2021
DOI: 10.48550/arxiv.2108.13710
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Cross-Toeplitz Operators on the Fock--Segal--Bargmann Spaces and Two-Sided Convolutions on the Heisenberg Group

Abstract: We introduce an extended class of cross-Toeplitz operators which act between Fock-Segal-Bargmann spaces with different weights. It is natural to consider these operators in the framework of representation theory of the Heisenberg group. Our main technique is representation of cross-Toeplitz by two-sided relative convolutions from the Heisenberg group. In turn, two-sided convolutions are reduced to usual (one-sided) convolutions on the Heisenberg group of the doubled dimensionality. This allows us to utilise th… Show more

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Cited by 1 publication
(2 citation statements)
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“…We start from a brief account of groups involved in the consideration. An element of the one-dimensional Heisenberg group H [10,19,25] will be denoted by (s, x, y) ∈ R 3 . The group law on H is defined as follows:…”
Section: Heisenberg Sl 2 (R) Affine Schr öDinger and Ssr Groupsmentioning
confidence: 99%
See 1 more Smart Citation
“…We start from a brief account of groups involved in the consideration. An element of the one-dimensional Heisenberg group H [10,19,25] will be denoted by (s, x, y) ∈ R 3 . The group law on H is defined as follows:…”
Section: Heisenberg Sl 2 (R) Affine Schr öDinger and Ssr Groupsmentioning
confidence: 99%
“…We are also using the notation ≈ f := W φ f from [26] which now can be explained as the double covariant transform for the Heisenberg and the affine groups simultaneously. The image space L φ (R 4 + ) of the metamorphism is a subspace of square-integrable functions on L 2 (R 4 + , • µ ), see (25). Remark 5.3.…”
Section: Image Spaces Of the Covariant Transformsmentioning
confidence: 99%