<p>We study a coupled dispersionless system in <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\((1+1)\)</EquationSource> </InlineEquation> dimensions with a time-dependent coefficient in the nonlinear coupling. The model consists of a real field <i>u</i>(<i>x</i>,&#xa0;<i>t</i>) and a complex field <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\psi (x,t)\)</EquationSource> </InlineEquation>, driven by a prescribed modulation function <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\alpha (t)\)</EquationSource> </InlineEquation>. A <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(2\times 2\)</EquationSource> </InlineEquation> Lax pair of Zakharov–Shabat type is constructed, showing that the system remains integrable with the temporal dependence confined to diagonal terms of the Lax matrices. Using a Darboux transformation adapted to this Lax pair, we derive Wronskian-type formulas for multi-soliton solutions and obtain explicit families of bright and dark traveling waves for several representative choices of <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\alpha (t)\)</EquationSource> </InlineEquation>. In addition, a time reparametrization transforms the model to an autonomous form whose traveling-wave reduction yields a planar Hamiltonian system with equilibria and phase portraits identical to the constant-coefficient coupled dispersionless equations. The modulation <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\alpha (t)\)</EquationSource> </InlineEquation> therefore leaves the intrinsic traveling-wave dynamics unchanged but reshapes how these waves are embedded in the (<i>x</i>,&#xa0;<i>t</i>)-plane, enabling management of soliton amplitudes, velocities and curved or oscillatory trajectories.</p>

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Soliton management in a variable-coefficient coupled dispersionless system via Darboux transformation

  • H. W. A. Riaz,
  • Y. Yildirim,
  • Altaf Alshuhail

摘要

We study a coupled dispersionless system in \((1+1)\) dimensions with a time-dependent coefficient in the nonlinear coupling. The model consists of a real field u(xt) and a complex field \(\psi (x,t)\) , driven by a prescribed modulation function \(\alpha (t)\) . A \(2\times 2\) Lax pair of Zakharov–Shabat type is constructed, showing that the system remains integrable with the temporal dependence confined to diagonal terms of the Lax matrices. Using a Darboux transformation adapted to this Lax pair, we derive Wronskian-type formulas for multi-soliton solutions and obtain explicit families of bright and dark traveling waves for several representative choices of \(\alpha (t)\) . In addition, a time reparametrization transforms the model to an autonomous form whose traveling-wave reduction yields a planar Hamiltonian system with equilibria and phase portraits identical to the constant-coefficient coupled dispersionless equations. The modulation \(\alpha (t)\) therefore leaves the intrinsic traveling-wave dynamics unchanged but reshapes how these waves are embedded in the (xt)-plane, enabling management of soliton amplitudes, velocities and curved or oscillatory trajectories.