Soliton versus the gas: Fredholm determinants, analysis, and the rapid oscillations behind the kinetic equation

Author:

Girotti Manuela1,Grava Tamara2,Jenkins Robert3,McLaughlin Ken T‐R4,Minakov Alexander5

Affiliation:

1. Saint Mary's University

2. SISSA INFN sezione di Trieste and University of Bristol

3. University of Central Florida

4. Tulane University

5. Univerzita Karlova

Abstract

AbstractWe analyse the case of a dense modified Korteweg–de Vries (mKdV) soliton gas and its large time behaviour in the presence of a single trial soliton. We show that the solution can be expressed in terms of Fredholm determinants as well as in terms of a Riemann–Hilbert problem. We then show that the solution can be decomposed as the sum of the background gas solution (a modulated elliptic wave), plus a soliton solution: the individual expressions are however quite convoluted due to the interaction dynamics. Additionally, we are able to derive the local phase shift of the gas after the passage of the soliton, and we can trace the location of the soliton peak as the dynamics evolves. Finally, we show that the soliton peak, while interacting with the soliton gas, has an oscillatory velocity whose leading order average value satisfies the kinetic velocity equation analogous to the one posited by V. Zakharov and G. El.

Funder

National Science Foundation

Natural Sciences and Engineering Research Council of Canada

Simons Foundation

Publisher

Wiley

Subject

Applied Mathematics,General Mathematics

Reference54 articles.

1. NIST digital library of mathematical functions http://dlmf.nist.gov/ Release 1.1.3 of 2021‐09‐15.F. W. J.Olver A. B.Olde Daalhuis D. W.Lozier B. I.Schneider R. F.Boisvert C. W.Clark B. R.Miller B. V.Saunders H. S.Cohl andM. A.McClain eds.

2. M. J.Ablowitz J. T.Cole G. A.El M. A.Hoefer andX.Luo Soliton‐mean field interaction in Korteweg‐de Vries dispersive hydrodynamics arXiv:2211.14884 2022.

3. Lectures on Integral Transforms

4. The largest real eigenvalue in the real Ginibre ensemble and its relation to the Zakharov–Shabat system

5. Scattering and inverse scattering for first order systems

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