<p>We are interested in the following critical biharmonic Schrödinger equation <Equation ID="Equ65"> <EquationSource Format="TEX">\( \left\{ \begin{array}{ll} \Delta ^2 u+\lambda u=g(u)+|u|^{4^*-2}u \,\,\,\, \text{ in }\,\,\, \mathbb {R}^{N}, \\ \int _{\mathbb {R}^N}|u|^2 dx=c, \end{array}\right. \)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mrow> <msup> <mi mathvariant="normal">Δ</mi> <mn>2</mn> </msup> <mi>u</mi> <mo>+</mo> <mi>λ</mi> <mi>u</mi> <mo>=</mo> <mi>g</mi> <mrow> <mo stretchy="false">(</mo> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> <mo>+</mo> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <msup> <mn>4</mn> <mo>∗</mo> </msup> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> <mspace width="0.166667em" /> <mspace width="0.166667em" /> <mspace width="0.166667em" /> <mspace width="0.166667em" /> <mspace width="0.333333em" /> <mtext>in</mtext> <mspace width="0.333333em" /> <mspace width="0.166667em" /> <mspace width="0.166667em" /> <mspace width="0.166667em" /> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <msub> <mo>∫</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> </msub> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mn>2</mn> </msup> <mi>d</mi> <mi>x</mi> <mo>=</mo> <mi>c</mi> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </math></EquationSource> </Equation>where <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(5\le N\le 7\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>5</mn> <mo>≤</mo> <mi>N</mi> <mo>≤</mo> <mn>7</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(4^*:=\frac{2N}{N-4}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mn>4</mn> <mo>∗</mo> </msup> <mo>:</mo> <mo>=</mo> <mfrac> <mrow> <mn>2</mn> <mi>N</mi> </mrow> <mrow> <mi>N</mi> <mo>-</mo> <mn>4</mn> </mrow> </mfrac> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(c&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>c</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\lambda \in \mathbb {R}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>λ</mi> <mo>∈</mo> <mi mathvariant="double-struck">R</mi> </mrow> </math></EquationSource> </InlineEquation> appears as a Lagrange multiplier. The novelty of this paper is that, under a class of general mass-supercritical conditions on <i>g</i>(<i>u</i>), we obtain the existence of ground state solutions and derive an asymptotic behavior of the ground state energy as <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(c\rightarrow +\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>c</mi> <mo stretchy="false">→</mo> <mo>+</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation>. The key ingredient of our proof relies on an alternative criterion and some subtle energy estimation technique. Some recent results are generalized and improved significantly.</p>

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Normalized Ground State Solutions for Critical Biharmonic Schrödinger Equations with General Mass-Supercritical Nonlinear Perturbation

  • Ying Wang,
  • Ziheng Zhang

摘要

We are interested in the following critical biharmonic Schrödinger equation \( \left\{ \begin{array}{ll} \Delta ^2 u+\lambda u=g(u)+|u|^{4^*-2}u \,\,\,\, \text{ in }\,\,\, \mathbb {R}^{N}, \\ \int _{\mathbb {R}^N}|u|^2 dx=c, \end{array}\right. \) Δ 2 u + λ u = g ( u ) + | u | 4 - 2 u in R N , R N | u | 2 d x = c , where \(5\le N\le 7\) 5 N 7 , \(4^*:=\frac{2N}{N-4}\) 4 : = 2 N N - 4 , \(c>0\) c > 0 and \(\lambda \in \mathbb {R}\) λ R appears as a Lagrange multiplier. The novelty of this paper is that, under a class of general mass-supercritical conditions on g(u), we obtain the existence of ground state solutions and derive an asymptotic behavior of the ground state energy as \(c\rightarrow +\infty \) c + . The key ingredient of our proof relies on an alternative criterion and some subtle energy estimation technique. Some recent results are generalized and improved significantly.