Abstract
In the above paper, the plane-wave integral representation for well-stirred fields in reverberation chambers was extended to apply near the chamber walls. Several analytical terms for the mean of squared field magnitudes were derived. The formulas are inaccurate for describing the conditions near the chamber walls and need to be corrected, since they lead to non-physical negative values for the mean of squared magnitudes for small input values kx, ky, or kz.
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