2014
DOI: 10.1016/j.anihpc.2013.06.001
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On linear instability of solitary waves for the nonlinear Dirac equation

Abstract: Abstract. We consider the nonlinear Dirac equation, also known as the Soler model:We study the point spectrum of linearizations at solitary waves that bifurcate from NLS solitary waves in the limit ω → m, proving that if k > 2/n, then one positive and one negative eigenvalue are present in the spectrum of the linearizations at these solitary waves with ω sufficiently close to m, so that these solitary waves are linearly unstable. The approach is based on applying the Rayleigh-Schrödinger perturbation theory to… Show more

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Cited by 24 publications
(32 citation statements)
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“…This result is consistent with the rigorous analysis in the nonrelativistic limit [42]. The spectral analysis of the NLD equation was also recently studied [43].…”
Section: Introductionsupporting
confidence: 77%
“…This result is consistent with the rigorous analysis in the nonrelativistic limit [42]. The spectral analysis of the NLD equation was also recently studied [43].…”
Section: Introductionsupporting
confidence: 77%
“…In the nonrelativistic limit ω m, for k ∈ (0, 2), one has spectral stability according to [BC12b]; for k > 2, there is linear instability by [CGG14].…”
Section: The (Generalized) Massive Thirring Model In (1+1)d Is Characmentioning
confidence: 99%
“…In view of recent results on stability and instability for the nonlinear Dirac equation [CKMS10,BC12a,BC12b,CGG14] it is becoming clear that the VK criterion is still useful for the spinor systems in the nonrelativistic limit, when the amplitude of solitary waves is small. In particular, the ground states ("smallest energy solitary waves") in the charge-subcritical nonlinear Dirac equation (with the nonlinearity of order 2k + 1, with k < 2/n) are linearly stable in the nonrelativistic limit ω m, which corresponds to solitary waves of small amplitudes.…”
Section: Introductionmentioning
confidence: 99%
“…This approach seemed to violate the continuity argument that the nonlinear Dirac (NLD) equation becomes a modified nonlinear Schrödinger (NLS) equation when ω approaches the mass parameter m of the Dirac equation from below. This argument has been made more rigorous by Comech [14]. Comech (private communication) has been able to prove that for κ < 2 the Vakhitov-Kolokolov [15] criterion guarantees linear stability in the nonrelativistic regime of the NLD equation for solutions of the form (in the rest frame) (x,t) = ψ(x)e −iωt where ω is less than but approximately equal to m. He was also able to show linear instability in the same nonrelativistic regime for κ > 2.…”
Section: Introductionmentioning
confidence: 99%