<p>In this paper, we study the following (<i>p</i>,<i>q</i>)-Laplacian equation: <Equation ID="Equ65"> <EquationSource Format="TEX">\(\left\{ \begin{aligned}&amp;-\Delta _{p}u - \Delta _{q}u = \lambda |u|^{p-2}u + |u|^{\overline{q}-2}u + \mu |u|^{t-2}u,&amp;\int _{\mathbb {R}^{N}} |u|^{p}dx = a^{p}, \end{aligned} \right. \)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mfenced open="{"> <mrow> <mtable> <mtr> <mtd /> <mtd columnalign="left"> <mrow> <mo>-</mo> <msub> <mi mathvariant="normal">Δ</mi> <mi>p</mi> </msub> <mi>u</mi> <mo>-</mo> <msub> <mi mathvariant="normal">Δ</mi> <mi>q</mi> </msub> <mi>u</mi> <mo>=</mo> <msup> <mrow> <mi>λ</mi> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>p</mi> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> <mo>+</mo> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mover> <mi>q</mi> <mo>¯</mo> </mover> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> <mo>+</mo> <mi>μ</mi> <msup> <mrow> <mo stretchy="false">|</mo> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>t</mi> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mi>u</mi> <mo>,</mo> </mrow> </mtd> <mtd columnalign="right"> <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> <mi>p</mi> </msup> <mi>d</mi> <mi>x</mi> <mo>=</mo> <msup> <mi>a</mi> <mi>p</mi> </msup> <mo>,</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </mfenced> </math></EquationSource> </Equation>where <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(1&lt; p&lt; q &lt; N\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1</mn> <mo>&lt;</mo> <mi>p</mi> <mo>&lt;</mo> <mi>q</mi> <mo>&lt;</mo> <mi>N</mi> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\Delta _{i} = \text {div}(|\nabla u|^{i-2} \nabla u)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="normal">Δ</mi> <mi>i</mi> </msub> <mo>=</mo> <msup> <mrow> <mtext>div</mtext> <mo stretchy="false">(</mo> <mo stretchy="false">|</mo> <mi mathvariant="normal">∇</mi> <mi>u</mi> <mo stretchy="false">|</mo> </mrow> <mrow> <mi>i</mi> <mo>-</mo> <mn>2</mn> </mrow> </msup> <mrow> <mi mathvariant="normal">∇</mi> <mi>u</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> for <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(i \in \{ p, q \}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>i</mi> <mo>∈</mo> <mo stretchy="false">{</mo> <mi>p</mi> <mo>,</mo> <mi>q</mi> <mo stretchy="false">}</mo> </mrow> </math></EquationSource> </InlineEquation> is the <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(i\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>i</mi> </math></EquationSource> </InlineEquation>-Laplacian operator, <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>λ</mi> </math></EquationSource> </InlineEquation> is a Lagrange multiplier, <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\overline{q} = q + \frac{pq}{N}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mover> <mi>q</mi> <mo>¯</mo> </mover> <mo>=</mo> <mi>q</mi> <mo>+</mo> <mfrac> <mrow> <mi mathvariant="italic">pq</mi> </mrow> <mi>N</mi> </mfrac> </mrow> </math></EquationSource> </InlineEquation> is the <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(L^p\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>L</mi> <mi>p</mi> </msup> </math></EquationSource> </InlineEquation>-critical exponent, <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\mu \in \mathbb {R}^{+}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>μ</mi> <mo>∈</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mo>+</mo> </msup> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(p&lt; t &lt; p^{*} = \frac{Np}{N-p}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>&lt;</mo> <mi>t</mi> <mo>&lt;</mo> <msup> <mi>p</mi> <mrow> <mrow /> <mo>∗</mo> </mrow> </msup> <mo>=</mo> <mfrac> <mrow> <mi mathvariant="italic">Np</mi> </mrow> <mrow> <mi>N</mi> <mo>-</mo> <mi>p</mi> </mrow> </mfrac> </mrow> </math></EquationSource> </InlineEquation>. In the <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(L^p\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>L</mi> <mi>p</mi> </msup> </math></EquationSource> </InlineEquation>-critical case, the different values of <i>t</i> affect the geometric structure of the functional corresponding to the equation. The purpose of this paper is to establish the existence of radial normalized solution on different <i>t</i>.</p>

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Normalized solutions for (p,q)-Laplacian equations with combined nonlinearities: the \(L^{p}\)-critical case

  • Jian-Hui Deng,
  • Xin Qiu,
  • Zeng-Qi Ou,
  • Ying Lv

摘要

In this paper, we study the following (p,q)-Laplacian equation: \(\left\{ \begin{aligned}&-\Delta _{p}u - \Delta _{q}u = \lambda |u|^{p-2}u + |u|^{\overline{q}-2}u + \mu |u|^{t-2}u,&\int _{\mathbb {R}^{N}} |u|^{p}dx = a^{p}, \end{aligned} \right. \) - Δ p u - Δ q u = λ | u | p - 2 u + | u | q ¯ - 2 u + μ | u | t - 2 u , R N | u | p d x = a p , where \(1< p< q < N\) 1 < p < q < N , \(\Delta _{i} = \text {div}(|\nabla u|^{i-2} \nabla u)\) Δ i = div ( | u | i - 2 u ) for \(i \in \{ p, q \}\) i { p , q } is the \(i\) i -Laplacian operator, \(\lambda \) λ is a Lagrange multiplier, \(\overline{q} = q + \frac{pq}{N}\) q ¯ = q + pq N is the \(L^p\) L p -critical exponent, \(\mu \in \mathbb {R}^{+}\) μ R + and \(p< t < p^{*} = \frac{Np}{N-p}\) p < t < p = Np N - p . In the \(L^p\) L p -critical case, the different values of t affect the geometric structure of the functional corresponding to the equation. The purpose of this paper is to establish the existence of radial normalized solution on different t.