1979
DOI: 10.1007/bf00670060
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Stability of charged solitons

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Cited by 19 publications
(16 citation statements)
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“…so that (3.32) As a preparatory step, following the papers (Movchan 1960, Kumar, Nisichenko andMakhankov 1990) According to the general theorem in the theory of stability (Zubov 1957;Malkin 1962) The proof was based on the apparent negativeness of the second variation (derivative) in some neighbourhood of static soliton solutions under scale perturbations 6<p = xio;u.…”
Section: Example 31 Complex Scalar Fields With Harmonic Time-dependmentioning
confidence: 99%
“…so that (3.32) As a preparatory step, following the papers (Movchan 1960, Kumar, Nisichenko andMakhankov 1990) According to the general theorem in the theory of stability (Zubov 1957;Malkin 1962) The proof was based on the apparent negativeness of the second variation (derivative) in some neighbourhood of static soliton solutions under scale perturbations 6<p = xio;u.…”
Section: Example 31 Complex Scalar Fields With Harmonic Time-dependmentioning
confidence: 99%
“…where ξ( x) = a( x) + b * ( x) and η( x) = a( x) − b * ( x). The structure of solutions (39) and (44), together with the form of nonlinear equation of motion (8), suggests that the nonlinear overlap term between these modes κ × (t, x) has the form…”
Section: Overlap Terms Between Oscillation and Nonoscillation Modesmentioning
confidence: 99%
“…where the real parameter α ≪ 1 is introduced for convenience and can be considered as the expansion parameter (in such a case, the functions ψ 1,n (t, x) and ψ 2,n (t, x) can be considered to be of the order of f (r)). Here ψ 1,n (t, x) satisfies the linearized equation of motion, following from (8). The standard ansatz for ψ 1,n (t, x) has the form [16,17]…”
Section: Introductionmentioning
confidence: 99%
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