2017
DOI: 10.1088/1361-6544/aa6f29
|View full text |Cite
|
Sign up to set email alerts
|

Numerical study of blow-up and stability of line solitons for the Novikov–Veselov equation

Abstract: We study numerically the evolution of perturbed Korteweg-de Vries solitons and of well localized initial data by the Novikov-Veselov (NV) equation at different levels of the "energy" parameter E. We show that as |E| → ∞, NV behaves, as expected, similarly to its formal limit, the Kadomtsev-Petviashvili equation. However at intermediate regimes, i.e. when |E| is not very large, more varied scenarios are possible, in particular, blow-ups are observed. The mechanism of the blow-up is studied.

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
5
0

Year Published

2018
2018
2023
2023

Publication Types

Select...
5
2

Relationship

0
7

Authors

Journals

citations
Cited by 9 publications
(11 citation statements)
references
References 37 publications
0
5
0
Order By: Relevance
“…Our goal here is to study the time evolution of initial data that are not single peaked, but have the same maximum along a certain set, for example, an interval or a curve. In the wall-type data above (22) we have the maximum elongated in the y and z directions, and in the x-direction the maximum is still localized in a single point (at x = 0). The ZK evolution for such data with A = 3.6, a = 1.5 at t = 0.05, 0.2, 0.35 is shown in Fig.…”
Section: Soliton Resolutionmentioning
confidence: 75%
See 1 more Smart Citation
“…Our goal here is to study the time evolution of initial data that are not single peaked, but have the same maximum along a certain set, for example, an interval or a curve. In the wall-type data above (22) we have the maximum elongated in the y and z directions, and in the x-direction the maximum is still localized in a single point (at x = 0). The ZK evolution for such data with A = 3.6, a = 1.5 at t = 0.05, 0.2, 0.35 is shown in Fig.…”
Section: Soliton Resolutionmentioning
confidence: 75%
“…Figure 13. Soliton resolution and control parameters for the wall-type initial data (22). The profile of the solution at t = 5 (top left), time dependence of the L ∞ norm (top right), the difference of the solution at t = 5 and a rescaled soliton (bottom left), the Fourier coefficients at t = 5 (bottom right).…”
Section: Soliton Resolutionmentioning
confidence: 99%
“…18 indicate that it is resolved to the order of the rounding error. This means that (similar to the case of blow-up in the Novikov-Veselov equation [11]) the resolution is first lost in time (compare this to the case of blow-up solutions in DS II system [17], where the limiting factor is spatial resolution). The loss of resolution in time leads eventually to a breaking of the code.…”
Section: The L 2 -Critical Casementioning
confidence: 94%
“…Let φ q be a positive solution to the Schrodinger equation and let c ∞ be given by (18). By Nachman [28, lemma 3.5] for critical potentials and Music [26, theorem 1.4] for subcritical potentials with c ∞ = 0, we have that [I + G 0 * (q • )] is invertible for critical/subcritical q on W 1,p −β (R 2 ) for β > 2/p.…”
Section: Topology Of the Set Of Subcritical Potentialsmentioning
confidence: 99%
“…Moreover, the NV equation exhibits many dynamical phenomena that also occur for the KP equations. For example, the NV equation at nonzero energy has line soliton solutions and algebraic solitons (see [18] for a numerical study of the stability of such structures, their relationship with analogous structures for the KP I and KP II equations, and a review of the literature), while the NV equation at zero energy has a static lump solution. Thus, the zero-energy NV equation is part of a continuum of dispersive equations which exhibit important nonlinear wave phenomena and whose limits describe phenomena of physical interest.…”
Section: Introductionmentioning
confidence: 99%