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/content/aip/journal/pof1/5/5/10.1063/1.1706652
1.
1.H. Margenau, Phys. Rev. 109, 6 (1958).
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2.I. B. Bernstein and S. K. Trehan, Nuclear Fusion 1, 3 (1960).
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3.L. Spitzer, Jr., Physics of Fully Ionized Gases (Interscience Publishers, Inc., New York, 1956), p. 76.
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4.We shall take the uniform field results to apply for either long‐wavelength transverse or longitudinal plasma oscillations.
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5.P. A. G. Scheuer, Monthly Notices Roy. Astron. Soc. 120, 231 (1960).
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6.B. Fried and S. Conte, Space Technology Laboratory Rept. STL/TR‐60‐0000‐09216 (1960).
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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.
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8.O. Theimer and L. S. Taylor, Ann. Phys. (N.Y.) 11, 377 (1960).
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/content/aip/journal/pof1/5/5/10.1063/1.1706652
2004-12-09
2016-12-06
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