School of Mathematical & Statistical Sciences Faculty Publications

Document Type

Article

Publication Date

10-2026

Abstract

In quantum theory the quantum expectation region of an observable describes the set of attainable measurement statistics over all pure states. We study how these regions and their maximal expectation values evolve under Aluthge-type quantum channels acting on bounded operators and commuting pairs of operators. These quantum channels generate nonlinear operator flows that regularize non-normal operators while preserving essential measurement information. These results provide a geometric setting for understanding the stability of measurement statistics of compatible quantum operators under structured quantum channels. For a commuting pair๐“=(๐‘‡1,๐‘‡2), we analyze the associated linear pencil ย  ๐ฟโข๐‘โก(๐“)={๐‘‡1+๐œ†โข๐‘‡2:๐œ†โˆˆโ„‚}, ย  which admits both generalized and spherical Aluthge quantum channels. We characterize when these quantum channels coincide in terms of the abelian๐ถโˆ—-algebra generated by the corresponding positive operator and interpret this situation as a fixed-point configuration of the induced quantum channels. As a special case, the mean quantum channel yields characterizations of quasinormal operators via matricial quasinormality and stability of quantum expectation regions. Under a convexity stability assumption, we show that the limit of joint quantum expectation regions of iterated spherical Aluthge quantum channels coincides with the convex hull of the Taylor spectrum. We further determine the Taylor spectrum for a pair of the form๐“=(๐‘†,๐›ฅ1โก(๐‘†))ย under the Bรฉzout identity and establish a mapping theorem for quantum expectation regions of linear pencils together with inequalities relating joint and pencil maximal expectation values.

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Original published version available atย https://doi.org/10.1016/j.aop.2026.170624

Publication Title

Annals of Physics

DOI

10.1016/j.aop.2026.170624

Available for download on Sunday, July 09, 2028

Included in

Mathematics Commons

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