{"title":"解析函数的边值","authors":"A. G. Ramm","doi":"10.17654/0972096023011","DOIUrl":null,"url":null,"abstract":"Let $D$ be a connected bounded domain in $\\R^2$, $S$ be its boundary which is closed, connected and smooth. Let $\\Phi(z)=\\frac 1 {2\\pi i}\\int_S\\frac{f(s)ds}{s-z}$, $f\\in L^1(S)$, $z=x+iy$. Boundary values of $\\Phi(z)$ on $S$ are studied. The function $\\Phi(t)$, $t\\in S$, is defined in a new way. Necessary and sufficient conditions are given for $f\\in L^1(S)$ to be boundary value of an analytic in $D$ function. The Sokhotsky-Plemelj formulas are derived for $f\\in L^1(S)$.","PeriodicalId":89368,"journal":{"name":"Far east journal of applied mathematics","volume":" ","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2023-05-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"BOUNDARY VALUES OF ANALYTIC FUNCTIONS\",\"authors\":\"A. G. Ramm\",\"doi\":\"10.17654/0972096023011\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Let $D$ be a connected bounded domain in $\\\\R^2$, $S$ be its boundary which is closed, connected and smooth. Let $\\\\Phi(z)=\\\\frac 1 {2\\\\pi i}\\\\int_S\\\\frac{f(s)ds}{s-z}$, $f\\\\in L^1(S)$, $z=x+iy$. Boundary values of $\\\\Phi(z)$ on $S$ are studied. The function $\\\\Phi(t)$, $t\\\\in S$, is defined in a new way. Necessary and sufficient conditions are given for $f\\\\in L^1(S)$ to be boundary value of an analytic in $D$ function. The Sokhotsky-Plemelj formulas are derived for $f\\\\in L^1(S)$.\",\"PeriodicalId\":89368,\"journal\":{\"name\":\"Far east journal of applied mathematics\",\"volume\":\" \",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2023-05-15\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Far east journal of applied mathematics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.17654/0972096023011\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Far east journal of applied mathematics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.17654/0972096023011","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Let $D$ be a connected bounded domain in $\R^2$, $S$ be its boundary which is closed, connected and smooth. Let $\Phi(z)=\frac 1 {2\pi i}\int_S\frac{f(s)ds}{s-z}$, $f\in L^1(S)$, $z=x+iy$. Boundary values of $\Phi(z)$ on $S$ are studied. The function $\Phi(t)$, $t\in S$, is defined in a new way. Necessary and sufficient conditions are given for $f\in L^1(S)$ to be boundary value of an analytic in $D$ function. The Sokhotsky-Plemelj formulas are derived for $f\in L^1(S)$.