{"title":"矩阵多项式的根函数及其在微分方程和亚纯矩阵函数中的应用","authors":"Muhamed Borogovac","doi":"10.1007/s43036-025-00432-2","DOIUrl":null,"url":null,"abstract":"<div><p>First, we present a method for obtaining a canonical set of root functions and Jordan chains of the invertible matrix polynomial <i>L</i>(<i>z</i>) through elementary transformations of the matrix <i>L</i>(<i>z</i>) alone. This method provides a new and simple approach to deriving a general solution of the system of ordinary linear differential equations <span>\\(L\\left( \\frac{d}{dt}\\right) u=0\\)</span>, where <i>u</i>(<i>t</i>) is <i>n</i>-dimensional unknown function. We illustrate the effectiveness of this method by applying it to solve a high-order linear system of ODEs. Second, given a matrix generalized Nevanlinna function <span>\\(Q\\in N_{\\kappa }^{n \\times n}\\)</span>, that satisfies certain conditions at <span>\\(\\infty \\)</span>, and a canonical set of root functions of <span>\\(\\hat{Q}(z):= -Q(z)^{-1}\\)</span>, we construct the corresponding Pontryagin space <span>\\((\\mathcal {K}, [.,.])\\)</span>, a self-adjoint operator <span>\\(A:\\mathcal {K}\\rightarrow \\mathcal {K}\\)</span>, and an operator <span>\\(\\Gamma : \\mathbb {C}^{n}\\rightarrow \\mathcal {K}\\)</span>, that represent the function <i>Q</i>(<i>z</i>) in a Krein–Langer type representation. We illustrate the application of main results with examples involving concrete matrix polynomials <i>L</i>(<i>z</i>) and their inverses, defined as <span>\\(Q(z):=\\hat{L}(z):= -L(z)^{-1}\\)</span>.</p></div>","PeriodicalId":44371,"journal":{"name":"Advances in Operator Theory","volume":"10 2","pages":""},"PeriodicalIF":0.8000,"publicationDate":"2025-03-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1007/s43036-025-00432-2.pdf","citationCount":"0","resultStr":"{\"title\":\"An approach to root functions of matrix polynomials with applications in differential equations and meromorphic matrix functions\",\"authors\":\"Muhamed Borogovac\",\"doi\":\"10.1007/s43036-025-00432-2\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>First, we present a method for obtaining a canonical set of root functions and Jordan chains of the invertible matrix polynomial <i>L</i>(<i>z</i>) through elementary transformations of the matrix <i>L</i>(<i>z</i>) alone. This method provides a new and simple approach to deriving a general solution of the system of ordinary linear differential equations <span>\\\\(L\\\\left( \\\\frac{d}{dt}\\\\right) u=0\\\\)</span>, where <i>u</i>(<i>t</i>) is <i>n</i>-dimensional unknown function. We illustrate the effectiveness of this method by applying it to solve a high-order linear system of ODEs. Second, given a matrix generalized Nevanlinna function <span>\\\\(Q\\\\in N_{\\\\kappa }^{n \\\\times n}\\\\)</span>, that satisfies certain conditions at <span>\\\\(\\\\infty \\\\)</span>, and a canonical set of root functions of <span>\\\\(\\\\hat{Q}(z):= -Q(z)^{-1}\\\\)</span>, we construct the corresponding Pontryagin space <span>\\\\((\\\\mathcal {K}, [.,.])\\\\)</span>, a self-adjoint operator <span>\\\\(A:\\\\mathcal {K}\\\\rightarrow \\\\mathcal {K}\\\\)</span>, and an operator <span>\\\\(\\\\Gamma : \\\\mathbb {C}^{n}\\\\rightarrow \\\\mathcal {K}\\\\)</span>, that represent the function <i>Q</i>(<i>z</i>) in a Krein–Langer type representation. We illustrate the application of main results with examples involving concrete matrix polynomials <i>L</i>(<i>z</i>) and their inverses, defined as <span>\\\\(Q(z):=\\\\hat{L}(z):= -L(z)^{-1}\\\\)</span>.</p></div>\",\"PeriodicalId\":44371,\"journal\":{\"name\":\"Advances in Operator Theory\",\"volume\":\"10 2\",\"pages\":\"\"},\"PeriodicalIF\":0.8000,\"publicationDate\":\"2025-03-21\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://link.springer.com/content/pdf/10.1007/s43036-025-00432-2.pdf\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Advances in Operator Theory\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://link.springer.com/article/10.1007/s43036-025-00432-2\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"MATHEMATICS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Advances in Operator Theory","FirstCategoryId":"1085","ListUrlMain":"https://link.springer.com/article/10.1007/s43036-025-00432-2","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"MATHEMATICS","Score":null,"Total":0}
An approach to root functions of matrix polynomials with applications in differential equations and meromorphic matrix functions
First, we present a method for obtaining a canonical set of root functions and Jordan chains of the invertible matrix polynomial L(z) through elementary transformations of the matrix L(z) alone. This method provides a new and simple approach to deriving a general solution of the system of ordinary linear differential equations \(L\left( \frac{d}{dt}\right) u=0\), where u(t) is n-dimensional unknown function. We illustrate the effectiveness of this method by applying it to solve a high-order linear system of ODEs. Second, given a matrix generalized Nevanlinna function \(Q\in N_{\kappa }^{n \times n}\), that satisfies certain conditions at \(\infty \), and a canonical set of root functions of \(\hat{Q}(z):= -Q(z)^{-1}\), we construct the corresponding Pontryagin space \((\mathcal {K}, [.,.])\), a self-adjoint operator \(A:\mathcal {K}\rightarrow \mathcal {K}\), and an operator \(\Gamma : \mathbb {C}^{n}\rightarrow \mathcal {K}\), that represent the function Q(z) in a Krein–Langer type representation. We illustrate the application of main results with examples involving concrete matrix polynomials L(z) and their inverses, defined as \(Q(z):=\hat{L}(z):= -L(z)^{-1}\).