{"title":"具有测量值势的Schrödinger方程的Strichartz估计","authors":"M. Erdogan, M. Goldberg, William Green","doi":"10.1090/bproc/79","DOIUrl":null,"url":null,"abstract":"<p>We prove Strichartz estimates for the Schrödinger equation in <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"double-struck upper R Superscript n\">\n <mml:semantics>\n <mml:msup>\n <mml:mrow class=\"MJX-TeXAtom-ORD\">\n <mml:mi mathvariant=\"double-struck\">R</mml:mi>\n </mml:mrow>\n <mml:mi>n</mml:mi>\n </mml:msup>\n <mml:annotation encoding=\"application/x-tex\">\\mathbb {R}^n</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula>, <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"n greater-than-or-equal-to 3\">\n <mml:semantics>\n <mml:mrow>\n <mml:mi>n</mml:mi>\n <mml:mo>≥<!-- ≥ --></mml:mo>\n <mml:mn>3</mml:mn>\n </mml:mrow>\n <mml:annotation encoding=\"application/x-tex\">n\\geq 3</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula>, with a Hamiltonian <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"upper H equals negative normal upper Delta plus mu\">\n <mml:semantics>\n <mml:mrow>\n <mml:mi>H</mml:mi>\n <mml:mo>=</mml:mo>\n <mml:mo>−<!-- − --></mml:mo>\n <mml:mi mathvariant=\"normal\">Δ<!-- Δ --></mml:mi>\n <mml:mo>+</mml:mo>\n <mml:mi>μ<!-- μ --></mml:mi>\n </mml:mrow>\n <mml:annotation encoding=\"application/x-tex\">H = -\\Delta + \\mu</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula>. The perturbation <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"mu\">\n <mml:semantics>\n <mml:mi>μ<!-- μ --></mml:mi>\n <mml:annotation encoding=\"application/x-tex\">\\mu</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula> is a compactly supported measure in <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"double-struck upper R Superscript n\">\n <mml:semantics>\n <mml:msup>\n <mml:mrow class=\"MJX-TeXAtom-ORD\">\n <mml:mi mathvariant=\"double-struck\">R</mml:mi>\n </mml:mrow>\n <mml:mi>n</mml:mi>\n </mml:msup>\n <mml:annotation encoding=\"application/x-tex\">\\mathbb {R}^n</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula> with dimension <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"alpha greater-than n minus left-parenthesis 1 plus StartFraction 1 Over n minus 1 EndFraction right-parenthesis\">\n <mml:semantics>\n <mml:mrow>\n <mml:mi>α<!-- α --></mml:mi>\n <mml:mo>></mml:mo>\n <mml:mi>n</mml:mi>\n <mml:mo>−<!-- − --></mml:mo>\n <mml:mo stretchy=\"false\">(</mml:mo>\n <mml:mn>1</mml:mn>\n <mml:mo>+</mml:mo>\n <mml:mfrac>\n <mml:mn>1</mml:mn>\n <mml:mrow>\n <mml:mi>n</mml:mi>\n <mml:mo>−<!-- − --></mml:mo>\n <mml:mn>1</mml:mn>\n </mml:mrow>\n </mml:mfrac>\n <mml:mo stretchy=\"false\">)</mml:mo>\n </mml:mrow>\n <mml:annotation encoding=\"application/x-tex\">\\alpha > n-(1+\\frac {1}{n-1})</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula>. The main intermediate step is a local decay estimate in <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"upper L squared left-parenthesis mu right-parenthesis\">\n <mml:semantics>\n <mml:mrow>\n <mml:msup>\n <mml:mi>L</mml:mi>\n <mml:mn>2</mml:mn>\n </mml:msup>\n <mml:mo stretchy=\"false\">(</mml:mo>\n <mml:mi>μ<!-- μ --></mml:mi>\n <mml:mo stretchy=\"false\">)</mml:mo>\n </mml:mrow>\n <mml:annotation encoding=\"application/x-tex\">L^2(\\mu )</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula> for both the free and perturbed Schrödinger evolution.</p>","PeriodicalId":106316,"journal":{"name":"Proceedings of the American Mathematical Society, Series B","volume":"5 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2021-11-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Strichartz estimates for the Schrödinger equation with a measure-valued potential\",\"authors\":\"M. Erdogan, M. Goldberg, William Green\",\"doi\":\"10.1090/bproc/79\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>We prove Strichartz estimates for the Schrödinger equation in <inline-formula content-type=\\\"math/mathml\\\">\\n<mml:math xmlns:mml=\\\"http://www.w3.org/1998/Math/MathML\\\" alttext=\\\"double-struck upper R Superscript n\\\">\\n <mml:semantics>\\n <mml:msup>\\n <mml:mrow class=\\\"MJX-TeXAtom-ORD\\\">\\n <mml:mi mathvariant=\\\"double-struck\\\">R</mml:mi>\\n </mml:mrow>\\n <mml:mi>n</mml:mi>\\n </mml:msup>\\n <mml:annotation encoding=\\\"application/x-tex\\\">\\\\mathbb {R}^n</mml:annotation>\\n </mml:semantics>\\n</mml:math>\\n</inline-formula>, <inline-formula content-type=\\\"math/mathml\\\">\\n<mml:math xmlns:mml=\\\"http://www.w3.org/1998/Math/MathML\\\" alttext=\\\"n greater-than-or-equal-to 3\\\">\\n <mml:semantics>\\n <mml:mrow>\\n <mml:mi>n</mml:mi>\\n <mml:mo>≥<!-- ≥ --></mml:mo>\\n <mml:mn>3</mml:mn>\\n </mml:mrow>\\n <mml:annotation encoding=\\\"application/x-tex\\\">n\\\\geq 3</mml:annotation>\\n </mml:semantics>\\n</mml:math>\\n</inline-formula>, with a Hamiltonian <inline-formula content-type=\\\"math/mathml\\\">\\n<mml:math xmlns:mml=\\\"http://www.w3.org/1998/Math/MathML\\\" alttext=\\\"upper H equals negative normal upper Delta plus mu\\\">\\n <mml:semantics>\\n <mml:mrow>\\n <mml:mi>H</mml:mi>\\n <mml:mo>=</mml:mo>\\n <mml:mo>−<!-- − --></mml:mo>\\n <mml:mi mathvariant=\\\"normal\\\">Δ<!-- Δ --></mml:mi>\\n <mml:mo>+</mml:mo>\\n <mml:mi>μ<!-- μ --></mml:mi>\\n </mml:mrow>\\n <mml:annotation encoding=\\\"application/x-tex\\\">H = -\\\\Delta + \\\\mu</mml:annotation>\\n </mml:semantics>\\n</mml:math>\\n</inline-formula>. The perturbation <inline-formula content-type=\\\"math/mathml\\\">\\n<mml:math xmlns:mml=\\\"http://www.w3.org/1998/Math/MathML\\\" alttext=\\\"mu\\\">\\n <mml:semantics>\\n <mml:mi>μ<!-- μ --></mml:mi>\\n <mml:annotation encoding=\\\"application/x-tex\\\">\\\\mu</mml:annotation>\\n </mml:semantics>\\n</mml:math>\\n</inline-formula> is a compactly supported measure in <inline-formula content-type=\\\"math/mathml\\\">\\n<mml:math xmlns:mml=\\\"http://www.w3.org/1998/Math/MathML\\\" alttext=\\\"double-struck upper R Superscript n\\\">\\n <mml:semantics>\\n <mml:msup>\\n <mml:mrow class=\\\"MJX-TeXAtom-ORD\\\">\\n <mml:mi mathvariant=\\\"double-struck\\\">R</mml:mi>\\n </mml:mrow>\\n <mml:mi>n</mml:mi>\\n </mml:msup>\\n <mml:annotation encoding=\\\"application/x-tex\\\">\\\\mathbb {R}^n</mml:annotation>\\n </mml:semantics>\\n</mml:math>\\n</inline-formula> with dimension <inline-formula content-type=\\\"math/mathml\\\">\\n<mml:math xmlns:mml=\\\"http://www.w3.org/1998/Math/MathML\\\" alttext=\\\"alpha greater-than n minus left-parenthesis 1 plus StartFraction 1 Over n minus 1 EndFraction right-parenthesis\\\">\\n <mml:semantics>\\n <mml:mrow>\\n <mml:mi>α<!-- α --></mml:mi>\\n <mml:mo>></mml:mo>\\n <mml:mi>n</mml:mi>\\n <mml:mo>−<!-- − --></mml:mo>\\n <mml:mo stretchy=\\\"false\\\">(</mml:mo>\\n <mml:mn>1</mml:mn>\\n <mml:mo>+</mml:mo>\\n <mml:mfrac>\\n <mml:mn>1</mml:mn>\\n <mml:mrow>\\n <mml:mi>n</mml:mi>\\n <mml:mo>−<!-- − --></mml:mo>\\n <mml:mn>1</mml:mn>\\n </mml:mrow>\\n </mml:mfrac>\\n <mml:mo stretchy=\\\"false\\\">)</mml:mo>\\n </mml:mrow>\\n <mml:annotation encoding=\\\"application/x-tex\\\">\\\\alpha > n-(1+\\\\frac {1}{n-1})</mml:annotation>\\n </mml:semantics>\\n</mml:math>\\n</inline-formula>. The main intermediate step is a local decay estimate in <inline-formula content-type=\\\"math/mathml\\\">\\n<mml:math xmlns:mml=\\\"http://www.w3.org/1998/Math/MathML\\\" alttext=\\\"upper L squared left-parenthesis mu right-parenthesis\\\">\\n <mml:semantics>\\n <mml:mrow>\\n <mml:msup>\\n <mml:mi>L</mml:mi>\\n <mml:mn>2</mml:mn>\\n </mml:msup>\\n <mml:mo stretchy=\\\"false\\\">(</mml:mo>\\n <mml:mi>μ<!-- μ --></mml:mi>\\n <mml:mo stretchy=\\\"false\\\">)</mml:mo>\\n </mml:mrow>\\n <mml:annotation encoding=\\\"application/x-tex\\\">L^2(\\\\mu )</mml:annotation>\\n </mml:semantics>\\n</mml:math>\\n</inline-formula> for both the free and perturbed Schrödinger evolution.</p>\",\"PeriodicalId\":106316,\"journal\":{\"name\":\"Proceedings of the American Mathematical Society, Series B\",\"volume\":\"5 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2021-11-22\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Proceedings of the American Mathematical Society, Series B\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1090/bproc/79\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Proceedings of the American Mathematical Society, Series B","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1090/bproc/79","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
摘要
我们证明Strichartz薛定谔的保守for the equation in R n \ mathbb {R) ^ n , n≥3 \ geq 3里,用a哈密顿 H = −Δ + μH = -三角洲+ \你。《perturbationμ\你是个compactly supported所拘束的 R n \ mathbb {R ^ n和维度的 α > n− ( 1 + 1 n − 1 ) \ 阿尔法> n - (1 + \ frac {1} {n-1})。《玩中级站是a local decay estimate in L 2 ( μ ) L ^ 2 (\ mu)一起的两人薛定谔(free and perturbed进化。
Strichartz estimates for the Schrödinger equation with a measure-valued potential
We prove Strichartz estimates for the Schrödinger equation in Rn\mathbb {R}^n, n≥3n\geq 3, with a Hamiltonian H=−Δ+μH = -\Delta + \mu. The perturbation μ\mu is a compactly supported measure in Rn\mathbb {R}^n with dimension α>n−(1+1n−1)\alpha > n-(1+\frac {1}{n-1}). The main intermediate step is a local decay estimate in L2(μ)L^2(\mu ) for both the free and perturbed Schrödinger evolution.