trajectories lying inside the Wigner–Seitz cell. The conductivity in this approximation is proportional to the plasma frequency and is close to the experimentally measured conductivity of a dense cesium plasma.

中文翻译：

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非理想全电离等离子体的等离子体频率，抛物线轨迹和电导率

摘要

非理想，完全电离的等离子体的电导率是在没有电子轨迹的直线部分的假设下计算的。该轨迹由位于Wigner-Seitz单元内的抛物线轨迹组成。在这种近似中，电导率与等离子体频率成正比，并且接近于实验测量的致密铯等离子体的电导率。