Abstract:We study the periodic traveling wave solutions of the derivative nonlinear Schrödinger equation (DNLS). It is known that DNLS has two types of solitons on the whole line; one has exponential decay and the other has algebraic decay. The latter corresponds to the soliton for the massless case. In the new global results recently obtained by Fukaya, Hayashi and Inui [15], the properties of two-parameter of the solitons are essentially used in the proof, and especially the soliton for the massless case plays an imp… Show more
“…where s * := −γ/(1 − γ) and γ := 1 + 16 3 b. We note that the value b = −3/16 gives the turning point in the structure of the solitons.…”
Section: Dnls and Mass Critical Nlsmentioning
confidence: 96%
“…There is a large literature on the Cauchy problem for (DNLS); see [38,39,19,20,36,3,8,9,42,43,15,11,16,23,24] and references therein. Here we are mainly interested in the results of energy space H 1 (R).…”
Section: Dnls and Mass Critical Nlsmentioning
confidence: 99%
“…where γ = 1 + 16 3 b. From Φ ω,c ∈ H 1 (R) and the equation (2.5), one can show that Im Φ ω,c Φ ω,c = 0 (see [7,Lemma 2]).…”
Section: Solitons and Conserved Quantitiesmentioning
We consider the following nonlinear Schrödinger equation of derivative type:(1)this equation is known as a standard derivative nonlinear Schrödinger equation (DNLS), which is mass critical and completely integrable. The equation (1) can be considered as a generalized equation of DNLS while preserving mass criticality and Hamiltonian structure. For DNLS it is known that if the initial data u 0 ∈ H 1 (R) satisfies the mass condition u 0 2 L 2 < 4π, the corresponding solution is global and bounded. In this paper we first establish the mass condition on (1) for general b ∈ R, which is exactly corresponding to 4π-mass condition for DNLS, and then characterize it from the viewpoint of potential well theory. We see that the mass threshold value gives the turning point in the structure of potential well generated by solitons. In particular, our results for DNLS give a characterization of both 4π-mass condition and algebraic solitons.
“…where s * := −γ/(1 − γ) and γ := 1 + 16 3 b. We note that the value b = −3/16 gives the turning point in the structure of the solitons.…”
Section: Dnls and Mass Critical Nlsmentioning
confidence: 96%
“…There is a large literature on the Cauchy problem for (DNLS); see [38,39,19,20,36,3,8,9,42,43,15,11,16,23,24] and references therein. Here we are mainly interested in the results of energy space H 1 (R).…”
Section: Dnls and Mass Critical Nlsmentioning
confidence: 99%
“…where γ = 1 + 16 3 b. From Φ ω,c ∈ H 1 (R) and the equation (2.5), one can show that Im Φ ω,c Φ ω,c = 0 (see [7,Lemma 2]).…”
Section: Solitons and Conserved Quantitiesmentioning
We consider the following nonlinear Schrödinger equation of derivative type:(1)this equation is known as a standard derivative nonlinear Schrödinger equation (DNLS), which is mass critical and completely integrable. The equation (1) can be considered as a generalized equation of DNLS while preserving mass criticality and Hamiltonian structure. For DNLS it is known that if the initial data u 0 ∈ H 1 (R) satisfies the mass condition u 0 2 L 2 < 4π, the corresponding solution is global and bounded. In this paper we first establish the mass condition on (1) for general b ∈ R, which is exactly corresponding to 4π-mass condition for DNLS, and then characterize it from the viewpoint of potential well theory. We see that the mass threshold value gives the turning point in the structure of potential well generated by solitons. In particular, our results for DNLS give a characterization of both 4π-mass condition and algebraic solitons.
“…The connection of solitons with two different decays for (DNLS) has been studied in [19,20], where the proofs depend on the explicit formulae of solitons, which is not applicable to at least higher-dimensional case in our setting. Here we use variational characterization of ground states effectively for the proof of Theorem 1.4.…”
Section: Stability Properties Of Standing Wavesmentioning
We consider nonlinear Schrödinger equations with double power nonlinearities which are defocusing and focusing. This equation has two types of standing waves: one decays exponentially, and the other decays only algebraically. In this paper we study instability and strong instability of standing waves including algebraic standing waves. We improve the instability results in previous works in one-dimensional case, and moreover establish new instability results in higher-dimensional case. The key point in our approach is to take advantage of variational characterization of algebraic standing waves. Contents 1. Introduction 1.1. Setting of the problem 1.2. Ground states on zero mass case 1.3. Stability properties of standing waves 1.4. Main results 1.5. Outline of the paper 2. Properties of ground states 2.1. Variational characterization 2.2. Characterization of ground states 2.3. Decay estimates 3. Connection between two types of standing waves 4. Strong instability for the case q ≥ 1 + 4/N 4.1. Blowup 4.2. Strong instability 5. Instability for the case q < 1 + 4/N 5.1. Sufficient conditions for instability 5.2. Instability for algebraic standing waves 5.3. Instability of standing waves for small ω Appendix A. Radial compactness lemma Appendix B. Revisit on the stability theory for large ω
“…Such solutions are generally quasi-periodic when they are expressed in the polar form φ ω,ν = R ω,ν e iΘω,ν with R ω,ν and Θ ω,ν being periodic with the same period L. The simplest periodic standing wave solutions to the DNLS equation (1.1) can be analyzed directly by separating the variables in the polar form [15]. Convergence of periodic waves to the solitary waves (1.5) was shown in [21]. Spectral stability of periodic waves with non-vanishing φ ω,c was established with respect to perturbations of the same period in [20].…”
We consider the periodic standing waves in the derivative nonlinear Schrödinger (DNLS) equation arising in plasma physics. By using a newly developed algebraic method with two eigenvalues, we classify all periodic standing waves in terms of eight eigenvalues of the Kaup-Newell spectral problem located at the end points of the spectral bands outside the real line. The analytical work is complemented with the numerical approximation of the spectral bands, this enables us to fully characterize the modulational instability of the periodic standing waves in the DNLS equation.
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