1986
DOI: 10.1016/0370-1573(86)90016-5
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Soliton stability in plasmas and hydrodynamics

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Cited by 524 publications
(372 citation statements)
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“…Note that this stability indication is consistent with that for the cubic NLS solitons (V.8) which, as is well-known, are stable (see, e.g. [33]). Now we show that the lower soliton branch (µ < 0) is stable: solitons from this branch indeed realize a minimum of the Hamiltonian H for a fixed number of waves N .…”
supporting
confidence: 89%
“…Note that this stability indication is consistent with that for the cubic NLS solitons (V.8) which, as is well-known, are stable (see, e.g. [33]). Now we show that the lower soliton branch (µ < 0) is stable: solitons from this branch indeed realize a minimum of the Hamiltonian H for a fixed number of waves N .…”
supporting
confidence: 89%
“…(n, v +c, ϕ)(x −ct, t) and, respectively, (n, v, ϕ)(−x, −t) are solutions, if (n, v, ϕ)(x, t) is a solution. We refer to [15,21,29] and the references therein for more information on the physical background of these equations. A particular solution is found for constant density n ≡ 1, vanishing potential ϕ ≡ 0, and constant velocity v ≡ v 0 ; here v 0 is arbitrary due to Galilean invariance.…”
Section: Introductionmentioning
confidence: 99%
“…This system of equations, however, is generic and applies to a wide range of physical situations, including nonlinear, nonlocal media for which the response to a beam involves some sort of diffusive mechanism [35], for instance thermo-optic media [36] such as lead glasses [37][38][39] and photorefractive crystals [40]. A similar system of equations also arises in the so-called α models of turbulence [41,42].…”
Section: Introductionmentioning
confidence: 99%