{"title":"具有组合非线性的准线性薛定谔方程的归一化解","authors":"Anmin Mao, Shuyao Lu","doi":"10.1017/s001309152400004x","DOIUrl":null,"url":null,"abstract":"We consider the radially symmetric positive solutions to quasilinear problem <jats:disp-formula> <jats:alternatives> <jats:graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" mimetype=\"image\" xlink:href=\"S001309152400004X_eqnU1.png\" /> <jats:tex-math>\\begin{equation*}-\\triangle u-u\\triangle u^{2}+\\lambda u=f(u),\\quad{\\rm in} \\ \\mathbb{R}^{N},\\end{equation*}</jats:tex-math> </jats:alternatives> </jats:disp-formula> having prescribed mass <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" mimetype=\"image\" xlink:href=\"S001309152400004X_inline1.png\" /> <jats:tex-math>$\\int_{\\mathbb{R}^{N}}|u|^2 =a^2,$</jats:tex-math> </jats:alternatives> </jats:inline-formula> where <jats:italic>a</jats:italic> > 0 is a constant, <jats:italic>λ</jats:italic> appears as a Lagrange multiplier. We focus on the pure <jats:italic>L</jats:italic><jats:sup>2</jats:sup>-supercritical case and combination case of <jats:italic>L</jats:italic><jats:sup>2</jats:sup>-subcritical and <jats:italic>L</jats:italic><jats:sup>2</jats:sup>-supercritical nonlinearities <jats:disp-formula> <jats:alternatives> <jats:graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" mimetype=\"image\" xlink:href=\"S001309152400004X_eqnU2.png\" /> <jats:tex-math>\\begin{equation*}f(u)=\\tau |u|^{q-2}u+|u|^{p-2}u,\\quad \\tau \\gt 0,\\qquad{\\rm where}\\ \\ 2 \\lt q \\lt 2+\\frac{4}{N} \\ {\\rm and} \\quad \\ p \\gt \\bar{p},\\end{equation*}</jats:tex-math> </jats:alternatives> </jats:disp-formula> where <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" mime-subtype=\"png\" mimetype=\"image\" xlink:href=\"S001309152400004X_inline2.png\" /> <jats:tex-math>$\\bar{p}:=4+\\frac{4}{N}$</jats:tex-math> </jats:alternatives> </jats:inline-formula> is the <jats:italic>L</jats:italic><jats:sup>2</jats:sup>-critical exponent. Our work extends and develops some recent results in the literature.","PeriodicalId":0,"journal":{"name":"","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2024-04-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Normalized solutions to the quasilinear Schrödinger equations with combined nonlinearities\",\"authors\":\"Anmin Mao, Shuyao Lu\",\"doi\":\"10.1017/s001309152400004x\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We consider the radially symmetric positive solutions to quasilinear problem <jats:disp-formula> <jats:alternatives> <jats:graphic xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\" mime-subtype=\\\"png\\\" mimetype=\\\"image\\\" xlink:href=\\\"S001309152400004X_eqnU1.png\\\" /> <jats:tex-math>\\\\begin{equation*}-\\\\triangle u-u\\\\triangle u^{2}+\\\\lambda u=f(u),\\\\quad{\\\\rm in} \\\\ \\\\mathbb{R}^{N},\\\\end{equation*}</jats:tex-math> </jats:alternatives> </jats:disp-formula> having prescribed mass <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\" mime-subtype=\\\"png\\\" mimetype=\\\"image\\\" xlink:href=\\\"S001309152400004X_inline1.png\\\" /> <jats:tex-math>$\\\\int_{\\\\mathbb{R}^{N}}|u|^2 =a^2,$</jats:tex-math> </jats:alternatives> </jats:inline-formula> where <jats:italic>a</jats:italic> > 0 is a constant, <jats:italic>λ</jats:italic> appears as a Lagrange multiplier. We focus on the pure <jats:italic>L</jats:italic><jats:sup>2</jats:sup>-supercritical case and combination case of <jats:italic>L</jats:italic><jats:sup>2</jats:sup>-subcritical and <jats:italic>L</jats:italic><jats:sup>2</jats:sup>-supercritical nonlinearities <jats:disp-formula> <jats:alternatives> <jats:graphic xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\" mime-subtype=\\\"png\\\" mimetype=\\\"image\\\" xlink:href=\\\"S001309152400004X_eqnU2.png\\\" /> <jats:tex-math>\\\\begin{equation*}f(u)=\\\\tau |u|^{q-2}u+|u|^{p-2}u,\\\\quad \\\\tau \\\\gt 0,\\\\qquad{\\\\rm where}\\\\ \\\\ 2 \\\\lt q \\\\lt 2+\\\\frac{4}{N} \\\\ {\\\\rm and} \\\\quad \\\\ p \\\\gt \\\\bar{p},\\\\end{equation*}</jats:tex-math> </jats:alternatives> </jats:disp-formula> where <jats:inline-formula> <jats:alternatives> <jats:inline-graphic xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\" mime-subtype=\\\"png\\\" mimetype=\\\"image\\\" xlink:href=\\\"S001309152400004X_inline2.png\\\" /> <jats:tex-math>$\\\\bar{p}:=4+\\\\frac{4}{N}$</jats:tex-math> </jats:alternatives> </jats:inline-formula> is the <jats:italic>L</jats:italic><jats:sup>2</jats:sup>-critical exponent. Our work extends and develops some recent results in the literature.\",\"PeriodicalId\":0,\"journal\":{\"name\":\"\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":0.0,\"publicationDate\":\"2024-04-12\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"\",\"FirstCategoryId\":\"100\",\"ListUrlMain\":\"https://doi.org/10.1017/s001309152400004x\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"","FirstCategoryId":"100","ListUrlMain":"https://doi.org/10.1017/s001309152400004x","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Normalized solutions to the quasilinear Schrödinger equations with combined nonlinearities
We consider the radially symmetric positive solutions to quasilinear problem \begin{equation*}-\triangle u-u\triangle u^{2}+\lambda u=f(u),\quad{\rm in} \ \mathbb{R}^{N},\end{equation*} having prescribed mass $\int_{\mathbb{R}^{N}}|u|^2 =a^2,$ where a > 0 is a constant, λ appears as a Lagrange multiplier. We focus on the pure L2-supercritical case and combination case of L2-subcritical and L2-supercritical nonlinearities \begin{equation*}f(u)=\tau |u|^{q-2}u+|u|^{p-2}u,\quad \tau \gt 0,\qquad{\rm where}\ \ 2 \lt q \lt 2+\frac{4}{N} \ {\rm and} \quad \ p \gt \bar{p},\end{equation*} where $\bar{p}:=4+\frac{4}{N}$ is the L2-critical exponent. Our work extends and develops some recent results in the literature.