Infinite matrices and their finite sections : an introduction to the limit operator method

In this book we are concerned with the study of a certain class of in?nite matrices and two important properties of them: their Fredholmness and the stability of the approximation by their ?nite truncations. Let us take these two properties as a starting point for the big picture that shall be prese...

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Detalles Bibliográficos
Autor Principal: Lindner, Marko, 1973-
Formato: Livre numérique
Idioma:Anglais
Publicado: Basel : Birkhäuser Basel 2006.
Cham : Springer Nature
Series:Frontiers in Mathematics
Sujets:
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Nota: Archives Springer e-books (Licence nationale)
Archives Springer e-books (Licence nationale)
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Edition sous un autre format:• Infinite Matrices and their Finite Sections, Texte imprimé, 9783764391539
• Infinite Matrices and their Finite Sections, Texte imprimé, 9783764377663
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245 1 0 |a Infinite matrices and their finite sections :  |b an introduction to the limit operator method   |c by Marko Lindner. 
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505 0 |a Preliminaries -- Invertibility at Infinity -- Limit Operators -- Stability of the Finite Section Method. 
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520 |a In this book we are concerned with the study of a certain class of in?nite matrices and two important properties of them: their Fredholmness and the stability of the approximation by their ?nite truncations. Let us take these two properties as a starting point for the big picture that shall be presented in what follows. Stability Fredholmness We think of our in?nite matrices as bounded linear operators on a Banach space E of two-sided in?nite sequences. Probably the simplest case to start with 2 +? is the space E = of all complex-valued sequences u=(u ) for which m m=?? 2 /u / is summable over m? Z. m Theclassofoperatorsweareinterestedinconsistsofthoseboundedandlinear operatorsonE whichcanbeapproximatedintheoperatornormbybandmatrices. We refer to them as band-dominated operators. Of course, these considerations 2 are not limited to the space E = . We will widen the selection of the underlying space E in three directions: p We pass to the classical sequence spaces with 1? p??. n Our elements u=(u )? E have indices m? Z rather than just m? Z. m We allow values u in an arbitrary ?xed Banach spaceX rather than C. 
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