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{"title":"包含分数阶p-拉普拉斯和双临界非线性的方程组","authors":"Mousomi Bhakta, Kanishka Perera, Firoj Sk","doi":"10.1515/ans-2023-0103","DOIUrl":null,"url":null,"abstract":"Abstract This article deals with existence of solutions to the following fractional <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"> <m:mi>p</m:mi> </m:math> p -Laplacian system of equations: <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\" display=\"block\"> <m:mfenced open=\"{\" close=\"\"> <m:mrow> <m:mtable displaystyle=\"true\"> <m:mtr> <m:mtd columnalign=\"left\"> <m:msup> <m:mrow> <m:mrow> <m:mo>(</m:mo> <m:mrow> <m:mo>−</m:mo> <m:msub> <m:mrow> <m:mi mathvariant=\"normal\">Δ</m:mi> </m:mrow> <m:mrow> <m:mi>p</m:mi> </m:mrow> </m:msub> </m:mrow> <m:mo>)</m:mo> </m:mrow> </m:mrow> <m:mrow> <m:mi>s</m:mi> </m:mrow> </m:msup> <m:mi>u</m:mi> <m:mo>=</m:mo> <m:msup> <m:mrow> <m:mo>∣</m:mo> <m:mi>u</m:mi> <m:mo>∣</m:mo> </m:mrow> <m:mrow> <m:msubsup> <m:mrow> <m:mi>p</m:mi> </m:mrow> <m:mrow> <m:mi>s</m:mi> </m:mrow> <m:mrow> <m:mo>*</m:mo> </m:mrow> </m:msubsup> <m:mo>−</m:mo> <m:mn>2</m:mn> </m:mrow> </m:msup> <m:mi>u</m:mi> <m:mo>+</m:mo> <m:mfrac> <m:mrow> <m:mi>γ</m:mi> <m:mi>α</m:mi> </m:mrow> <m:mrow> <m:msubsup> <m:mrow> <m:mi>p</m:mi> </m:mrow> <m:mrow> <m:mi>s</m:mi> </m:mrow> <m:mrow> <m:mo>*</m:mo> </m:mrow> </m:msubsup> </m:mrow> </m:mfrac> <m:msup> <m:mrow> <m:mo>∣</m:mo> <m:mi>u</m:mi> <m:mo>∣</m:mo> </m:mrow> <m:mrow> <m:mi>α</m:mi> <m:mo>−</m:mo> <m:mn>2</m:mn> </m:mrow> </m:msup> <m:mi>u</m:mi> <m:msup> <m:mrow> <m:mo>∣</m:mo> <m:mi>v</m:mi> <m:mo>∣</m:mo> </m:mrow> <m:mrow> <m:mi>β</m:mi> </m:mrow> </m:msup> <m:mspace width=\"0.33em\" /> <m:mspace width=\"0.33em\" /> <m:mstyle> <m:mspace width=\"0.1em\" /> <m:mtext>in</m:mtext> <m:mspace width=\"0.1em\" /> </m:mstyle> <m:mspace width=\"0.33em\" /> <m:mi mathvariant=\"normal\">Ω</m:mi> <m:mo>,</m:mo> <m:mspace width=\"1.0em\" /> </m:mtd> </m:mtr> <m:mtr> <m:mtd columnalign=\"left\"> <m:msup> <m:mrow> <m:mrow> <m:mo>(</m:mo> <m:mrow> <m:mo>−</m:mo> <m:msub> <m:mrow> <m:mi mathvariant=\"normal\">Δ</m:mi> </m:mrow> <m:mrow> <m:mi>p</m:mi> </m:mrow> </m:msub> </m:mrow> <m:mo>)</m:mo> </m:mrow> </m:mrow> <m:mrow> <m:mi>s</m:mi> </m:mrow> </m:msup> <m:mi>v</m:mi> <m:mo>=</m:mo> <m:msup> <m:mrow> <m:mo>∣</m:mo> <m:mi>v</m:mi> <m:mo>∣</m:mo> </m:mrow> <m:mrow> <m:msubsup> <m:mrow> <m:mi>p</m:mi> </m:mrow> <m:mrow> <m:mi>s</m:mi> </m:mrow> <m:mrow> <m:mo>*</m:mo> </m:mrow> </m:msubsup> <m:mo>−</m:mo> <m:mn>2</m:mn> </m:mrow> </m:msup> <m:mi>v</m:mi> <m:mo>+</m:mo> <m:mfrac> <m:mrow> <m:mi>γ</m:mi> <m:mi>β</m:mi> </m:mrow> <m:mrow> <m:msubsup> <m:mrow> <m:mi>p</m:mi> </m:mrow> <m:mrow> <m:mi>s</m:mi> </m:mrow> <m:mrow> <m:mo>*</m:mo> </m:mrow> </m:msubsup> </m:mrow> </m:mfrac> <m:msup> <m:mrow> <m:mo>∣</m:mo> <m:mi>v</m:mi> <m:mo>∣</m:mo> </m:mrow> <m:mrow> <m:mi>β</m:mi> <m:mo>−</m:mo> <m:mn>2</m:mn> </m:mrow> </m:msup> <m:mi>v</m:mi> <m:msup> <m:mrow> <m:mo>∣</m:mo> <m:mi>u</m:mi> <m:mo>∣</m:mo> </m:mrow> <m:mrow> <m:mi>α</m:mi> </m:mrow> </m:msup> <m:mspace width=\"0.33em\" /> <m:mspace width=\"0.33em\" /> <m:mstyle> <m:mspace width=\"0.1em\" /> <m:mtext>in</m:mtext> <m:mspace width=\"0.1em\" /> </m:mstyle> <m:mspace width=\"0.33em\" /> <m:mi mathvariant=\"normal\">Ω</m:mi> <m:mo>,</m:mo> <m:mspace width=\"1.0em\" /> </m:mtd> </m:mtr> </m:mtable> </m:mrow> </m:mfenced> </m:math> \\left\\{\\begin{array}{l}{\\left(-{\\Delta }_{p})}^{s}u={| u| }^{{p}_{s}^{* }-2}u+\\frac{\\gamma \\alpha }{{p}_{s}^{* }}{| u| }^{\\alpha -2}u{| v| }^{\\beta }\\hspace{0.33em}\\hspace{0.33em}\\hspace{0.1em}\\text{in}\\hspace{0.1em}\\hspace{0.33em}\\Omega ,\\hspace{1.0em}\\\\ {\\left(-{\\Delta }_{p})}^{s}v={| v| }^{{p}_{s}^{* }-2}v+\\frac{\\gamma \\beta }{{p}_{s}^{* }}{| v| }^{\\beta -2}v{| u| }^{\\alpha }\\hspace{0.33em}\\hspace{0.33em}\\hspace{0.1em}\\text{in}\\hspace{0.1em}\\hspace{0.33em}\\Omega ,\\hspace{1.0em}\\end{array}\\right. where <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"> <m:mi>s</m:mi> <m:mo>∈</m:mo> <m:mrow> <m:mo>(</m:mo> <m:mrow> <m:mn>0</m:mn> <m:mo>,</m:mo> <m:mn>1</m:mn> </m:mrow> <m:mo>)</m:mo> </m:mrow> </m:math> s\\in \\left(0,1) , <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"> <m:mi>p</m:mi> <m:mo>∈</m:mo> <m:mrow> <m:mo>(</m:mo> <m:mrow> <m:mn>1</m:mn> <m:mo>,</m:mo> <m:mi>∞</m:mi> </m:mrow> <m:mo>)</m:mo> </m:mrow> </m:math> p\\in \\left(1,\\infty ) with <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"> <m:mi>N</m:mi> <m:mo>></m:mo> <m:mi>s</m:mi> <m:mi>p</m:mi> </m:math> N\\gt sp , <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"> <m:mi>α</m:mi> <m:mo>,</m:mo> <m:mi>β</m:mi> <m:mo>></m:mo> <m:mn>1</m:mn> </m:math> \\alpha ,\\beta \\gt 1 such that <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"> <m:mi>α</m:mi> <m:mo>+</m:mo> <m:mi>β</m:mi> <m:mo>=</m:mo> <m:msubsup> <m:mrow> <m:mi>p</m:mi> </m:mrow> <m:mrow> <m:mi>s</m:mi> </m:mrow> <m:mrow> <m:mo>*</m:mo> </m:mrow> </m:msubsup> <m:mo>≔</m:mo> <m:mfrac> <m:mrow> <m:mi>N</m:mi> <m:mi>p</m:mi> </m:mrow> <m:mrow> <m:mi>N</m:mi> <m:mo>−</m:mo> <m:mi>s</m:mi> <m:mi>p</m:mi> </m:mrow> </m:mfrac> </m:math> \\alpha +\\beta ={p}_{s}^{* }:= \\frac{Np}{N-sp} and <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"> <m:mi mathvariant=\"normal\">Ω</m:mi> <m:mo>=</m:mo> <m:msup> <m:mrow> <m:mi mathvariant=\"double-struck\">R</m:mi> </m:mrow> <m:mrow> <m:mi>N</m:mi> </m:mrow> </m:msup> </m:math> \\Omega ={{\\mathbb{R}}}^{N} or smooth bounded domains in <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"> <m:msup> <m:mrow> <m:mi mathvariant=\"double-struck\">R</m:mi> </m:mrow> <m:mrow> <m:mi>N</m:mi> </m:mrow> </m:msup> </m:math> {{\\mathbb{R}}}^{N} . When <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"> <m:mi mathvariant=\"normal\">Ω</m:mi> <m:mo>=</m:mo> <m:msup> <m:mrow> <m:mi mathvariant=\"double-struck\">R</m:mi> </m:mrow> <m:mrow> <m:mi>N</m:mi> </m:mrow> </m:msup> </m:math> \\Omega ={{\\mathbb{R}}}^{N} and <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"> <m:mi>γ</m:mi> <m:mo>=</m:mo> <m:mn>1</m:mn> </m:math> \\gamma =1 , we show that any ground state solution of the aforementioned system has the form <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"> <m:mrow> <m:mo>(</m:mo> <m:mrow> <m:mi>λ</m:mi> <m:mi>U</m:mi> <m:mo>,</m:mo> <m:mi>τ</m:mi> <m:mi>λ</m:mi> <m:mi>V</m:mi> </m:mrow> <m:mo>)</m:mo> </m:mrow> </m:math> \\left(\\lambda U,\\tau \\lambda V) for certain <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"> <m:mi>τ</m:mi> <m:mo>></m:mo> <m:mn>0</m:mn> </m:math> \\tau \\gt 0 and <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"> <m:mi>U</m:mi> </m:math> U and <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"> <m:mi>V</m:mi> </m:math> V are two positive ground state solutions of <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"> <m:msup> <m:mrow> <m:mrow> <m:mo>(</m:mo> <m:mrow> <m:mo>−</m:mo> <m:msub> <m:mrow> <m:mi mathvariant=\"normal\">Δ</m:mi> </m:mrow> <m:mrow> <m:mi>p</m:mi> </m:mrow> </m:msub> </m:mrow> <m:mo>)</m:mo> </m:mrow> </m:mrow> <m:mrow> <m:mi>s</m:mi> </m:mrow> </m:msup> <m:mi>u</m:mi> <m:mo>=</m:mo> <m:msup> <m:mrow> <m:mo>∣</m:mo> <m:mi>u</m:mi> <m:mo>∣</m:mo> </m:mrow> <m:mrow> <m:msubsup> <m:mrow> <m:mi>p</m:mi> </m:mrow> <m:mrow> <m:mi>s</m:mi> </m:mrow> <m:mrow> <m:mo>*</m:mo> </m:mrow> </m:msubsup> <m:mo>−</m:mo> <m:mn>2</m:mn> </m:mrow> </m:msup> <m:mi>u</m:mi> </m:math> {\\left(-{\\Delta }_{p})}^{s}u={| u| }^{{p}_{s}^{* }-2}u in <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"> <m:msup> <m:mrow> <m:mi mathvariant=\"double-struck\">R</m:mi> </m:mrow> <m:mrow> <m:mi>N</m:mi> </m:mrow> </m:msup> </m:math> {{\\mathbb{R}}}^{N} . For all <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"> <m:mi>γ</m:mi> <m:mo>></m:mo> <m:mn>0</m:mn> </m:math> \\gamma \\gt 0 , we establish existence of a positive radial solution to the aforementioned system in balls. When <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"> <m:mi mathvariant=\"normal\">Ω</m:mi> <m:mo>=</m:mo> <m:msup> <m:mrow> <m:mi mathvariant=\"double-struck\">R</m:mi> </m:mrow> <m:mrow> <m:mi>N</m:mi> </m:mrow> </m:msup> </m:math> \\Omega ={{\\mathbb{R}}}^{N} , we also establish existence of positive radial solutions to the aforementioned system in various ranges of <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\"> <m:mi>γ</m:mi> </m:math> \\gamma .","PeriodicalId":7191,"journal":{"name":"Advanced Nonlinear Studies","volume":"39 1","pages":"0"},"PeriodicalIF":2.1000,"publicationDate":"2023-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"A system of equations involving the fractional <i>p</i>-Laplacian and doubly critical nonlinearities\",\"authors\":\"Mousomi Bhakta, Kanishka Perera, Firoj Sk\",\"doi\":\"10.1515/ans-2023-0103\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Abstract This article deals with existence of solutions to the following fractional <m:math xmlns:m=\\\"http://www.w3.org/1998/Math/MathML\\\"> <m:mi>p</m:mi> </m:math> p -Laplacian system of equations: <m:math xmlns:m=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"block\\\"> <m:mfenced open=\\\"{\\\" close=\\\"\\\"> <m:mrow> <m:mtable displaystyle=\\\"true\\\"> <m:mtr> <m:mtd columnalign=\\\"left\\\"> <m:msup> <m:mrow> <m:mrow> <m:mo>(</m:mo> <m:mrow> <m:mo>−</m:mo> <m:msub> <m:mrow> <m:mi mathvariant=\\\"normal\\\">Δ</m:mi> </m:mrow> <m:mrow> <m:mi>p</m:mi> </m:mrow> </m:msub> </m:mrow> <m:mo>)</m:mo> </m:mrow> </m:mrow> <m:mrow> <m:mi>s</m:mi> </m:mrow> </m:msup> <m:mi>u</m:mi> <m:mo>=</m:mo> <m:msup> <m:mrow> <m:mo>∣</m:mo> <m:mi>u</m:mi> <m:mo>∣</m:mo> </m:mrow> <m:mrow> <m:msubsup> <m:mrow> <m:mi>p</m:mi> </m:mrow> <m:mrow> <m:mi>s</m:mi> </m:mrow> <m:mrow> <m:mo>*</m:mo> </m:mrow> </m:msubsup> <m:mo>−</m:mo> <m:mn>2</m:mn> </m:mrow> </m:msup> <m:mi>u</m:mi> <m:mo>+</m:mo> <m:mfrac> <m:mrow> <m:mi>γ</m:mi> <m:mi>α</m:mi> </m:mrow> <m:mrow> <m:msubsup> <m:mrow> <m:mi>p</m:mi> </m:mrow> <m:mrow> <m:mi>s</m:mi> </m:mrow> <m:mrow> <m:mo>*</m:mo> </m:mrow> </m:msubsup> </m:mrow> </m:mfrac> <m:msup> <m:mrow> <m:mo>∣</m:mo> <m:mi>u</m:mi> <m:mo>∣</m:mo> </m:mrow> <m:mrow> <m:mi>α</m:mi> <m:mo>−</m:mo> <m:mn>2</m:mn> </m:mrow> </m:msup> <m:mi>u</m:mi> <m:msup> <m:mrow> <m:mo>∣</m:mo> <m:mi>v</m:mi> <m:mo>∣</m:mo> </m:mrow> <m:mrow> <m:mi>β</m:mi> </m:mrow> </m:msup> <m:mspace width=\\\"0.33em\\\" /> <m:mspace width=\\\"0.33em\\\" /> <m:mstyle> <m:mspace width=\\\"0.1em\\\" /> <m:mtext>in</m:mtext> <m:mspace width=\\\"0.1em\\\" /> </m:mstyle> <m:mspace width=\\\"0.33em\\\" /> <m:mi mathvariant=\\\"normal\\\">Ω</m:mi> <m:mo>,</m:mo> <m:mspace width=\\\"1.0em\\\" /> </m:mtd> </m:mtr> <m:mtr> <m:mtd columnalign=\\\"left\\\"> <m:msup> <m:mrow> <m:mrow> <m:mo>(</m:mo> <m:mrow> <m:mo>−</m:mo> <m:msub> <m:mrow> <m:mi mathvariant=\\\"normal\\\">Δ</m:mi> </m:mrow> <m:mrow> <m:mi>p</m:mi> </m:mrow> </m:msub> </m:mrow> <m:mo>)</m:mo> </m:mrow> </m:mrow> <m:mrow> <m:mi>s</m:mi> </m:mrow> </m:msup> <m:mi>v</m:mi> <m:mo>=</m:mo> <m:msup> <m:mrow> <m:mo>∣</m:mo> <m:mi>v</m:mi> <m:mo>∣</m:mo> </m:mrow> <m:mrow> <m:msubsup> <m:mrow> <m:mi>p</m:mi> </m:mrow> <m:mrow> <m:mi>s</m:mi> </m:mrow> <m:mrow> <m:mo>*</m:mo> </m:mrow> </m:msubsup> <m:mo>−</m:mo> <m:mn>2</m:mn> </m:mrow> </m:msup> <m:mi>v</m:mi> <m:mo>+</m:mo> <m:mfrac> <m:mrow> <m:mi>γ</m:mi> <m:mi>β</m:mi> </m:mrow> <m:mrow> <m:msubsup> <m:mrow> <m:mi>p</m:mi> </m:mrow> <m:mrow> <m:mi>s</m:mi> </m:mrow> <m:mrow> <m:mo>*</m:mo> </m:mrow> </m:msubsup> </m:mrow> </m:mfrac> <m:msup> <m:mrow> <m:mo>∣</m:mo> <m:mi>v</m:mi> <m:mo>∣</m:mo> </m:mrow> <m:mrow> <m:mi>β</m:mi> <m:mo>−</m:mo> <m:mn>2</m:mn> </m:mrow> </m:msup> <m:mi>v</m:mi> <m:msup> <m:mrow> <m:mo>∣</m:mo> <m:mi>u</m:mi> <m:mo>∣</m:mo> </m:mrow> <m:mrow> <m:mi>α</m:mi> </m:mrow> </m:msup> <m:mspace width=\\\"0.33em\\\" /> <m:mspace width=\\\"0.33em\\\" /> <m:mstyle> <m:mspace width=\\\"0.1em\\\" /> <m:mtext>in</m:mtext> <m:mspace width=\\\"0.1em\\\" /> </m:mstyle> <m:mspace width=\\\"0.33em\\\" /> <m:mi mathvariant=\\\"normal\\\">Ω</m:mi> <m:mo>,</m:mo> <m:mspace width=\\\"1.0em\\\" /> </m:mtd> </m:mtr> </m:mtable> </m:mrow> </m:mfenced> </m:math> \\\\left\\\\{\\\\begin{array}{l}{\\\\left(-{\\\\Delta }_{p})}^{s}u={| u| }^{{p}_{s}^{* }-2}u+\\\\frac{\\\\gamma \\\\alpha }{{p}_{s}^{* }}{| u| }^{\\\\alpha -2}u{| v| }^{\\\\beta }\\\\hspace{0.33em}\\\\hspace{0.33em}\\\\hspace{0.1em}\\\\text{in}\\\\hspace{0.1em}\\\\hspace{0.33em}\\\\Omega ,\\\\hspace{1.0em}\\\\\\\\ {\\\\left(-{\\\\Delta }_{p})}^{s}v={| v| }^{{p}_{s}^{* }-2}v+\\\\frac{\\\\gamma \\\\beta }{{p}_{s}^{* }}{| v| }^{\\\\beta -2}v{| u| }^{\\\\alpha }\\\\hspace{0.33em}\\\\hspace{0.33em}\\\\hspace{0.1em}\\\\text{in}\\\\hspace{0.1em}\\\\hspace{0.33em}\\\\Omega ,\\\\hspace{1.0em}\\\\end{array}\\\\right. where <m:math xmlns:m=\\\"http://www.w3.org/1998/Math/MathML\\\"> <m:mi>s</m:mi> <m:mo>∈</m:mo> <m:mrow> <m:mo>(</m:mo> <m:mrow> <m:mn>0</m:mn> <m:mo>,</m:mo> <m:mn>1</m:mn> </m:mrow> <m:mo>)</m:mo> </m:mrow> </m:math> s\\\\in \\\\left(0,1) , <m:math xmlns:m=\\\"http://www.w3.org/1998/Math/MathML\\\"> <m:mi>p</m:mi> <m:mo>∈</m:mo> <m:mrow> <m:mo>(</m:mo> <m:mrow> <m:mn>1</m:mn> <m:mo>,</m:mo> <m:mi>∞</m:mi> </m:mrow> <m:mo>)</m:mo> </m:mrow> </m:math> p\\\\in \\\\left(1,\\\\infty ) with <m:math xmlns:m=\\\"http://www.w3.org/1998/Math/MathML\\\"> <m:mi>N</m:mi> <m:mo>></m:mo> <m:mi>s</m:mi> <m:mi>p</m:mi> </m:math> N\\\\gt sp , <m:math xmlns:m=\\\"http://www.w3.org/1998/Math/MathML\\\"> <m:mi>α</m:mi> <m:mo>,</m:mo> <m:mi>β</m:mi> <m:mo>></m:mo> <m:mn>1</m:mn> </m:math> \\\\alpha ,\\\\beta \\\\gt 1 such that <m:math xmlns:m=\\\"http://www.w3.org/1998/Math/MathML\\\"> <m:mi>α</m:mi> <m:mo>+</m:mo> <m:mi>β</m:mi> <m:mo>=</m:mo> <m:msubsup> <m:mrow> <m:mi>p</m:mi> </m:mrow> <m:mrow> <m:mi>s</m:mi> </m:mrow> <m:mrow> <m:mo>*</m:mo> </m:mrow> </m:msubsup> <m:mo>≔</m:mo> <m:mfrac> <m:mrow> <m:mi>N</m:mi> <m:mi>p</m:mi> </m:mrow> <m:mrow> <m:mi>N</m:mi> <m:mo>−</m:mo> <m:mi>s</m:mi> <m:mi>p</m:mi> </m:mrow> </m:mfrac> </m:math> \\\\alpha +\\\\beta ={p}_{s}^{* }:= \\\\frac{Np}{N-sp} and <m:math xmlns:m=\\\"http://www.w3.org/1998/Math/MathML\\\"> <m:mi mathvariant=\\\"normal\\\">Ω</m:mi> <m:mo>=</m:mo> <m:msup> <m:mrow> <m:mi mathvariant=\\\"double-struck\\\">R</m:mi> </m:mrow> <m:mrow> <m:mi>N</m:mi> </m:mrow> </m:msup> </m:math> \\\\Omega ={{\\\\mathbb{R}}}^{N} or smooth bounded domains in <m:math xmlns:m=\\\"http://www.w3.org/1998/Math/MathML\\\"> <m:msup> <m:mrow> <m:mi mathvariant=\\\"double-struck\\\">R</m:mi> </m:mrow> <m:mrow> <m:mi>N</m:mi> </m:mrow> </m:msup> </m:math> {{\\\\mathbb{R}}}^{N} . When <m:math xmlns:m=\\\"http://www.w3.org/1998/Math/MathML\\\"> <m:mi mathvariant=\\\"normal\\\">Ω</m:mi> <m:mo>=</m:mo> <m:msup> <m:mrow> <m:mi mathvariant=\\\"double-struck\\\">R</m:mi> </m:mrow> <m:mrow> <m:mi>N</m:mi> </m:mrow> </m:msup> </m:math> \\\\Omega ={{\\\\mathbb{R}}}^{N} and <m:math xmlns:m=\\\"http://www.w3.org/1998/Math/MathML\\\"> <m:mi>γ</m:mi> <m:mo>=</m:mo> <m:mn>1</m:mn> </m:math> \\\\gamma =1 , we show that any ground state solution of the aforementioned system has the form <m:math xmlns:m=\\\"http://www.w3.org/1998/Math/MathML\\\"> <m:mrow> <m:mo>(</m:mo> <m:mrow> <m:mi>λ</m:mi> <m:mi>U</m:mi> <m:mo>,</m:mo> <m:mi>τ</m:mi> <m:mi>λ</m:mi> <m:mi>V</m:mi> </m:mrow> <m:mo>)</m:mo> </m:mrow> </m:math> \\\\left(\\\\lambda U,\\\\tau \\\\lambda V) for certain <m:math xmlns:m=\\\"http://www.w3.org/1998/Math/MathML\\\"> <m:mi>τ</m:mi> <m:mo>></m:mo> <m:mn>0</m:mn> </m:math> \\\\tau \\\\gt 0 and <m:math xmlns:m=\\\"http://www.w3.org/1998/Math/MathML\\\"> <m:mi>U</m:mi> </m:math> U and <m:math xmlns:m=\\\"http://www.w3.org/1998/Math/MathML\\\"> <m:mi>V</m:mi> </m:math> V are two positive ground state solutions of <m:math xmlns:m=\\\"http://www.w3.org/1998/Math/MathML\\\"> <m:msup> <m:mrow> <m:mrow> <m:mo>(</m:mo> <m:mrow> <m:mo>−</m:mo> <m:msub> <m:mrow> <m:mi mathvariant=\\\"normal\\\">Δ</m:mi> </m:mrow> <m:mrow> <m:mi>p</m:mi> </m:mrow> </m:msub> </m:mrow> <m:mo>)</m:mo> </m:mrow> </m:mrow> <m:mrow> <m:mi>s</m:mi> </m:mrow> </m:msup> <m:mi>u</m:mi> <m:mo>=</m:mo> <m:msup> <m:mrow> <m:mo>∣</m:mo> <m:mi>u</m:mi> <m:mo>∣</m:mo> </m:mrow> <m:mrow> <m:msubsup> <m:mrow> <m:mi>p</m:mi> </m:mrow> <m:mrow> <m:mi>s</m:mi> </m:mrow> <m:mrow> <m:mo>*</m:mo> </m:mrow> </m:msubsup> <m:mo>−</m:mo> <m:mn>2</m:mn> </m:mrow> </m:msup> <m:mi>u</m:mi> </m:math> {\\\\left(-{\\\\Delta }_{p})}^{s}u={| u| }^{{p}_{s}^{* }-2}u in <m:math xmlns:m=\\\"http://www.w3.org/1998/Math/MathML\\\"> <m:msup> <m:mrow> <m:mi mathvariant=\\\"double-struck\\\">R</m:mi> </m:mrow> <m:mrow> <m:mi>N</m:mi> </m:mrow> </m:msup> </m:math> {{\\\\mathbb{R}}}^{N} . For all <m:math xmlns:m=\\\"http://www.w3.org/1998/Math/MathML\\\"> <m:mi>γ</m:mi> <m:mo>></m:mo> <m:mn>0</m:mn> </m:math> \\\\gamma \\\\gt 0 , we establish existence of a positive radial solution to the aforementioned system in balls. When <m:math xmlns:m=\\\"http://www.w3.org/1998/Math/MathML\\\"> <m:mi mathvariant=\\\"normal\\\">Ω</m:mi> <m:mo>=</m:mo> <m:msup> <m:mrow> <m:mi mathvariant=\\\"double-struck\\\">R</m:mi> </m:mrow> <m:mrow> <m:mi>N</m:mi> </m:mrow> </m:msup> </m:math> \\\\Omega ={{\\\\mathbb{R}}}^{N} , we also establish existence of positive radial solutions to the aforementioned system in various ranges of <m:math xmlns:m=\\\"http://www.w3.org/1998/Math/MathML\\\"> <m:mi>γ</m:mi> </m:math> \\\\gamma .\",\"PeriodicalId\":7191,\"journal\":{\"name\":\"Advanced Nonlinear Studies\",\"volume\":\"39 1\",\"pages\":\"0\"},\"PeriodicalIF\":2.1000,\"publicationDate\":\"2023-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Advanced Nonlinear Studies\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1515/ans-2023-0103\",\"RegionNum\":2,\"RegionCategory\":\"数学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"MATHEMATICS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Advanced Nonlinear Studies","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1515/ans-2023-0103","RegionNum":2,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"MATHEMATICS","Score":null,"Total":0}
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摘要
摘要 本文论述下列分数 p p -拉普拉斯方程组的解的存在性: ( - Δ p ) s u = ∣ u ∣ p s * - 2 u + γ α p s * ∣ u ∣ α - 2 u ∣ v ∣ β in Ω 、 ( - Δ p ) s v = ∣ v ∣ p s * - 2 v + γ β p s * ∣ v ∣ β - 2 v ∣ u ∣ α in Ω 、 \left(-{Delta }_{p})}^{s}u={| u| }^{p}_{s}^{* }-2}u+frac{gamma \alpha }{p}_{s}^{* }}{ u| }^{\alpha -2}u{| v| }^{beta }\hspace{0.33em}\hspace{0.33em}\hspace{0.1em}\text{in}\hspace{0.1em}\hspace{0.33em}\Omega ,\hspace{1.0em}\ {left(-{\Delta }_{p})}^{s}v={| v| }^{p}_{s}^{* }-2}v+\frac{gamma \beta }{{p}_{s}^{* }}{| v| }^{\beta -2}v{| u| }^{alpha }\hspace{0.33em}\hspace{0.33em}\hspace{0.1em}\text{in}\hspace{0.1em}\hspace{0.33em}\Omega ,\hspace{1.0em}\end{array}\right.其中 s∈ ( 0 , 1 ) s\in \left(0,1) , p∈ ( 1 , ∞ ) p\in \left(1,\infty ) with N > s p N\gt sp , α , β >;1 \alpha ,\beta 1 such that α + β = p s * ≔ N p N - s p \alpha +\beta ={p}_{s}^{* }:= \frac{Np}{N-sp} 和 Ω = R N \Omega ={{mathbb{R}}}^{N} 或 R N 中的光滑有界域 {{mathbb{R}}}^{N} 。当 Ω = R N \Omega ={{\mathbb{R}}}^{N} 且 γ = 1 \gamma =1 时,我们证明在一定的 τ > 条件下,上述系统的任何基态解都具有 ( λ U , τ λ V ) \left(\lambda U,\tau \lambda V) 的形式;0 \tau \gt 0 且 U U 和 V V 是 ( - Δ p ) s u = ∣ u ∣ p s * - 2 u {\left(-{Delta }_{p})}^{s}u={| u| }^{p}_{s}^{* }-2}u in R N {{\mathbb{R}}}^{N} 的两个正基态解。对于所有 γ > 0 \gamma \gt 0,我们确定了上述系统在球中的正径向解的存在性。当 Ω = R N \Omega ={\mathbb{R}}}^{N} 时,我们也建立了上述系统在不同 γ \gamma 范围内的正径向解的存在性。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
A system of equations involving the fractional p -Laplacian and doubly critical nonlinearities
Abstract This article deals with existence of solutions to the following fractional p p -Laplacian system of equations: ( − Δ p ) s u = ∣ u ∣ p s * − 2 u + γ α p s * ∣ u ∣ α − 2 u ∣ v ∣ β in Ω , ( − Δ p ) s v = ∣ v ∣ p s * − 2 v + γ β p s * ∣ v ∣ β − 2 v ∣ u ∣ α in Ω , \left\{\begin{array}{l}{\left(-{\Delta }_{p})}^{s}u={| u| }^{{p}_{s}^{* }-2}u+\frac{\gamma \alpha }{{p}_{s}^{* }}{| u| }^{\alpha -2}u{| v| }^{\beta }\hspace{0.33em}\hspace{0.33em}\hspace{0.1em}\text{in}\hspace{0.1em}\hspace{0.33em}\Omega ,\hspace{1.0em}\\ {\left(-{\Delta }_{p})}^{s}v={| v| }^{{p}_{s}^{* }-2}v+\frac{\gamma \beta }{{p}_{s}^{* }}{| v| }^{\beta -2}v{| u| }^{\alpha }\hspace{0.33em}\hspace{0.33em}\hspace{0.1em}\text{in}\hspace{0.1em}\hspace{0.33em}\Omega ,\hspace{1.0em}\end{array}\right. where s ∈ ( 0 , 1 ) s\in \left(0,1) , p ∈ ( 1 , ∞ ) p\in \left(1,\infty ) with N > s p N\gt sp , α , β > 1 \alpha ,\beta \gt 1 such that α + β = p s * ≔ N p N − s p \alpha +\beta ={p}_{s}^{* }:= \frac{Np}{N-sp} and Ω = R N \Omega ={{\mathbb{R}}}^{N} or smooth bounded domains in R N {{\mathbb{R}}}^{N} . When Ω = R N \Omega ={{\mathbb{R}}}^{N} and γ = 1 \gamma =1 , we show that any ground state solution of the aforementioned system has the form ( λ U , τ λ V ) \left(\lambda U,\tau \lambda V) for certain τ > 0 \tau \gt 0 and U U and V V are two positive ground state solutions of ( − Δ p ) s u = ∣ u ∣ p s * − 2 u {\left(-{\Delta }_{p})}^{s}u={| u| }^{{p}_{s}^{* }-2}u in R N {{\mathbb{R}}}^{N} . For all γ > 0 \gamma \gt 0 , we establish existence of a positive radial solution to the aforementioned system in balls. When Ω = R N \Omega ={{\mathbb{R}}}^{N} , we also establish existence of positive radial solutions to the aforementioned system in various ranges of γ \gamma .