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In mathematics, Aleksandrov–Clark (AC) measures are specially constructed measures named after the two mathematicians, A. B. Aleksandrov and Douglas Clark, who discovered some of their deepest properties. The measures are also called either Aleksandrov measures, Clark measures, or occasionally spectral measures. AC measures are used to extract information about self-maps of the unit disc, and have applications in a number of areas of complex analysis, most notably those related to operator theory. Systems of AC measures have also been constructed for higher dimensions, and for the half-plane. ==Construction of the measures== The original construction of Clark relates to one-dimensional perturbations of compressed shift operators on subspaces of the Hardy space: : By virtue of Beurling's theorem, any shift-invariant subspace of this space is of the form : where is an inner function. As such, any invariant subspace of the adjoint of the shift is of the form : We now define to be the shift operator compressed to , that is : Clark noticed that all the one-dimensional perturbations of , which were also unitary maps, were of the form : and related each such map to a measure, on the unit circle, via the Spectral theorem. This collection of measures, one for each on the unit circle , is then called the collection of AC measures associated with . 抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)』 ■ウィキペディアで「Aleksandrov–Clark measure」の詳細全文を読む スポンサード リンク
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