<p>This paper is devoted to studying the mass concentration behavior of <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(L^2\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>L</mi> <mn>2</mn> </msup> </math></EquationSource> </InlineEquation>-norm prescribed minimizers for the Gross-Pitaevskii energy functional with a mass subcritical perturbation <Equation ID="Equ41"> <EquationSource Format="TEX">\( E_a(u)=\int _{\mathbb {R}^2}|\nabla u|^2\textrm{d}x+\int _{\mathbb {R}^2}V(x)|u|^2\textrm{d}x -\frac{a}{2}\int _{\mathbb {R}^2}|u|^4\textrm{d}x-\frac{2\mu _a}{q+2}\int _{\mathbb {R}^2}|u|^{q+2}\textrm{d}x, \)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <msub> <mi>E</mi> <mi>a</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <msub> <mo>∫</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>2</mn> </msup> </msub> <msup> <mrow> <mo stretchy="false">|</mo> <mi mathvariant="normal">∇</mi> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mn>2</mn> </msup> <mtext>d</mtext> <mi>x</mi> <mo>+</mo> <msub> <mo>∫</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>2</mn> </msup> </msub> <msup> <mrow> <mi>V</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mn>2</mn> </msup> <mtext>d</mtext> <mi>x</mi> <mo>-</mo> <mfrac> <mi>a</mi> <mn>2</mn> </mfrac> <msub> <mo>∫</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>2</mn> </msup> </msub> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mn>4</mn> </msup> <mtext>d</mtext> <mi>x</mi> <mo>-</mo> <mfrac> <mrow> <mn>2</mn> <msub> <mi>μ</mi> <mi>a</mi> </msub> </mrow> <mrow> <mi>q</mi> <mo>+</mo> <mn>2</mn> </mrow> </mfrac> <msub> <mo>∫</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>2</mn> </msup> </msub> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>q</mi> <mo>+</mo> <mn>2</mn> </mrow> </msup> <mtext>d</mtext> <mi>x</mi> <mo>,</mo> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(0&lt;q&lt;2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>0</mn> <mo>&lt;</mo> <mi>q</mi> <mo>&lt;</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(a&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>a</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\mu _a\ge 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>μ</mi> <mi>a</mi> </msub> <mo>≥</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> is a small parameter depending on <i>a</i> and <i>V</i>(<i>x</i>) is a trapping potential. It is shown that there is a constant <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(a^*&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>a</mi> <mo>∗</mo> </msup> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> such that the minimizer exists if <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(a&lt;a^*\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>a</mi> <mo>&lt;</mo> <msup> <mi>a</mi> <mo>∗</mo> </msup> </mrow> </math></EquationSource> </InlineEquation> and the minimizer does not exist if <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(a=a^*\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>a</mi> <mo>=</mo> <msup> <mi>a</mi> <mo>∗</mo> </msup> </mrow> </math></EquationSource> </InlineEquation>. By establishing the delicate estimate on the minimal energy, we give a detailed description of limit behavior for minimizers as <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(a\nearrow a^*\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>a</mi> <mo>↗</mo> <msup> <mi>a</mi> <mo>∗</mo> </msup> </mrow> </math></EquationSource> </InlineEquation>, which implies that the minimizers must concentrate at the flattest global minimum of the trapping potential. Finally, we prove the local uniqueness of minimizers when <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(a&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>a</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> is sufficiently close to <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(a^*\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>a</mi> <mo>∗</mo> </msup> </math></EquationSource> </InlineEquation>. In particular, if <i>V</i>(<i>x</i>) is a radial function, the local uniqueness still holds when <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\mu _a=const&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>μ</mi> <mi>a</mi> </msub> <mo>=</mo> <mi>c</mi> <mi>o</mi> <mi>n</mi> <mi>s</mi> <mi>t</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>.</p>

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Limit behavior of minimizers for the Gross-Pitaevskii functional with a mass subcritical perturbation

  • Chen Yang,
  • Shubin Yu,
  • Chun-Lei Tang

摘要

This paper is devoted to studying the mass concentration behavior of \(L^2\) L 2 -norm prescribed minimizers for the Gross-Pitaevskii energy functional with a mass subcritical perturbation \( E_a(u)=\int _{\mathbb {R}^2}|\nabla u|^2\textrm{d}x+\int _{\mathbb {R}^2}V(x)|u|^2\textrm{d}x -\frac{a}{2}\int _{\mathbb {R}^2}|u|^4\textrm{d}x-\frac{2\mu _a}{q+2}\int _{\mathbb {R}^2}|u|^{q+2}\textrm{d}x, \) E a ( u ) = R 2 | u | 2 d x + R 2 V ( x ) | u | 2 d x - a 2 R 2 | u | 4 d x - 2 μ a q + 2 R 2 | u | q + 2 d x , where \(0<q<2\) 0 < q < 2 , \(a>0\) a > 0 , \(\mu _a\ge 0\) μ a 0 is a small parameter depending on a and V(x) is a trapping potential. It is shown that there is a constant \(a^*>0\) a > 0 such that the minimizer exists if \(a<a^*\) a < a and the minimizer does not exist if \(a=a^*\) a = a . By establishing the delicate estimate on the minimal energy, we give a detailed description of limit behavior for minimizers as \(a\nearrow a^*\) a a , which implies that the minimizers must concentrate at the flattest global minimum of the trapping potential. Finally, we prove the local uniqueness of minimizers when \(a>0\) a > 0 is sufficiently close to \(a^*\) a . In particular, if V(x) is a radial function, the local uniqueness still holds when \(\mu _a=const>0\) μ a = c o n s t > 0 .