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Volumn 3, Issue 3, 1996, Pages 874-888

Statistical description and transport in stochastic magnetic fields

Author keywords

[No Author keywords available]

Indexed keywords


EID: 0008439980     PISSN: 1070664X     EISSN: None     Source Type: Journal    
DOI: 10.1063/1.871791     Document Type: Article
Times cited : (19)

References (45)
  • 8
    • 0000655156 scopus 로고
    • Plasma Physics and Controlled Nuclear Fusion Research, Innsbruck, 1978 Internatinoal Atomic Energy Agency, Vienna
    • B. B. Kadomtsev and O. P. Pogutse, in Plasma Physics and Controlled Nuclear Fusion Research, Proceedings of the 7th International Conference, Innsbruck, 1978 (Internatinoal Atomic Energy Agency, Vienna, 1979), Vol. 1, p. 649.
    • (1979) Proceedings of the 7th International Conference , vol.1 , pp. 649
    • Kadomtsev, B.B.1    Pogutse, O.P.2
  • 31
    • 85033860988 scopus 로고    scopus 로고
    • note
    • It should be noted that the hybrid kinetic equation (3) can be coupled with the Maxwell equations, and, hence, allows a self-consistent treatment of the magnetic field. In contrast, the Langevin equations (2) are necessarily non-self-consistent. The self-consistency problem will not be considered here and the magnetic field properties will be specified a priori.
  • 39
    • 0001466688 scopus 로고
    • edited by M. N. Rosenbluth and R. Z. Sagdeev North-Holland, Amsterdam
    • J. A. Krommes, Handbook of Plasma Physics, edited by M. N. Rosenbluth and R. Z. Sagdeev (North-Holland, Amsterdam, 1984), Vol. 2, p. 183.
    • (1984) Handbook of Plasma Physics , vol.2 , pp. 183
    • Krommes, J.A.1
  • 45
    • 85033854273 scopus 로고    scopus 로고
    • note
    • Two comments about this result: The distribution function F depends on z, contrary to the density profile n(x;t) introduced in Ref. 33. The density profile n(x;t) of Ref. 33, defined with a different choice of normalization, must thus be identified with our reduced distribution function (32).


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.