{"title":"指数多项式矩阵的伪谱","authors":"Robert M Corless","doi":"10.1145/1577190.1577192","DOIUrl":null,"url":null,"abstract":"ẋ(t) = Ax(t) (1) where x ∈ C and A ∈ C(n×n), together with (say) initial conditions x(0) = x0, occurs often as a simple model of many applied dynamical phenomena, for instance in theoretical evolution or in the physics of lasers, to name only two out of many possibilities. The so-called characteristic equation det(λI − A) = 0 occurs when looking for solutions of the form x(t) = ev for some vector v ∈ C. Understanding the exact solution x(t) = exp(At)x0 comes from the eigenvalues (spectrum) of A, and more recently from the pseudospectrum of A, by which is meant the set [5, 17]","PeriodicalId":308716,"journal":{"name":"Symbolic-Numeric Computation","volume":"37 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2009-08-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"Pseudospectra for exponential polynomial matrices\",\"authors\":\"Robert M Corless\",\"doi\":\"10.1145/1577190.1577192\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"ẋ(t) = Ax(t) (1) where x ∈ C and A ∈ C(n×n), together with (say) initial conditions x(0) = x0, occurs often as a simple model of many applied dynamical phenomena, for instance in theoretical evolution or in the physics of lasers, to name only two out of many possibilities. The so-called characteristic equation det(λI − A) = 0 occurs when looking for solutions of the form x(t) = ev for some vector v ∈ C. Understanding the exact solution x(t) = exp(At)x0 comes from the eigenvalues (spectrum) of A, and more recently from the pseudospectrum of A, by which is meant the set [5, 17]\",\"PeriodicalId\":308716,\"journal\":{\"name\":\"Symbolic-Numeric Computation\",\"volume\":\"37 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2009-08-03\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Symbolic-Numeric Computation\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1145/1577190.1577192\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Symbolic-Numeric Computation","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1145/1577190.1577192","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
ẋ(t) = Ax(t) (1) where x ∈ C and A ∈ C(n×n), together with (say) initial conditions x(0) = x0, occurs often as a simple model of many applied dynamical phenomena, for instance in theoretical evolution or in the physics of lasers, to name only two out of many possibilities. The so-called characteristic equation det(λI − A) = 0 occurs when looking for solutions of the form x(t) = ev for some vector v ∈ C. Understanding the exact solution x(t) = exp(At)x0 comes from the eigenvalues (spectrum) of A, and more recently from the pseudospectrum of A, by which is meant the set [5, 17]