1993
DOI: 10.1017/s0022377800017268
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Oblique nonlinear Alfvén waves in strongly magnetized beam plasmas. Part 1. Nonlinear vector evolution equation

Abstract: Nonlinear MHD waves propagating obliquely to the external magnetic field in warm multi-species plasmas with anisotropic pressures and different equilibrium drifts are treated without imposing the customary quasi-neutrality between the different species or neglecting the displacement current in Ampère's law. The wave magnetic field obeys a vector nonlinear evolution equation, which in the limits of parallel propagation or of both the neglect of the displacement current and the imposition of quasi-neutrality red… Show more

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Cited by 18 publications
(11 citation statements)
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References 16 publications
(14 reference statements)
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“…19 • On the contrary, the same model plays a fundamental role in plasma physics. In warm multi-species plasmas with anisotropic pressures and different equilibrium drifts, coupled DNLSEs govern the oblique propagation of nonlinear magnetohydrodynamic waves relative to an external magnetic field under certain conditions, dropping the quasi-neutrality assumption [20]. If Alfvén waves in a magnetized plasma bear both right and left circular polarizations, the equations for the respective amplitudes lead to the system of DNLSEs in the form of Eq.…”
Section: Gauge Transformations and Applicationsmentioning
confidence: 99%
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“…19 • On the contrary, the same model plays a fundamental role in plasma physics. In warm multi-species plasmas with anisotropic pressures and different equilibrium drifts, coupled DNLSEs govern the oblique propagation of nonlinear magnetohydrodynamic waves relative to an external magnetic field under certain conditions, dropping the quasi-neutrality assumption [20]. If Alfvén waves in a magnetized plasma bear both right and left circular polarizations, the equations for the respective amplitudes lead to the system of DNLSEs in the form of Eq.…”
Section: Gauge Transformations and Applicationsmentioning
confidence: 99%
“…(1). For a weak noise level of 1%, the configurations of both the 'elevation-elevation' and 'elevation -four-petal' types exhibit reasonable robustness, in the sense that the growth phase of the 20 RWs persists in an essentially unaffected form on top of only a mildly disturbed background (Figs. 9 and 10).…”
Section: Numerical Studies On the Effects Of Perturbationsmentioning
confidence: 99%
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“…The methods described in this paper can be applied to other equations not mentioned in Sections 4 and 6. Some other examples include: the KdV equation, Hirota's equation (or the mixed generalized NLS‐generalized mKdV equation) 23,34 , the Modified Vector dNLS equation, 35 the Massive Thirring Model, 36 the O4 nonlinear σ‐model, 37 the complex reverse space‐time nonlocal mKdV equation, 38 and the reverse space‐time nonlocal generalized sine‐Gordon equations 38 …”
Section: Resultsmentioning
confidence: 99%
“…The DNLS can account for oblique propagation, provided α is zero, i.e. imposing charge neutrality to all orders and neglecting the displacement current in Ampère's law (Deconinck, Meuris and Verheest 1993a). The bothersome third term in (1) also disappears if B ⊥0 is zero, in the case of strictly parallel propagation.…”
Section: Mvdnlsmentioning
confidence: 99%