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The compact picture of symmetry breaking operators for rank one orthogonal and unitary groups Jan Mllers (FAU Erlangen-Nrnberg) joint w/ Bent rsted 50th Seminar Sophus Lie, Bedlewo September 26, 2016 Jan Mllers Symmetry breaking


  1. The compact picture of symmetry breaking operators for rank one orthogonal and unitary groups Jan Möllers (FAU Erlangen-Nürnberg) joint w/ Bent Ørsted 50th Seminar Sophus Lie, Bedlewo September 26, 2016 Jan Möllers Symmetry breaking operators September 26, 2016 1 / 10

  2. Symmetry breaking operators Let G be a real reductive Lie group and G ′ ⊆ G a reductive subgroup. Jan Möllers Symmetry breaking operators September 26, 2016 2 / 10

  3. Symmetry breaking operators Let G be a real reductive Lie group and G ′ ⊆ G a reductive subgroup. Definition (Symmetry breaking operator) A symmetry breaking operator is a (continuous) intertwining operator from a representation π of G to a representation τ of G ′ , intertwining for the subgroup G ′ : Hom G ′ ( π | G ′ , τ ) . Jan Möllers Symmetry breaking operators September 26, 2016 2 / 10

  4. Symmetry breaking operators Let G be a real reductive Lie group and G ′ ⊆ G a reductive subgroup. Definition (Symmetry breaking operator) A symmetry breaking operator is a (continuous) intertwining operator from a representation π of G to a representation τ of G ′ , intertwining for the subgroup G ′ : Hom G ′ ( π | G ′ , τ ) . In the category of smooth admissible Fréchet representations of moderate growth: Jan Möllers Symmetry breaking operators September 26, 2016 2 / 10

  5. Symmetry breaking operators Let G be a real reductive Lie group and G ′ ⊆ G a reductive subgroup. Definition (Symmetry breaking operator) A symmetry breaking operator is a (continuous) intertwining operator from a representation π of G to a representation τ of G ′ , intertwining for the subgroup G ′ : Hom G ′ ( π | G ′ , τ ) . In the category of smooth admissible Fréchet representations of moderate growth: 1 (Kobayashi–Oshima 2013, Krötz–Schlichtkrull 2013) dim Hom G ′ ( π | G ′ , τ ) < ∞ for all irreducible π , τ if the homogeneous space ( G × G ′ ) / diag ( G ′ ) is real spherical. Jan Möllers Symmetry breaking operators September 26, 2016 2 / 10

  6. Symmetry breaking operators Let G be a real reductive Lie group and G ′ ⊆ G a reductive subgroup. Definition (Symmetry breaking operator) A symmetry breaking operator is a (continuous) intertwining operator from a representation π of G to a representation τ of G ′ , intertwining for the subgroup G ′ : Hom G ′ ( π | G ′ , τ ) . In the category of smooth admissible Fréchet representations of moderate growth: 1 (Kobayashi–Oshima 2013, Krötz–Schlichtkrull 2013) dim Hom G ′ ( π | G ′ , τ ) < ∞ for all irreducible π , τ if the homogeneous space ( G × G ′ ) / diag ( G ′ ) is real spherical. 2 (Sun–Zhu 2012) dim Hom G ′ ( π | G ′ , τ ) ≤ 1 for all irreducible π , τ if ( G , G ′ ) is one of the multiplicity-one pairs ( GL ( n , R ) , GL ( n − 1 , R )) , ( O ( p , q ) , O ( p , q − 1 )) , ( U ( p , q ) , U ( p , q − 1 )) , . . . Jan Möllers Symmetry breaking operators September 26, 2016 2 / 10

  7. Symmetry breaking operators Let G be a real reductive Lie group and G ′ ⊆ G a reductive subgroup. Definition (Symmetry breaking operator) A symmetry breaking operator is a (continuous) intertwining operator from a representation π of G to a representation τ of G ′ , intertwining for the subgroup G ′ : Hom G ′ ( π | G ′ , τ ) . In the category of smooth admissible Fréchet representations of moderate growth: 1 (Kobayashi–Oshima 2013, Krötz–Schlichtkrull 2013) dim Hom G ′ ( π | G ′ , τ ) < ∞ for all irreducible π , τ if the homogeneous space ( G × G ′ ) / diag ( G ′ ) is real spherical. 2 (Sun–Zhu 2012) dim Hom G ′ ( π | G ′ , τ ) ≤ 1 for all irreducible π , τ if ( G , G ′ ) is one of the multiplicity-one pairs ( GL ( n , R ) , GL ( n − 1 , R )) , ( O ( p , q ) , O ( p , q − 1 )) , ( U ( p , q ) , U ( p , q − 1 )) , . . . Question 2 , for which π, τ is the multiplicity = 1? In case If the multiplicity is = 1, construct explicitly a symmetry breaking operator π | G ′ → τ . Jan Möllers Symmetry breaking operators September 26, 2016 2 / 10

  8. Symmetry breaking operators Let G be a real reductive Lie group and G ′ ⊆ G a reductive subgroup. Definition (Symmetry breaking operator) A symmetry breaking operator is a (continuous) intertwining operator from a representation π of G to a representation τ of G ′ , intertwining for the subgroup G ′ : Hom G ′ ( π | G ′ , τ ) . In the category of smooth admissible Fréchet representations of moderate growth: 1 (Kobayashi–Oshima 2013, Krötz–Schlichtkrull 2013) dim Hom G ′ ( π | G ′ , τ ) < ∞ for all irreducible π , τ if the homogeneous space ( G × G ′ ) / diag ( G ′ ) is real spherical. 2 (Sun–Zhu 2012) dim Hom G ′ ( π | G ′ , τ ) ≤ 1 for all irreducible π , τ if ( G , G ′ ) is one of the multiplicity-one pairs ( GL ( n , R ) , GL ( n − 1 , R )) , ( O ( p , q ) , O ( p , q − 1 )) , ( U ( p , q ) , U ( p , q − 1 )) , . . . Question 2 , for which π, τ is the multiplicity = 1? In case If the multiplicity is = 1, construct explicitly a symmetry breaking operator π | G ′ → τ . Idea: Study this question algebraically � in a different category. Jan Möllers Symmetry breaking operators September 26, 2016 2 / 10

  9. Harish-Chandra modules Let G be a real reductive group, g its Lie algebra and K ⊆ G a maximal compact subgroup. Jan Möllers Symmetry breaking operators September 26, 2016 3 / 10

  10. Harish-Chandra modules Let G be a real reductive group, g its Lie algebra and K ⊆ G a maximal compact subgroup. Construction (Harish-Chandra module) To each smooth admissible representation ( π, V ) of G one can associate the Harish-Chandra module ( π HC , V HC ) of ( g , K ) on � V HC = { v ∈ V : dim span π ( K ) v < ∞} ≃ [ π | K : σ ] · σ ( K -finite vectors in V ). � �� � σ ∈ � K < ∞ Jan Möllers Symmetry breaking operators September 26, 2016 3 / 10

  11. Harish-Chandra modules Let G be a real reductive group, g its Lie algebra and K ⊆ G a maximal compact subgroup. Construction (Harish-Chandra module) To each smooth admissible representation ( π, V ) of G one can associate the Harish-Chandra module ( π HC , V HC ) of ( g , K ) on � V HC = { v ∈ V : dim span π ( K ) v < ∞} ≃ [ π | K : σ ] · σ ( K -finite vectors in V ). � �� � σ ∈ � K < ∞ Theorem (Casselman–Wallach) The functor π �→ π HC is an equivalence of categories: � � smooth admissible Fréchet representations → { Harish-Chandra modules } of moderate growth Jan Möllers Symmetry breaking operators September 26, 2016 3 / 10

  12. Harish-Chandra modules Let G be a real reductive group, g its Lie algebra and K ⊆ G a maximal compact subgroup. Construction (Harish-Chandra module) To each smooth admissible representation ( π, V ) of G one can associate the Harish-Chandra module ( π HC , V HC ) of ( g , K ) on � V HC = { v ∈ V : dim span π ( K ) v < ∞} ≃ [ π | K : σ ] · σ ( K -finite vectors in V ). � �� � σ ∈ � K < ∞ Theorem (Casselman–Wallach) The functor π �→ π HC is an equivalence of categories: � � smooth admissible Fréchet representations → { Harish-Chandra modules } of moderate growth Problem For a smooth admissible representation π of G the restriction π | G ′ is in general not admissible. � injective map: Hom G ′ ( π | G ′ , τ ) ֒ → Hom ( g ′ , K ′ ) ( π HC | ( g ′ , K ′ ) , τ HC ) . Jan Möllers Symmetry breaking operators September 26, 2016 3 / 10

  13. Harish-Chandra modules Let G be a real reductive group, g its Lie algebra and K ⊆ G a maximal compact subgroup. Construction (Harish-Chandra module) To each smooth admissible representation ( π, V ) of G one can associate the Harish-Chandra module ( π HC , V HC ) of ( g , K ) on � V HC = { v ∈ V : dim span π ( K ) v < ∞} ≃ [ π | K : σ ] · σ ( K -finite vectors in V ). � �� � σ ∈ � K < ∞ Theorem (Casselman–Wallach) The functor π �→ π HC is an equivalence of categories: � � smooth admissible Fréchet representations → { Harish-Chandra modules } of moderate growth Problem For a smooth admissible representation π of G the restriction π | G ′ is in general not admissible. � injective map: Hom G ′ ( π | G ′ , τ ) ֒ → Hom ( g ′ , K ′ ) ( π HC | ( g ′ , K ′ ) , τ HC ) . Remark: Surjectivity of this map is equivalent to the automatic continuity of invariant distribution vectors for the homogeneous space ( G × G ′ ) / diag ( G ′ ) . Jan Möllers Symmetry breaking operators September 26, 2016 3 / 10

  14. Degenerate principal series representations Question Construct and classify algebraic symmetry breaking operators in Hom ( g ′ , K ′ ) ( π HC | ( g ′ , K ′ ) , τ HC ) for irreducible Harish-Chandra modules π and τ of G and G ′ and multiplicity-one pairs ( G , G ′ ) . Jan Möllers Symmetry breaking operators September 26, 2016 4 / 10

  15. Degenerate principal series representations Question Construct and classify algebraic symmetry breaking operators in Hom ( g ′ , K ′ ) ( π HC | ( g ′ , K ′ ) , τ HC ) for irreducible Harish-Chandra modules π and τ of G and G ′ and multiplicity-one pairs ( G , G ′ ) . Casselman Embedding Theorem Every irreducible Harish-Chandra module occurs as a subrepresentation inside a (degenerate) principal series representation. Jan Möllers Symmetry breaking operators September 26, 2016 4 / 10

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