<p>In this paper, we are concerned with the nonlinear Helmholtz system of Hamiltonian type <Equation ID="Equ50"> <EquationSource Format="TEX">\(\begin{aligned} \left\{ \begin{array}{l} -\Delta u-k^2 u=P(x)|v|^{p-2}v,\quad \text {in}\ \mathbb {R}^N, \\ -\Delta v-k^2v=Q(x)|u|^{q-2}u,\quad \text {in}\ \mathbb {R}^N, \end{array} \right. \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd columnalign="left"> <mrow> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mi>u</mi> <mo>-</mo> <msup> <mi>k</mi> <mn>2</mn> </msup> <mi>u</mi> <mo>=</mo> <mi>P</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <msup> <mrow> <mo stretchy="false">|</mo> <mi>v</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>p</mi> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>v</mi> <mo>,</mo> <mspace width="1em" /> <mtext>in</mtext> <mspace width="4pt" /> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> <mo>,</mo> </mrow> </mtd> </mtr> <mtr> <mtd columnalign="left"> <mrow> <mrow /> <mo>-</mo> <mi mathvariant="normal">Δ</mi> <mi>v</mi> <mo>-</mo> <msup> <mi>k</mi> <mn>2</mn> </msup> <mi>v</mi> <mo>=</mo> <mi>Q</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <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> <mi>u</mi> <mo>,</mo> <mspace width="1em" /> <mtext>in</mtext> <mspace width="4pt" /> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(N\ge 3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo>≥</mo> <mn>3</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(P,Q:\mathbb {R}^N\rightarrow \mathbb {R}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>P</mi> <mo>,</mo> <mi>Q</mi> <mo>:</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>N</mi> </msup> <mo stretchy="false">→</mo> <mi mathvariant="double-struck">R</mi> </mrow> </math></EquationSource> </InlineEquation> are two positive continuous functions, the exponents <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(p,q&gt;2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>,</mo> <mi>q</mi> <mo>&gt;</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation> satisfy <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\frac{1}{p}+\frac{1}{q}&gt;\frac{N-2}{N}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mfrac> <mn>1</mn> <mi>p</mi> </mfrac> <mo>+</mo> <mfrac> <mn>1</mn> <mi>q</mi> </mfrac> <mo>&gt;</mo> <mfrac> <mrow> <mi>N</mi> <mo>-</mo> <mn>2</mn> </mrow> <mi>N</mi> </mfrac> </mrow> </math></EquationSource> </InlineEquation>. First, we obtained the existence of a ground state solution via a dual variational method. Moreover, the concentration behavior of such dual ground state solutions is established as <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(k\rightarrow \infty \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>k</mi> <mo stretchy="false">→</mo> <mi>∞</mi> </mrow> </math></EquationSource> </InlineEquation>, where a rescaling technique and the generalized Birman–Schwinger operator are involved. In addition, we also investigated the relation between the number of solutions and the topology of the set of the global maxima of the functions <i>P</i> and <i>Q</i>.</p>

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Multiplicity and concentration of dual solutions for a Helmholtz system

  • Ruowen Qiu,
  • Fei Yuan,
  • Fukun Zhao

摘要

In this paper, we are concerned with the nonlinear Helmholtz system of Hamiltonian type \(\begin{aligned} \left\{ \begin{array}{l} -\Delta u-k^2 u=P(x)|v|^{p-2}v,\quad \text {in}\ \mathbb {R}^N, \\ -\Delta v-k^2v=Q(x)|u|^{q-2}u,\quad \text {in}\ \mathbb {R}^N, \end{array} \right. \end{aligned}\) - Δ u - k 2 u = P ( x ) | v | p - 2 v , in R N , - Δ v - k 2 v = Q ( x ) | u | q - 2 u , in R N , where \(N\ge 3\) N 3 , \(P,Q:\mathbb {R}^N\rightarrow \mathbb {R}\) P , Q : R N R are two positive continuous functions, the exponents \(p,q>2\) p , q > 2 satisfy \(\frac{1}{p}+\frac{1}{q}>\frac{N-2}{N}\) 1 p + 1 q > N - 2 N . First, we obtained the existence of a ground state solution via a dual variational method. Moreover, the concentration behavior of such dual ground state solutions is established as \(k\rightarrow \infty \) k , where a rescaling technique and the generalized Birman–Schwinger operator are involved. In addition, we also investigated the relation between the number of solutions and the topology of the set of the global maxima of the functions P and Q.