{"title":"Singular Value Analyses of Inversion of Laplace and Optical Imaging Transforms","authors":"M. Bertero, E. Pike","doi":"10.1364/srs.1983.tha20","DOIUrl":null,"url":null,"abstract":"The use of the eigenvalues and eigenfunctions of the first order Fredholm equations describing optical imaging has long been known. The eigenvalues and eigenfunctions of the first order Fredholm equation of the Laplace transform have only recently been discovered and similarly used (McWhirter and Pike 1978). Let us consider for simplicity the one dimensional case with magnification unity. For an eigenfunction to be defined the linear mapping A:f → g of the \"object\" f into its \"image\" g must define a compact bijective operator A of, say, L2 (−1,+1) into itself.","PeriodicalId":279385,"journal":{"name":"Topical Meeting on Signal Recovery and Synthesis with Incomplete Information and Partial Constraints","volume":"32 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Topical Meeting on Signal Recovery and Synthesis with Incomplete Information and Partial Constraints","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1364/srs.1983.tha20","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
The use of the eigenvalues and eigenfunctions of the first order Fredholm equations describing optical imaging has long been known. The eigenvalues and eigenfunctions of the first order Fredholm equation of the Laplace transform have only recently been discovered and similarly used (McWhirter and Pike 1978). Let us consider for simplicity the one dimensional case with magnification unity. For an eigenfunction to be defined the linear mapping A:f → g of the "object" f into its "image" g must define a compact bijective operator A of, say, L2 (−1,+1) into itself.
描述光学成像的一阶Fredholm方程的特征值和特征函数的使用早已为人所知。拉普拉斯变换的一阶Fredholm方程的特征值和特征函数直到最近才被发现并被类似地使用(McWhirter and Pike 1978)。为了简单起见,让我们考虑具有放大统一度的一维情况。要定义一个特征函数,从“对象”f到它的“像”g的线性映射A:f→g必须定义一个紧双射算子A,比如L2(- 1,+1)到它自身。