Abstract <p> Solutions of a generalized constrained discrete KP (gcdKP) hierarchy with the constraint <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11232_2025_2606_Article_IEq1.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="230" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^k=(L^k)_{\geq m}+\sum_{i=1}^lq_i\Delta^{-1}\Lambda^mr_i\)</EquationSource> </InlineEquation> on the Lax operator are investigated by Darboux transformations <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11232_2025_2606_Article_IEq2.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="153" /> </InlineMediaObject> <EquationSource Format="TEX">\(T_D(f)=f^{[1]}\cdot\Delta\cdot f^{-1}\)</EquationSource> </InlineEquation> and <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11232_2025_2606_Article_IEq3.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="183" /> </InlineMediaObject> <EquationSource Format="TEX">\(T_I(g)=(g^{[-1]})^{-1}\cdot\Delta^{-1}\cdot g\)</EquationSource> </InlineEquation>. Due to the special constraint on the Lax operator, it can be shown that the generating functions <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11232_2025_2606_Article_IEq4.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\(f\)</EquationSource> </InlineEquation> and <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11232_2025_2606_Article_IEq5.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(g\)</EquationSource> </InlineEquation> of the corresponding Darboux transformations can only be chosen from (adjoint) wave functions or <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11232_2025_2606_Article_IEq6.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="191" /> </InlineMediaObject> <EquationSource Format="TEX">\((L^k)_{&lt;m}=\sum_{i=1}^lq_i\Delta^{-1}\Lambda^mr_i\)</EquationSource> </InlineEquation>. We discuss successive application of Darboux transformations for the gcdKP hierarchy. Solutions of the gcdKP hierarchy are obtained from <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11232_2025_2606_Article_IEq7.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="64" /> </InlineMediaObject> <EquationSource Format="TEX">\(L^{\{0\}}=\Lambda\)</EquationSource> </InlineEquation> by Darboux transformations, with a method that is highly nontrivial due to the special constraint on the Lax operator. </p>

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Solutions of a generalized constrained discrete KP hierarchy

  • Xuepu Mu,
  • Mengyao Chen,
  • Jipeng Cheng,
  • Jingsong He

摘要

Abstract

Solutions of a generalized constrained discrete KP (gcdKP) hierarchy with the constraint \(L^k=(L^k)_{\geq m}+\sum_{i=1}^lq_i\Delta^{-1}\Lambda^mr_i\) on the Lax operator are investigated by Darboux transformations \(T_D(f)=f^{[1]}\cdot\Delta\cdot f^{-1}\) and \(T_I(g)=(g^{[-1]})^{-1}\cdot\Delta^{-1}\cdot g\) . Due to the special constraint on the Lax operator, it can be shown that the generating functions \(f\) and \(g\) of the corresponding Darboux transformations can only be chosen from (adjoint) wave functions or \((L^k)_{<m}=\sum_{i=1}^lq_i\Delta^{-1}\Lambda^mr_i\) . We discuss successive application of Darboux transformations for the gcdKP hierarchy. Solutions of the gcdKP hierarchy are obtained from \(L^{\{0\}}=\Lambda\) by Darboux transformations, with a method that is highly nontrivial due to the special constraint on the Lax operator.