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Crawford numbers of powers of a matrix

dc.citation.epage2254en_US
dc.citation.issue11-12en_US
dc.citation.spage2243en_US
dc.citation.volume433en_US
dc.citation.woscount0
dc.contributor.authorWang, Kuo-Zhongen_US
dc.contributor.authorWu, Pei Yuanen_US
dc.contributor.authorGau, Hwa-Longen_US
dc.contributor.department應用數學系zh_TW
dc.contributor.departmentDepartment of Applied Mathematicsen_US
dc.date.accessioned2014-12-08T15:38:13Z
dc.date.available2014-12-08T15:38:13Z
dc.date.issued2010-12-30en_US
dc.description.abstractFor an n-by-n matrix A, its Crawford number c(A) (resp., generalized Crawford number C(A)) is, by definition, the distance from the origin to its numerical range W(A) (resp., the boundary of its numerical range partial derivative W(A)). It is shown that if A has eigenvalues lambda(1), ..., lambda(n) An arranged so that vertical bar lambda(1)vertical bar >= ... >= vertical bar lambda(n)vertical bar, then (lim) over bar (k) c(A(k))(1/k) (resp., (lim) over bar (k) C(A(k))(1/k))equals 0 or vertical bar lambda(n)vertical bar (resp., vertical bar lambda(j)vertical bar for some j, 1 <= j <= n). For a normal A. more can be said, namely, (lim) over bar (k) c(A(k))(1/k) = vertical bar lambda(n)vertical bar (resp., (lim) over bar (k) C(A(k))(1/k) = vertical bar lambda(j)vertical bar for some j, 3 <= j <= n). In these cases, the above possible values can all be assumed by some A. (C) 2010 Elsevier Inc. All rights reserved.en_US
dc.identifier.doi10.1016/j.laa.2010.08.004en_US
dc.identifier.issn0024-3795en_US
dc.identifier.journalLINEAR ALGEBRA AND ITS APPLICATIONSen_US
dc.identifier.urihttp://dx.doi.org/10.1016/j.laa.2010.08.004en_US
dc.identifier.urihttps://ir.lib.nycu.edu.tw/handle/11536/26204
dc.identifier.wosnumberWOS:000283893700040
dc.language.isoen_USen_US
dc.subjectNumerical rangeen_US
dc.subjectCrawford numberen_US
dc.subjectGeneralized Crawford numberen_US
dc.titleCrawford numbers of powers of a matrixen_US
dc.typeArticleen_US

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