<p>We consider the family of (poly)continua <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\mathcal {K}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="script">K</mi> </math></EquationSource> </InlineEquation> in the upper half-plane <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\({{\mathbb {H}}} \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="double-struck">H</mi> </math></EquationSource> </InlineEquation> that contain a preassigned finite <i>anchor</i> set <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(E\in {\mathbb {H}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>E</mi> <mo>∈</mo> <mi mathvariant="double-struck">H</mi> </mrow> </math></EquationSource> </InlineEquation>. For a given harmonic external field we define a Dirichlet energy functional <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\mathcal {I}(\mathcal {K})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="script">I</mi> <mo stretchy="false">(</mo> <mi mathvariant="script">K</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> and show that within each “connectivity class” of the family, there exists a minimizing compact <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\mathcal {K}^*\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="script">K</mi> </mrow> <mo>∗</mo> </msup> </math></EquationSource> </InlineEquation> consisting of critical trajectories of a quadratic differential. In many cases this quadratic differential coincides with the square of the real normalized quasimomentum differential <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\({\text {d}}{\textbf {p}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mtext>d</mtext> <mi mathvariant="bold">p</mi> </mrow> </math></EquationSource> </InlineEquation> associated with the finite gap solutions of the focusing Nonlinear Schrödinger equation (fNLS) defined by a hyperelliptic Riemann surface <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\mathfrak {R}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="fraktur">R</mi> </math></EquationSource> </InlineEquation> branched at the points <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(E\cup \bar{E}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>E</mi> <mo>∪</mo> <mover accent="true"> <mrow> <mi>E</mi> </mrow> <mrow> <mo stretchy="false">¯</mo> </mrow> </mover> </mrow> </math></EquationSource> </InlineEquation>. The motivation for this work lies in the problem of soliton condensate of least average intensity such that a given anchor set <i>E</i> belongs to the poly-continuum <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\mathcal {K}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="script">K</mi> </math></EquationSource> </InlineEquation>. An fNLS soliton condensate is defined by a compact <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\mathcal {K}\subset {{\mathbb {H}}} \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="script">K</mi> <mo>⊂</mo> <mi mathvariant="double-struck">H</mi> </mrow> </math></EquationSource> </InlineEquation> (its spectral support) whereas the average intensity of the condensate is proportional to <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\mathcal {I}(\mathcal {K})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="script">I</mi> <mo stretchy="false">(</mo> <mi mathvariant="script">K</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>. We prove that the spectral support <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(\mathcal {K}^*\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="script">K</mi> </mrow> <mo>∗</mo> </msup> </math></EquationSource> </InlineEquation> provides the fNLS soliton condensate of the least average intensity within a given “connectivity class”.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Dirichlet Energy and Focusing NLS Condensates of Minimal Intensity

  • Marco Bertola,
  • Alexander Tovbis

摘要

We consider the family of (poly)continua \(\mathcal {K}\) K in the upper half-plane \({{\mathbb {H}}} \) H that contain a preassigned finite anchor set \(E\in {\mathbb {H}}\) E H . For a given harmonic external field we define a Dirichlet energy functional \(\mathcal {I}(\mathcal {K})\) I ( K ) and show that within each “connectivity class” of the family, there exists a minimizing compact \(\mathcal {K}^*\) K consisting of critical trajectories of a quadratic differential. In many cases this quadratic differential coincides with the square of the real normalized quasimomentum differential \({\text {d}}{\textbf {p}}\) d p associated with the finite gap solutions of the focusing Nonlinear Schrödinger equation (fNLS) defined by a hyperelliptic Riemann surface \(\mathfrak {R}\) R branched at the points \(E\cup \bar{E}\) E E ¯ . The motivation for this work lies in the problem of soliton condensate of least average intensity such that a given anchor set E belongs to the poly-continuum \(\mathcal {K}\) K . An fNLS soliton condensate is defined by a compact \(\mathcal {K}\subset {{\mathbb {H}}} \) K H (its spectral support) whereas the average intensity of the condensate is proportional to \(\mathcal {I}(\mathcal {K})\) I ( K ) . We prove that the spectral support \(\mathcal {K}^*\) K provides the fNLS soliton condensate of the least average intensity within a given “connectivity class”.