2018
DOI: 10.1016/j.anihpc.2018.03.005
|View full text |Cite
|
Sign up to set email alerts
|

The Sine-Gordon regime of the Landau–Lifshitz equation with a strong easy-plane anisotropy

Abstract: We pursue our work on the asymptotic regimes of the Landau-Lifshitz equation for biaxial ferromagnets. We put the focus on the cubic Schrödinger equation, which is known to describe the dynamics in a regime of strong easy-axis anisotropy. In any dimension, we rigorously prove this claim for solutions with sufficient regularity. In this regime, we additionally classify the one-dimensional solitons of the Landau-Lifshitz equation and quantify their convergence towards the solitons of the one-dimensional cubic Sc… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
14
0

Year Published

2019
2019
2023
2023

Publication Types

Select...
7
1

Relationship

2
6

Authors

Journals

citations
Cited by 13 publications
(14 citation statements)
references
References 38 publications
0
14
0
Order By: Relevance
“…We also notice that other statements for Cauchy problem for the Gross-Pitaevskii equation have been established in different topologies when W = δ 0 (see e.g. [61,35,33,10,31,30] and the reference there in), and these results can probably be adapted to our nonlocal framework.…”
Section: Stabilitymentioning
confidence: 53%
“…We also notice that other statements for Cauchy problem for the Gross-Pitaevskii equation have been established in different topologies when W = δ 0 (see e.g. [61,35,33,10,31,30] and the reference there in), and these results can probably be adapted to our nonlocal framework.…”
Section: Stabilitymentioning
confidence: 53%
“…Real-valued solutions of (1.1) that initially are in H 1 sin × L 2 are preserved for all time, see e.g [17] and [52]. Additionally, they are globally well-defined thanks to the fact that sin(•) is a smooth bounded function.…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
“…Note that in Theorem 6.1 we do not specify the space where (φ, φ t ) are posed, this because (Q, 0)(t) in (1.5) does not belong to H 1 × L 2 . However, it is possible to show local and global well-posedness (LWP), such that H 1 ×L 2 perturbations are naturally allowed [17]. Remark 6.2 (Explicit examples).…”
Section: Now Recalling That H Satisfies the Equation Hmentioning
confidence: 99%
“…When 0 < α < 1, (LLG) is of parabolic type. We refer the reader to [40,29,32,33,12,14,15,13] and the references therein for more details and surveys on these equations.…”
Section: The Landau-lifshitz-gilbert Equation: Self-similar Solutionsmentioning
confidence: 99%