<p>The inverse scattering transform for the defocusing <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1885_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="75" /> </InlineMediaObject> <EquationSource Format="TEX">\(N(N&gt;3)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo stretchy="false">(</mo> <mi>N</mi> <mo>&gt;</mo> <mn>3</mn> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>-component nonlinear Schrödinger equation with nonzero boundary conditions still remains open. In this paper, we investigate the inverse scattering analysis of the defocusing <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1885_Article_IEq2.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="75" /> </InlineMediaObject> <EquationSource Format="TEX">\(N(N\geqslant 2)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo stretchy="false">(</mo> <mi>N</mi> <mo>⩾</mo> <mn>2</mn> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>-component nonlinear Schrödinger equation with a special class of nonzero boundary conditions. Through two modified Lax pairs, the direct problem is shown to be well posed for a class of initial values. By introducing the tensor product and the generalized cross product, a complete set of analytic eigenfunctions and their symmetries are established for characterizing the inverse problem. It has been shown that the solution of the defocusing <i>N</i>-component nonlinear Schrödinger equation can be expressed in terms of the solution of a <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40840_2025_1885_Article_IEq3.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="39" /> </InlineMediaObject> <EquationSource Format="TEX">\(3\times 3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>3</mn> <mo>×</mo> <mn>3</mn> </mrow> </math></EquationSource> </InlineEquation> block matrix Riemann–Hilbert problem. In the reflectionless case, some soliton and breather solutions are obtained with graphical descriptions.</p>

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Inverse scattering transformation for defocusing N-component NLS with nonzero boundaries

  • Huan Liu,
  • Jing Shen,
  • Xianguo Geng

摘要

The inverse scattering transform for the defocusing \(N(N>3)\) N ( N > 3 ) -component nonlinear Schrödinger equation with nonzero boundary conditions still remains open. In this paper, we investigate the inverse scattering analysis of the defocusing \(N(N\geqslant 2)\) N ( N 2 ) -component nonlinear Schrödinger equation with a special class of nonzero boundary conditions. Through two modified Lax pairs, the direct problem is shown to be well posed for a class of initial values. By introducing the tensor product and the generalized cross product, a complete set of analytic eigenfunctions and their symmetries are established for characterizing the inverse problem. It has been shown that the solution of the defocusing N-component nonlinear Schrödinger equation can be expressed in terms of the solution of a \(3\times 3\) 3 × 3 block matrix Riemann–Hilbert problem. In the reflectionless case, some soliton and breather solutions are obtained with graphical descriptions.