Concentration phenomena of normalized solutions for a fractional p-Laplacian Schrödinger–Choquard system in RN

IF 3.8 2区 数学 Q1 MATHEMATICS, APPLIED Communications in Nonlinear Science and Numerical Simulation Pub Date : 2025-02-11 DOI:10.1016/j.cnsns.2025.108665
Yuxuan Tong , Thin Van Nguyen , Sihua Liang
{"title":"Concentration phenomena of normalized solutions for a fractional p-Laplacian Schrödinger–Choquard system in RN","authors":"Yuxuan Tong ,&nbsp;Thin Van Nguyen ,&nbsp;Sihua Liang","doi":"10.1016/j.cnsns.2025.108665","DOIUrl":null,"url":null,"abstract":"<div><div>In this paper, we consider the following Schrödinger–Choquard system in <span><math><mi>R</mi></math></span><sup><em>N</em></sup> <span><span><span><math><mfenced><mrow><mtable><mtr><mtd><msubsup><mrow><mrow><mo>(</mo><mo>−</mo><mi>Δ</mi><mo>)</mo></mrow></mrow><mrow><mi>p</mi></mrow><mrow><mi>s</mi></mrow></msubsup><msub><mrow><mi>u</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>+</mo><mrow><mo>(</mo><msub><mrow><mi>V</mi></mrow><mrow><mn>1</mn></mrow></msub><mrow><mo>(</mo><mi>ɛ</mi><mi>x</mi><mo>)</mo></mrow><mo>−</mo><msub><mrow><mi>λ</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>)</mo></mrow><msup><mrow><mrow><mo>|</mo><msub><mrow><mi>u</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>|</mo></mrow></mrow><mrow><mi>p</mi><mo>−</mo><mn>2</mn></mrow></msup><msub><mrow><mi>u</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>=</mo><msub><mrow><mi>μ</mi></mrow><mrow><mn>1</mn></mrow></msub><mrow><mo>[</mo><mfrac><mrow><mn>1</mn></mrow><mrow><msup><mrow><mrow><mo>|</mo><mi>x</mi><mo>|</mo></mrow></mrow><mrow><mi>N</mi><mo>−</mo><mi>α</mi></mrow></msup></mrow></mfrac><mo>∗</mo><msub><mrow><mi>F</mi></mrow><mrow><mn>1</mn></mrow></msub><mrow><mo>(</mo><msub><mrow><mi>u</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>)</mo></mrow><mo>]</mo></mrow><msub><mrow><mi>f</mi></mrow><mrow><mn>1</mn></mrow></msub><mrow><mo>(</mo><msub><mrow><mi>u</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>)</mo></mrow><mo>+</mo><mi>β</mi><msub><mrow><mi>r</mi></mrow><mrow><mn>1</mn></mrow></msub><msup><mrow><mrow><mo>|</mo><msub><mrow><mi>u</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>|</mo></mrow></mrow><mrow><msub><mrow><mi>r</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>−</mo><mn>2</mn></mrow></msup><msub><mrow><mi>u</mi></mrow><mrow><mn>1</mn></mrow></msub><msup><mrow><mrow><mo>|</mo><msub><mrow><mi>u</mi></mrow><mrow><mn>2</mn></mrow></msub><mo>|</mo></mrow></mrow><mrow><msub><mrow><mi>r</mi></mrow><mrow><mn>2</mn></mrow></msub></mrow></msup><mspace></mspace><mtext>in</mtext><mspace></mspace><msup><mrow><mi>R</mi></mrow><mrow><mi>N</mi></mrow></msup><mo>,</mo></mtd></mtr><mtr><mtd><msubsup><mrow><mrow><mo>(</mo><mo>−</mo><mi>Δ</mi><mo>)</mo></mrow></mrow><mrow><mi>p</mi></mrow><mrow><mi>s</mi></mrow></msubsup><msub><mrow><mi>u</mi></mrow><mrow><mn>2</mn></mrow></msub><mo>+</mo><mrow><mo>(</mo><msub><mrow><mi>V</mi></mrow><mrow><mn>2</mn></mrow></msub><mrow><mo>(</mo><mi>ɛ</mi><mi>x</mi><mo>)</mo></mrow><mo>−</mo><msub><mrow><mi>λ</mi></mrow><mrow><mn>2</mn></mrow></msub><mo>)</mo></mrow><msup><mrow><mrow><mo>|</mo><msub><mrow><mi>u</mi></mrow><mrow><mn>2</mn></mrow></msub><mo>|</mo></mrow></mrow><mrow><mi>p</mi><mo>−</mo><mn>2</mn></mrow></msup><msub><mrow><mi>u</mi></mrow><mrow><mn>2</mn></mrow></msub><mo>=</mo><msub><mrow><mi>μ</mi></mrow><mrow><mn>2</mn></mrow></msub><mrow><mo>[</mo><mfrac><mrow><mn>1</mn></mrow><mrow><msup><mrow><mrow><mo>|</mo><mi>x</mi><mo>|</mo></mrow></mrow><mrow><mi>N</mi><mo>−</mo><mi>α</mi></mrow></msup></mrow></mfrac><mo>∗</mo><msub><mrow><mi>F</mi></mrow><mrow><mn>2</mn></mrow></msub><mrow><mo>(</mo><msub><mrow><mi>u</mi></mrow><mrow><mn>2</mn></mrow></msub><mo>)</mo></mrow><mo>]</mo></mrow><msub><mrow><mi>f</mi></mrow><mrow><mn>2</mn></mrow></msub><mrow><mo>(</mo><msub><mrow><mi>u</mi></mrow><mrow><mn>2</mn></mrow></msub><mo>)</mo></mrow><mo>+</mo><mi>β</mi><msub><mrow><mi>r</mi></mrow><mrow><mn>2</mn></mrow></msub><msup><mrow><mrow><mo>|</mo><msub><mrow><mi>u</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>|</mo></mrow></mrow><mrow><msub><mrow><mi>r</mi></mrow><mrow><mn>1</mn></mrow></msub></mrow></msup><msup><mrow><mrow><mo>|</mo><msub><mrow><mi>u</mi></mrow><mrow><mn>2</mn></mrow></msub><mo>|</mo></mrow></mrow><mrow><msub><mrow><mi>r</mi></mrow><mrow><mn>2</mn></mrow></msub><mo>−</mo><mn>2</mn></mrow></msup><msub><mrow><mi>u</mi></mrow><mrow><mn>2</mn></mrow></msub><mspace></mspace><mtext>in</mtext><mspace></mspace><msup><mrow><mi>R</mi></mrow><mrow><mi>N</mi></mrow></msup><mo>,</mo></mtd></mtr><mtr><mtd><msub><mrow><mo>∫</mo></mrow><mrow><msup><mrow><mi>R</mi></mrow><mrow><mi>N</mi></mrow></msup></mrow></msub><msup><mrow><mrow><mo>|</mo><msub><mrow><mi>u</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>|</mo></mrow></mrow><mrow><mi>p</mi></mrow></msup><mi>d</mi><mi>x</mi><mo>=</mo><msubsup><mrow><mi>a</mi></mrow><mrow><mn>1</mn></mrow><mrow><mi>p</mi></mrow></msubsup><mo>,</mo><mspace></mspace><msub><mrow><mo>∫</mo></mrow><mrow><msup><mrow><mi>R</mi></mrow><mrow><mi>N</mi></mrow></msup></mrow></msub><msup><mrow><mrow><mo>|</mo><msub><mrow><mi>u</mi></mrow><mrow><mn>2</mn></mrow></msub><mo>|</mo></mrow></mrow><mrow><mi>p</mi></mrow></msup><mi>d</mi><mi>x</mi><mo>=</mo><msubsup><mrow><mi>a</mi></mrow><mrow><mn>2</mn></mrow><mrow><mi>p</mi></mrow></msubsup><mo>,</mo></mtd></mtr></mtable></mrow></mfenced></math></span></span></span>where <span><math><msubsup><mrow><mrow><mo>(</mo><mo>−</mo><mi>Δ</mi><mo>)</mo></mrow></mrow><mrow><mi>p</mi></mrow><mrow><mi>s</mi></mrow></msubsup></math></span> is the fractional <span><math><mi>p</mi></math></span>-Laplacian operator, <span><math><mrow><mi>α</mi><mo>∈</mo><mrow><mo>(</mo><mn>0</mn><mo>,</mo><mi>N</mi><mo>)</mo></mrow></mrow></math></span>, <span><math><mrow><mi>s</mi><mo>∈</mo><mrow><mo>(</mo><mn>0</mn><mo>,</mo><mn>1</mn><mo>)</mo></mrow></mrow></math></span>, <span><math><mrow><msub><mrow><mi>r</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>,</mo><msub><mrow><mi>r</mi></mrow><mrow><mn>2</mn></mrow></msub><mo>&gt;</mo><mn>1</mn></mrow></math></span>, <span><math><mrow><msub><mrow><mi>r</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>+</mo><msub><mrow><mi>r</mi></mrow><mrow><mn>2</mn></mrow></msub><mo>∈</mo><mrow><mo>(</mo><mi>p</mi><mo>,</mo><mi>p</mi><mo>+</mo><mfrac><mrow><msup><mrow><mi>p</mi></mrow><mrow><mn>2</mn></mrow></msup><mi>s</mi></mrow><mrow><mi>N</mi></mrow></mfrac><mo>)</mo></mrow></mrow></math></span>, <span><math><mrow><mi>ɛ</mi><mo>&gt;</mo><mn>0</mn></mrow></math></span> is a parameter, <span><math><mrow><msub><mrow><mi>μ</mi></mrow><mrow><mi>i</mi></mrow></msub><mo>,</mo><msub><mrow><mi>a</mi></mrow><mrow><mi>i</mi></mrow></msub><mo>&gt;</mo><mn>0</mn></mrow></math></span> <span><math><mrow><mo>(</mo><mi>i</mi><mo>=</mo><mn>1</mn><mo>,</mo><mn>2</mn><mo>)</mo></mrow></math></span> and <span><math><mrow><mi>β</mi><mo>&gt;</mo><mn>0</mn></mrow></math></span> are prescribed, <span><math><msub><mrow><mi>λ</mi></mrow><mrow><mi>i</mi></mrow></msub></math></span> are the Lagrange multipliers to be determined, the nonlinear functions <span><math><msub><mrow><mi>f</mi></mrow><mrow><mi>i</mi></mrow></msub></math></span> are continuous, and the potential functions <span><math><msub><mrow><mi>V</mi></mrow><mrow><mi>i</mi></mrow></msub></math></span> satisfy some suitable conditions. With the aid of the Ljusternik–Schnirelmann category theory and variational methods, we obtain the multiplicity and concentration phenomena of normalized solutions for the above system. As far as we know, this study is the first contribution regarding the concentration and multiplicity properties of normalized solutions for fractional <span><math><mi>p</mi></math></span>-Laplacian Schrödinger–Choquard system in <span><math><msup><mrow><mi>R</mi></mrow><mrow><mi>N</mi></mrow></msup></math></span>. To some extent, the main results included in this paper complement several recent contributions to the study of nonlinear Schrödinger systems (Chen and Zou, 2021; Gou and Jeanjean, 2016).</div></div>","PeriodicalId":50658,"journal":{"name":"Communications in Nonlinear Science and Numerical Simulation","volume":"144 ","pages":"Article 108665"},"PeriodicalIF":3.8000,"publicationDate":"2025-02-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Communications in Nonlinear Science and Numerical Simulation","FirstCategoryId":"100","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S1007570425000760","RegionNum":2,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"MATHEMATICS, APPLIED","Score":null,"Total":0}
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Abstract

In this paper, we consider the following Schrödinger–Choquard system in RN (Δ)psu1+(V1(ɛx)λ1)|u1|p2u1=μ1[1|x|NαF1(u1)]f1(u1)+βr1|u1|r12u1|u2|r2inRN,(Δ)psu2+(V2(ɛx)λ2)|u2|p2u2=μ2[1|x|NαF2(u2)]f2(u2)+βr2|u1|r1|u2|r22u2inRN,RN|u1|pdx=a1p,RN|u2|pdx=a2p,where (Δ)ps is the fractional p-Laplacian operator, α(0,N), s(0,1), r1,r2>1, r1+r2(p,p+p2sN), ɛ>0 is a parameter, μi,ai>0 (i=1,2) and β>0 are prescribed, λi are the Lagrange multipliers to be determined, the nonlinear functions fi are continuous, and the potential functions Vi satisfy some suitable conditions. With the aid of the Ljusternik–Schnirelmann category theory and variational methods, we obtain the multiplicity and concentration phenomena of normalized solutions for the above system. As far as we know, this study is the first contribution regarding the concentration and multiplicity properties of normalized solutions for fractional p-Laplacian Schrödinger–Choquard system in RN. To some extent, the main results included in this paper complement several recent contributions to the study of nonlinear Schrödinger systems (Chen and Zou, 2021; Gou and Jeanjean, 2016).
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RN中分数阶p-拉普拉斯Schrödinger-Choquard系统归一化解的浓度现象
在本文中,我们考虑以下Schrödinger-Choquard系统在RN(−Δ)psu1+(V1(x)−λ1) bbbu1 |p−2u1=μ1[1|x|N−α * F1(u1)] F1(u1) +βr1|u1|r1−2u1|u2|r2inRN,(−Δ)psu2+(V2(x)−λ2)|u2|p−2u2=μ2[1|x|N−α * F2(u2)] F2(u2) +βr2|u1|r1|u2|r2−2u2inRN,∫RN|u1|pdx=a1p,∫RN|u2|pdx=a2p,其中(−Δ)ps为分数阶p-拉普拉斯算子,α∈(0,N), s∈(0,1),r1,r2>1, r1+r2∈(p,p+p2sN), λ >;0为参数,μi,ai>0 (i=1,2)和β>;0为待确定的拉格朗日乘子,λi为待确定的拉格朗日乘子,非线性函数fi是连续的,势函数Vi满足一定的条件。借助Ljusternik-Schnirelmann范畴论和变分方法,我们得到了上述系统归一化解的多重性和集中现象。据我们所知,本研究是关于RN中分数阶p-拉普拉斯Schrödinger-Choquard系统归一化解的浓度和多重性的第一个贡献。在某种程度上,本文中包含的主要结果补充了最近对非线性Schrödinger系统研究的几项贡献(Chen和Zou, 2021;Gou and Jeanjean, 2016)。
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来源期刊
Communications in Nonlinear Science and Numerical Simulation
Communications in Nonlinear Science and Numerical Simulation MATHEMATICS, APPLIED-MATHEMATICS, INTERDISCIPLINARY APPLICATIONS
CiteScore
6.80
自引率
7.70%
发文量
378
审稿时长
78 days
期刊介绍: The journal publishes original research findings on experimental observation, mathematical modeling, theoretical analysis and numerical simulation, for more accurate description, better prediction or novel application, of nonlinear phenomena in science and engineering. It offers a venue for researchers to make rapid exchange of ideas and techniques in nonlinear science and complexity. The submission of manuscripts with cross-disciplinary approaches in nonlinear science and complexity is particularly encouraged. Topics of interest: Nonlinear differential or delay equations, Lie group analysis and asymptotic methods, Discontinuous systems, Fractals, Fractional calculus and dynamics, Nonlinear effects in quantum mechanics, Nonlinear stochastic processes, Experimental nonlinear science, Time-series and signal analysis, Computational methods and simulations in nonlinear science and engineering, Control of dynamical systems, Synchronization, Lyapunov analysis, High-dimensional chaos and turbulence, Chaos in Hamiltonian systems, Integrable systems and solitons, Collective behavior in many-body systems, Biological physics and networks, Nonlinear mechanical systems, Complex systems and complexity. No length limitation for contributions is set, but only concisely written manuscripts are published. Brief papers are published on the basis of Rapid Communications. Discussions of previously published papers are welcome.
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