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High‐Frequency Conductivity and the Emission and Absorption Coefficients of a Fully Ionized Plasma
1.H. Margenau, Phys. Rev. 109, 6 (1958).
2.I. B. Bernstein and S. K. Trehan, Nuclear Fusion 1, 3 (1960).
3.L. Spitzer, Jr., Physics of Fully Ionized Gases (Interscience Publishers, Inc., New York, 1956), p. 76.
4.We shall take the uniform field results to apply for either long‐wavelength transverse or longitudinal plasma oscillations.
5.P. A. G. Scheuer, Monthly Notices Roy. Astron. Soc. 120, 231 (1960).
6.B. Fried and S. Conte, Space Technology Laboratory Rept. STL/TR‐60‐0000‐09216 (1960).
7.The assignment of energy per mode in thermal equilibrium can be justified by a thought experiment in which a bounded plasma is embedded in a vacuum thermal radiation field.
8.O. Theimer and L. S. Taylor, Ann. Phys. (N.Y.) 11, 377 (1960).
9.V. P. Silin, Soviet Phys.‐JETP 11, 1277 (1960).
10.S. Yoshikawa, M.I.T. Ph.D. thesis, unpublished (1961).
11.L. Oster, Revs. Modern Phys. 33, 525 (1961).
12.N. Rostoker and M. N. Rosenbluth, Phys. Fluids 3, 1 (1960).
13.N. Rostoker, Nuclear Fusion 1, 101 (1961).
14.R. L. Guernsey, Phys. Fluids 5, 322 (1962).
15.S. F. Edwards and J. J. Sanderson, Phil. Mag. 6, 71 (1960).
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