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2020
DOI: 10.1016/j.jfa.2020.108568
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Symmetry breaking operators for real reductive groups of rank one

Abstract: For a pair of real reductive groups G ′ ⊂ G we consider the space Hom G ′ (π| G ′ , τ ) of intertwining operators between spherical principal series representations π of G and τ of G ′ , also called symmetry breaking operators.

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Cited by 8 publications
(6 citation statements)
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“…Such operators are not only of interest when acting on functions but also when acting on sections of homogeneous vector bundles on spheres as well as in contexts where the conformal group of the sphere is replaced by other groups. We refer the interested reader to [KS15], [KS18], [KKP16], [FJS21], [FW20]. In the curved case, their definition uses a Poincaré-Einstein metric on X in the sense of Fefferman and Graham [FG12].…”
Section: Introductionmentioning
confidence: 99%
“…Such operators are not only of interest when acting on functions but also when acting on sections of homogeneous vector bundles on spheres as well as in contexts where the conformal group of the sphere is replaced by other groups. We refer the interested reader to [KS15], [KS18], [KKP16], [FJS21], [FW20]. In the curved case, their definition uses a Poincaré-Einstein metric on X in the sense of Fefferman and Graham [FG12].…”
Section: Introductionmentioning
confidence: 99%
“…In recent years, rapid progress in "Stage C" for the branching problems has been made in the construction and classification problems of symmetry breaking operators [23,36,81,97,99] in the "good framework" suggested by Theorem 6.7 or more strongly by Theorem 6.8. Some of them interact with parabolic geometry such as conformal geometry and also with the theory of automorphic forms.…”
Section: 1mentioning
confidence: 99%
“…F ↓ τ ρ j is called a symmetry breaking operator and F ↑ τ ρ j is called a holographic operator, according to the terminology introduced in [24,25] and [26] respectively. Such a problem is proposed by Kobayashi from the viewpoint of the representation theory (see [20]), and studied from various viewpoints by, e.g., [2,3,4,10,11,12,13,16,19,21,22,23,24,25,26,27,28,29,32,33,34,35,36,37,38,39] for holomorphic discrete series, principal series, and complementary series representations. Especially, it is proved by [19,24] that in the holomorphic setting, symmetry breaking operators F ↓ τ ρ j : O τ (D, V )| G 1 → O ρ j (D 1 , W j ) are always given by differential operators, that is, F ↓ τ ρ j are given by the form…”
Section: Introductionmentioning
confidence: 99%