{"title":"波导中的非齐次亥姆霍兹方程。能量法的存在性和唯一性结果","authors":"B. Schweizer","doi":"10.1017/s0956792522000080","DOIUrl":null,"url":null,"abstract":"The Helmholtz equation \n \n \n \n$-\\nabla\\cdot (a\\nabla u) - \\omega^2 u = f$\n\n \n is considered in an unbounded wave guide \n \n \n \n$\\Omega := \\mathbb{R} \\times S \\subset \\mathbb{R}^d$\n\n \n , \n \n \n \n$S\\subset \\mathbb{R}^{d-1}$\n\n \n a bounded domain. The coefficient a is strictly elliptic and either periodic in the unbounded direction \n \n \n \n$x_1 \\in \\mathbb{R}$\n\n \n or periodic outside a compact subset; in the latter case, two different periodic media can be used in the two unbounded directions. For non-singular frequencies \n \n \n \n$\\omega$\n\n \n , we show the existence of a solution u. While previous proofs of such results were based on analyticity arguments within operator theory, here, only energy methods are used.","PeriodicalId":2,"journal":{"name":"ACS Applied Bio Materials","volume":null,"pages":null},"PeriodicalIF":4.6000,"publicationDate":"2022-03-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Inhomogeneous Helmholtz equations in wave guides – existence and uniqueness results with energy methods\",\"authors\":\"B. Schweizer\",\"doi\":\"10.1017/s0956792522000080\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The Helmholtz equation \\n \\n \\n \\n$-\\\\nabla\\\\cdot (a\\\\nabla u) - \\\\omega^2 u = f$\\n\\n \\n is considered in an unbounded wave guide \\n \\n \\n \\n$\\\\Omega := \\\\mathbb{R} \\\\times S \\\\subset \\\\mathbb{R}^d$\\n\\n \\n , \\n \\n \\n \\n$S\\\\subset \\\\mathbb{R}^{d-1}$\\n\\n \\n a bounded domain. The coefficient a is strictly elliptic and either periodic in the unbounded direction \\n \\n \\n \\n$x_1 \\\\in \\\\mathbb{R}$\\n\\n \\n or periodic outside a compact subset; in the latter case, two different periodic media can be used in the two unbounded directions. For non-singular frequencies \\n \\n \\n \\n$\\\\omega$\\n\\n \\n , we show the existence of a solution u. While previous proofs of such results were based on analyticity arguments within operator theory, here, only energy methods are used.\",\"PeriodicalId\":2,\"journal\":{\"name\":\"ACS Applied Bio Materials\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":4.6000,\"publicationDate\":\"2022-03-30\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"ACS Applied Bio Materials\",\"FirstCategoryId\":\"100\",\"ListUrlMain\":\"https://doi.org/10.1017/s0956792522000080\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"MATERIALS SCIENCE, BIOMATERIALS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"ACS Applied Bio Materials","FirstCategoryId":"100","ListUrlMain":"https://doi.org/10.1017/s0956792522000080","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"MATERIALS SCIENCE, BIOMATERIALS","Score":null,"Total":0}
Inhomogeneous Helmholtz equations in wave guides – existence and uniqueness results with energy methods
The Helmholtz equation
$-\nabla\cdot (a\nabla u) - \omega^2 u = f$
is considered in an unbounded wave guide
$\Omega := \mathbb{R} \times S \subset \mathbb{R}^d$
,
$S\subset \mathbb{R}^{d-1}$
a bounded domain. The coefficient a is strictly elliptic and either periodic in the unbounded direction
$x_1 \in \mathbb{R}$
or periodic outside a compact subset; in the latter case, two different periodic media can be used in the two unbounded directions. For non-singular frequencies
$\omega$
, we show the existence of a solution u. While previous proofs of such results were based on analyticity arguments within operator theory, here, only energy methods are used.