On the rate of decay at infinity for solutions to the Schrödinger equation in a half-cylinder

IF 0.7 4区 数学 Q2 MATHEMATICS St Petersburg Mathematical Journal Pub Date : 2022-12-16 DOI:10.1090/spmj/1746
S. Krymskii, N. Filonov
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Assume that the potential <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"upper V\">\n <mml:semantics>\n <mml:mi>V</mml:mi>\n <mml:annotation encoding=\"application/x-tex\">V</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula> is bounded. The possible rate of decay at infinity for a nontrivial solution is studied. It is shown that the fastest rate of decay is <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"e Superscript minus c x\">\n <mml:semantics>\n <mml:msup>\n <mml:mi>e</mml:mi>\n <mml:mrow class=\"MJX-TeXAtom-ORD\">\n <mml:mo>−<!-- − --></mml:mo>\n <mml:mi>c</mml:mi>\n <mml:mi>x</mml:mi>\n </mml:mrow>\n </mml:msup>\n <mml:annotation encoding=\"application/x-tex\">e^{-cx}</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula> for <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"d equals 1\">\n <mml:semantics>\n <mml:mrow>\n <mml:mi>d</mml:mi>\n <mml:mo>=</mml:mo>\n <mml:mn>1</mml:mn>\n </mml:mrow>\n <mml:annotation encoding=\"application/x-tex\">d=1</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula> or <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"2\">\n <mml:semantics>\n <mml:mn>2</mml:mn>\n <mml:annotation encoding=\"application/x-tex\">2</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula> and <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"e Superscript minus c x Super Superscript 4 slash 3\">\n <mml:semantics>\n <mml:msup>\n <mml:mi>e</mml:mi>\n <mml:mrow class=\"MJX-TeXAtom-ORD\">\n <mml:mo>−<!-- − --></mml:mo>\n <mml:mi>c</mml:mi>\n <mml:msup>\n <mml:mi>x</mml:mi>\n <mml:mrow class=\"MJX-TeXAtom-ORD\">\n <mml:mn>4</mml:mn>\n <mml:mrow class=\"MJX-TeXAtom-ORD\">\n <mml:mo>/</mml:mo>\n </mml:mrow>\n <mml:mn>3</mml:mn>\n </mml:mrow>\n </mml:msup>\n </mml:mrow>\n </mml:msup>\n <mml:annotation encoding=\"application/x-tex\">e^{-cx^{4/3}}</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula> for <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"d greater-than-or-equal-to 3\">\n <mml:semantics>\n <mml:mrow>\n <mml:mi>d</mml:mi>\n <mml:mo>≥<!-- ≥ --></mml:mo>\n <mml:mn>3</mml:mn>\n </mml:mrow>\n <mml:annotation encoding=\"application/x-tex\">d\\ge 3</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula>; here <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"x\">\n <mml:semantics>\n <mml:mi>x</mml:mi>\n <mml:annotation encoding=\"application/x-tex\">x</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula> is the axial variable.</p>","PeriodicalId":51162,"journal":{"name":"St Petersburg Mathematical Journal","volume":null,"pages":null},"PeriodicalIF":0.7000,"publicationDate":"2022-12-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"St Petersburg Mathematical Journal","FirstCategoryId":"100","ListUrlMain":"https://doi.org/10.1090/spmj/1746","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: 1

Abstract

Consider the equation Δ u + V u = 0 -\Delta u + Vu = 0 in the half-cylinder [ 0 , ) × ( 0 , 2 π ) d [0, \infty ) \times (0,2\pi )^d with periodic boundary conditions. Assume that the potential V V is bounded. The possible rate of decay at infinity for a nontrivial solution is studied. It is shown that the fastest rate of decay is e c x e^{-cx} for d = 1 d=1 or 2 2 and e c x 4 / 3 e^{-cx^{4/3}} for d 3 d\ge 3 ; here x x is the axial variable.

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半圆柱体中Schrödinger方程解在无穷远处的衰减速率
考虑半圆柱体[0,∞)×(0,2π)d[0,\infty)\times(0,2\pi)中的方程−Δu+V u=0-\Δu+Vu=0^d具有周期性边界条件。假设电势V V是有界的。研究了一个非平凡解在无穷远处的可能衰变率。结果表明,当d=1 d=1或2 2时,最快的衰变率是e−c x e ^{-cx};当d≥3时,最慢的衰变率为e−c×第3页;这里x x是轴向变量。
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来源期刊
CiteScore
1.00
自引率
12.50%
发文量
52
审稿时长
>12 weeks
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.
期刊最新文献
Shape, velocity, and exact controllability for the wave equation on a graph with cycle On Kitaev’s determinant formula Resolvent stochastic processes Complete nonselfadjointness for Schrödinger operators on the semi-axis Behavior of large eigenvalues for the two-photon asymmetric quantum Rabi model
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