{"title":"Schrödinger operator with decreasing potential in a cylinder","authors":"N. Filonov","doi":"10.1090/spmj/1694","DOIUrl":null,"url":null,"abstract":"<p>The Schrödinger operator <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"negative normal upper Delta plus upper V left-parenthesis x comma y right-parenthesis\">\n <mml:semantics>\n <mml:mrow>\n <mml:mo>−<!-- − --></mml:mo>\n <mml:mi mathvariant=\"normal\">Δ<!-- Δ --></mml:mi>\n <mml:mo>+</mml:mo>\n <mml:mi>V</mml:mi>\n <mml:mo stretchy=\"false\">(</mml:mo>\n <mml:mi>x</mml:mi>\n <mml:mo>,</mml:mo>\n <mml:mi>y</mml:mi>\n <mml:mo stretchy=\"false\">)</mml:mo>\n </mml:mrow>\n <mml:annotation encoding=\"application/x-tex\">-\\Delta + V(x,y)</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula> is considered in a cylinder <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"double-struck upper R Superscript m Baseline times upper U\">\n <mml:semantics>\n <mml:mrow>\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>m</mml:mi>\n </mml:msup>\n <mml:mo>×<!-- × --></mml:mo>\n <mml:mi>U</mml:mi>\n </mml:mrow>\n <mml:annotation encoding=\"application/x-tex\">\\mathbb {R}^m \\times U</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula>, where <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"upper U\">\n <mml:semantics>\n <mml:mi>U</mml:mi>\n <mml:annotation encoding=\"application/x-tex\">U</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula> is a bounded domain 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 d\">\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>d</mml:mi>\n </mml:msup>\n <mml:annotation encoding=\"application/x-tex\">\\mathbb {R}^d</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula>. The spectrum of such an operator is studied under the assumption that the potential decreases in longitudinal variables, <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"StartAbsoluteValue upper V left-parenthesis x comma y right-parenthesis EndAbsoluteValue less-than-or-equal-to upper C mathematical left-angle x mathematical right-angle Superscript negative rho\">\n <mml:semantics>\n <mml:mrow>\n <mml:mrow class=\"MJX-TeXAtom-ORD\">\n <mml:mo stretchy=\"false\">|</mml:mo>\n </mml:mrow>\n <mml:mi>V</mml:mi>\n <mml:mo stretchy=\"false\">(</mml:mo>\n <mml:mi>x</mml:mi>\n <mml:mo>,</mml:mo>\n <mml:mi>y</mml:mi>\n <mml:mo stretchy=\"false\">)</mml:mo>\n <mml:mrow class=\"MJX-TeXAtom-ORD\">\n <mml:mo stretchy=\"false\">|</mml:mo>\n </mml:mrow>\n <mml:mo>≤<!-- ≤ --></mml:mo>\n <mml:mi>C</mml:mi>\n <mml:mo fence=\"false\" stretchy=\"false\">⟨<!-- ⟨ --></mml:mo>\n <mml:mi>x</mml:mi>\n <mml:msup>\n <mml:mo fence=\"false\" stretchy=\"false\">⟩<!-- ⟩ --></mml:mo>\n <mml:mrow class=\"MJX-TeXAtom-ORD\">\n <mml:mo>−<!-- − --></mml:mo>\n <mml:mi>ρ<!-- ρ --></mml:mi>\n </mml:mrow>\n </mml:msup>\n </mml:mrow>\n <mml:annotation encoding=\"application/x-tex\">|V(x,y)| \\le C \\langle x\\rangle ^{-\\rho }</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula>. If <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"rho greater-than 1\">\n <mml:semantics>\n <mml:mrow>\n <mml:mi>ρ<!-- ρ --></mml:mi>\n <mml:mo>></mml:mo>\n <mml:mn>1</mml:mn>\n </mml:mrow>\n <mml:annotation encoding=\"application/x-tex\">\\rho > 1</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula>, then the wave operators exist and are complete; the Birman invariance principle and the limiting absorption principle hold true; the absolute continuous spectrum fills the semiaxis; the singular continuous spectrum is empty; the eigenvalues can accumulate to the thresholds only.</p>","PeriodicalId":51162,"journal":{"name":"St Petersburg Mathematical Journal","volume":" ","pages":""},"PeriodicalIF":0.7000,"publicationDate":"2021-12-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"2","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"St Petersburg Mathematical Journal","FirstCategoryId":"100","ListUrlMain":"https://doi.org/10.1090/spmj/1694","RegionNum":4,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"MATHEMATICS","Score":null,"Total":0}
引用次数: 2
Abstract
The Schrödinger operator −Δ+V(x,y)-\Delta + V(x,y) is considered in a cylinder Rm×U\mathbb {R}^m \times U, where UU is a bounded domain in Rd\mathbb {R}^d. The spectrum of such an operator is studied under the assumption that the potential decreases in longitudinal variables, |V(x,y)|≤C⟨x⟩−ρ|V(x,y)| \le C \langle x\rangle ^{-\rho }. If ρ>1\rho > 1, then the wave operators exist and are complete; the Birman invariance principle and the limiting absorption principle hold true; the absolute continuous spectrum fills the semiaxis; the singular continuous spectrum is empty; the eigenvalues can accumulate to the thresholds only.
期刊介绍:
This journal is a cover-to-cover translation into English of Algebra i Analiz, published six times a year by the mathematics section of the Russian Academy of Sciences.