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/content/aip/journal/pof1/16/8/10.1063/1.1694506
1.
1.J. M. Berger, W. A. Newcomb, J. M. Dawson, E. A. Frieman, R. M. Kulsrud, and A. Lenard, Phys. Fluids 1, 301 (1958).
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2.A. Schlüter, Z. Naturforsch. 12A, 833 (1957).
3.
3.J. M. Dawson and M. F. Uman, Nucl. Fusion 5, 242 (1965).
4.
4.J. M. Dawson, N. K. Winsor, and E. C. Bowers, in Proceedings of the Fourth European Conference on Controlled Fusion and Plasma Physics (CNEN, Rome, 1970), p. 9.
5.
5.T. E. Stringer, Phys. Rev. Lett. 22, 770 (1969).
6.
6.M. N. Rosenbluth, P. H. Rutherford, J. B. Taylor, E. A. Frieman, and L. M. Kovrizhnikh, in Plasma Physics and Controlled Nuclear Fusion (International Atomic Energy Agency, Vienna, 1971), Vol. I, p. 495.
7.
7.See, for example, J. D. Jackson, Classical Electrodynamics (Wiley, New York, 1962), p. 411,
7.or L. L. Landau and E. Lifshitz, The Classical Theory of Fields (Addison‐Wesley, Reading, Mass., 1951), p. 180.
8.
8.See P. H. Rutherford and E. A. Frieman, Phys. Fluids 11, 569 (1968),
8.and J. B. Taylor and R. J. Hastie, Plasma Phys. 10, 479 (1968).
9.
9.M. N. Rosenbluth and J. B. Taylor, Phys. Rev. Lett. 23, 367 (1969).
10.
10.See, for example. L. I. Rudakov and R. Z. Sagdeev, Nucl. Fusion Suppl. 481 (1962);
10.B. B. Kadomtsev and O. P. Pogutse, in Reviews of Plasma Physics (Consultants Bureau, New York, 1970), Vol. 5, p. 249;
10.T. H. Stix, Phys. Fluids 10, 1601 (1967).
11.
11.T. H. Stix, Phys. Fluids (to be published).
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12.The neoclassical equilibrium‐state distribution functions are given by M. N. Rosenbluth, R. D. Hazeltine, and F. L. Hinton, Phys. Fluids 15, 116 (1972), Eqs. (180) and (181).
13.
13.J. D. Callen (private communication).
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2003-07-31
2016-09-29
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