<p>In this paper, we consider the Cauchy problem for the defocusing nonlinear Schr<InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\ddot{\text {o}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mover accent="true"> <mtext>o</mtext> <mo>¨</mo> </mover> </math></EquationSource> </InlineEquation>dinger equation with a finite genus algebro-geometric background. Long-time asymptotics of the solution are derived in four space-time regions. It comes out that the leading-order term in the expansion is, up to a constant, given by the background solution with a shift of the parameter. The subleading term, however, decays at different rates for different regions. We particularly highlight that in the two transition regions, they are of order <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\mathcal {O}(t^{-1/3})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="script">O</mi> <mo stretchy="false">(</mo> <msup> <mi>t</mi> <mrow> <mo>-</mo> <mn>1</mn> <mo stretchy="false">/</mo> <mn>3</mn> </mrow> </msup> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> and the coefficients involve an integral of the Painlevé XXXIV transcendent. We establish our results by applying a nonlinear steepest descent analysis to the associated Riemann–Hilbert problems.</p>

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Painlevé XXXIV asymptotics for the defocusing nonlinear Schrödinger equation with a finite-genus algebro-geometric background

  • Engui Fan,
  • Gaozhan Li,
  • Yiling Yang,
  • Lun Zhang

摘要

In this paper, we consider the Cauchy problem for the defocusing nonlinear Schr \(\ddot{\text {o}}\) o ¨ dinger equation with a finite genus algebro-geometric background. Long-time asymptotics of the solution are derived in four space-time regions. It comes out that the leading-order term in the expansion is, up to a constant, given by the background solution with a shift of the parameter. The subleading term, however, decays at different rates for different regions. We particularly highlight that in the two transition regions, they are of order \(\mathcal {O}(t^{-1/3})\) O ( t - 1 / 3 ) and the coefficients involve an integral of the Painlevé XXXIV transcendent. We establish our results by applying a nonlinear steepest descent analysis to the associated Riemann–Hilbert problems.