2017
DOI: 10.1007/s11005-017-0941-3
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Spectral stability of periodic waves in the generalized reduced Ostrovsky equation

Abstract: We consider stability of periodic travelling waves in the generalized reduced Ostrovsky equation with respect to co-periodic perturbations. Compared to the recent literature, we give a simple argument that proves spectral stability of all smooth periodic travelling waves independent of the nonlinearity power. The argument is based on the energy convexity and does not use coordinate transformations of the reduced Ostrovsky equations to the semi-linear equations of the Klein–Gordon type.

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Cited by 25 publications
(41 citation statements)
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“…Most of the content in Section 4.1 is contained in some recent papers, but we summarize it for the readers' convenience. Note that our reasoning applies equally well to both the fourth-and second-order versions of the eigenvalue problems, see (15) and (16).…”
Section: Stabilit Y Of the Wavessupporting
confidence: 59%
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“…Most of the content in Section 4.1 is contained in some recent papers, but we summarize it for the readers' convenience. Note that our reasoning applies equally well to both the fourth-and second-order versions of the eigenvalue problems, see (15) and (16).…”
Section: Stabilit Y Of the Wavessupporting
confidence: 59%
“…A full description of its periodic waves as well their stability can be found in the recent papers. 15,16 For the full Ostrovsky model under consideration, Liu and Ohta, 17 and by a slightly different method, Liu 18 have established the orbital stability for the classical Ostrovsky's equation (i.e., = 2) for large speeds. Another set of stability result, sometimes referred to as weak orbital stability, is given in Ref.…”
Section: Stability Resultsmentioning
confidence: 99%
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“…Spectral stability of smooth periodic waves with respect to perturbations of the same period was proven both for (1.1) and (1.2) in [7,14]. The analysis of [7] relies on the standard variational formulation of the periodic waves as critical points of energy subject to fixed momentum. The analysis of [14] relies on the coordinate transformation (1.7), which reduces the spectral stability problem of the form ∂ x Lv = λv with the self-adjoint operator L = c − U p + ∂ −2 z to the spectral problem of the form M v = λ∂ ξ v with the self-adjoint operator M = c − u p + ∂ 2 ξ .…”
Section: Introductionmentioning
confidence: 99%
“…The works [5,15] and [21] both exploit the integrable structure, so our result could be considered an alternate proof which does not uses integrability, but instead relies mainly on an invariant subspace decomposition and an elementary Krein-signature-type argument. See also the recent work [16] for related arguments.…”
mentioning
confidence: 96%