包含分数阶p-拉普拉斯和双临界非线性的方程组

IF 2.1 2区 数学 Q1 MATHEMATICS Advanced Nonlinear Studies Pub Date : 2023-01-01 DOI:10.1515/ans-2023-0103
Mousomi Bhakta, Kanishka Perera, Firoj Sk
{"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>&gt;</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>&gt;</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>&gt;</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>&gt;</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>&gt;</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>&gt;</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>&gt;</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>&gt;</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}
引用次数: 0

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。
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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 .
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来源期刊
CiteScore
3.00
自引率
5.60%
发文量
22
审稿时长
12 months
期刊介绍: Advanced Nonlinear Studies is aimed at publishing papers on nonlinear problems, particulalry those involving Differential Equations, Dynamical Systems, and related areas. It will also publish novel and interesting applications of these areas to problems in engineering and the sciences. Papers submitted to this journal must contain original, timely, and significant results. Articles will generally, but not always, be published in the order when the final copies were received.
期刊最新文献
Solutions to the coupled Schrödinger systems with steep potential well and critical exponent Solitons to the Willmore flow Remarks on analytical solutions to compressible Navier–Stokes equations with free boundaries Homogenization of Smoluchowski-type equations with transmission boundary conditions Regularity of center-outward distribution functions in non-convex domains
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