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Weyl type theorems for bounded linear operators on Banach spaces

机译:Banach空间上有界线性运营商的Weyl型定理

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In 1909 H. Weyl [59] studied the spectra of all compact linear perturbations of a self-adjoint operator defined on a Hubert space and found that their intersection consisted precisely of those points of the spectrum which are not isolated eigenvalues of finite multiplicity. Later, the property established by Weyl for self-adjoint operators has been observed for several other classes of operators, for instance hyponormal operators on Hilbert spaces, Toeplitz operators [33], convolution operators on group algebras [19], and many other classes of operators defined on Banach spaces ([52]). In the literature, a bounded linear operator defined on a Banach space which satisfies this property is said to satisfy Weyl's theorem. Weaker variants of Weyl's theorem have been discussed by Harte and Lee [44], while two approximate-point spectrum versions of Weyl's theorem have been introduced by Rakocevic [54], a-Weyl's theorem ([55], [2]), and the so-called property (w) ([54], [17]). In this course we describe all Weyl type theorems, together with some their generalized versions ([25], [27]) and we show the equivalences of these theorems for classes of operators which satisfy certain "polaroid" conditions on the isolated points of the spectrum ([5], or on the isolated points of the approximate point spectrum. Our main tool is an important property, the so-called single valued extension property (SVEP), introduced by Dunford [41], [42]. The SVEP plays an important role in local spectral theory, see the monograph of Laursen and Neumann [50], and a localized version of SVEP has deep connections with Fredholm theory, see the monograph [1]. In the last part of the course we study the permanence of Weyl type theorems under a quasi-affinity, or more in general, the permanence of Weyl type theorems from an operator T ? L(X) to an operator S ? L(Y), X and Y Banach spaces, in the case that T and S are intertwined asymptotically by an operator A G L(X,Y).
机译:1909年H. Weyl [59]研究了在Hubert Space上定义的自伴随操作员的所有紧凑线性扰动的光谱,发现它们的交点精确地组成的频谱的那些点,这些点不是有限多重的偏见的谱的那些点。后来,对于迄今为止的诸如希尔伯特空间,Toeplitz运算符[33]的卷积运营商[19],已经观察到由其他类别的运营商而建立的韦尔韦尔(Weyl)用于自伴运营商的财产,例如,在Hilbert Spaces上,卷积运营商[19],以及许多其他课程在Banach空间上定义的操作员([52])。在文献中,据说,在满足该属性的Banach空间上定义的有界线性的连续操作员可以满足Weyl的定理。 Harte和Lee讨论了Weyl的定理的较弱变体[44],而Rakocevic [54],A-Weyl的定理([55],[2]),和所谓的财产(W)([54],[17])。在本课程中,我们描述了所有Weyl型定理,以及他们的广义版本([25],[27]),我们向众多“偏振片”条件的孤立点上的某些“偏振片”条件的课程课程的课程定理的等效性频谱([5],或近似点频谱的孤立点。我们的主要工具是Dunford引入的所谓单值的延长物业(SVEP),[41],[42]。SVEP在当地光谱理论中发挥着重要作用,看看Laursen和Neumann [50]的专着,SVEP的局部版本与Fredholm理论有深入的连接,看专着[1]。在我们研究的课程的最后一部分在准亲和力下的Weyl型定理的持久性,或者一般来说,从操作员TΔl(x)到操作员s?l(y),x和y banach空间的veyl型定理的持续时间T和S由操作员AGL(X,Y)渐近地交织在一起。

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