<p>In this paper, we study the existence and multiplicity of normalized solutions to the quasilinear Schrödinger equation with prescribed mass where <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(N \ge 2, c&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo>≥</mo> <mn>2</mn> <mo>,</mo> <mi>c</mi> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> is a given constant, <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>λ</mi> </math></EquationSource> </InlineEquation> is a part of the unknown which arises as a Lagrange multiplier. The nonlinearity <i>g</i> is allowed to be strongly sublinear at the origin, i.e., <Equation ID="Equ31"> <EquationSource Format="TEX">\(\begin{aligned} \lim _{s \rightarrow 0} \frac{g(s)}{s}=-\infty , \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <munder> <mo movablelimits="true">lim</mo> <mrow> <mi>s</mi> <mo stretchy="false">→</mo> <mn>0</mn> </mrow> </munder> <mfrac> <mrow> <mi>g</mi> <mo stretchy="false">(</mo> <mi>s</mi> <mo stretchy="false">)</mo> </mrow> <mi>s</mi> </mfrac> <mo>=</mo> <mo>-</mo> <mi>∞</mi> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>which includes the logarithmic nonlinearity <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(g(s)=s \log s^2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>g</mi> <mrow> <mo stretchy="false">(</mo> <mi>s</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <mi>s</mi> <mo>log</mo> <msup> <mi>s</mi> <mn>2</mn> </msup> </mrow> </math></EquationSource> </InlineEquation>. The quasilinear term <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\Delta (u^2)u\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Δ</mi> <mo stretchy="false">(</mo> <msup> <mi>u</mi> <mn>2</mn> </msup> <mo stretchy="false">)</mo> <mi>u</mi> </mrow> </math></EquationSource> </InlineEquation> and the strongly sublinear term make the associated energy functional not well defined in <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(H^1(\mathbb {R}^N)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>H</mi> <mn>1</mn> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>. To overcome this difficulty, we use the dual approach and consider a family of approximating problems in <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(H^1(\mathbb {R}^N)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>H</mi> <mn>1</mn> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>. Then, we prove that such a family of solutions converges to a least-energy solution of the original problem. Additionally, under certain assumptions about <i>g</i> that allow us to work in a suitable subspace of <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(H^1(\mathbb {R}^N)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>H</mi> <mn>1</mn> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, we prove the existence of infinitely many solutions to <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\left( \mathcal {P}_\lambda \right) \)</EquationSource> <EquationSource Format="MATHML"><math> <mfenced close=")" open="("> <msub> <mi mathvariant="script">P</mi> <mi>λ</mi> </msub> </mfenced> </math></EquationSource> </InlineEquation>.</p>

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Normalized Solutions to Quasilinear Schrödinger Equations in the Strongly Sublinear Regime

  • Chao Ji,
  • Ning Yang

摘要

In this paper, we study the existence and multiplicity of normalized solutions to the quasilinear Schrödinger equation with prescribed mass where \(N \ge 2, c>0\) N 2 , c > 0 is a given constant, \(\lambda \) λ is a part of the unknown which arises as a Lagrange multiplier. The nonlinearity g is allowed to be strongly sublinear at the origin, i.e., \(\begin{aligned} \lim _{s \rightarrow 0} \frac{g(s)}{s}=-\infty , \end{aligned}\) lim s 0 g ( s ) s = - , which includes the logarithmic nonlinearity \(g(s)=s \log s^2\) g ( s ) = s log s 2 . The quasilinear term \(\Delta (u^2)u\) Δ ( u 2 ) u and the strongly sublinear term make the associated energy functional not well defined in \(H^1(\mathbb {R}^N)\) H 1 ( R N ) . To overcome this difficulty, we use the dual approach and consider a family of approximating problems in \(H^1(\mathbb {R}^N)\) H 1 ( R N ) . Then, we prove that such a family of solutions converges to a least-energy solution of the original problem. Additionally, under certain assumptions about g that allow us to work in a suitable subspace of \(H^1(\mathbb {R}^N)\) H 1 ( R N ) , we prove the existence of infinitely many solutions to \(\left( \mathcal {P}_\lambda \right) \) P λ .