explicit computations of all finite index bimodules for a
play

Explicit computations of all finite index bimodules for a family of - PowerPoint PPT Presentation

Explicit computations of all finite index bimodules for a family of II 1 factors Fields Institute Workshop Von Neumann Algebras Stefaan Vaes 1/20 II 1 factor without finite index subfactors Trivial subfactor : 1 N M n ( C ) N . Take


  1. Explicit computations of all finite index bimodules for a family of II 1 factors Fields Institute Workshop Von Neumann Algebras Stefaan Vaes 1/20

  2. II 1 factor without finite index subfactors Trivial subfactor : 1 ⊗ N ⊂ M n ( C ) ⊗ N . Take Γ = SL ( 2 , Q ) ⋉ Q 2 , with Γ ↷ ( X , µ) = ( X 0 , µ 0 ) Q 2 . Theorem (V, 2007) The II 1 factor M = L ∞ ( X ) ⋊ Ω α Γ has no non-trivial finite index subfactors if ◮ ( X 0 , µ 0 ) atomic with atoms of different weights, ◮ α ∈ R \ { 0 } and Ω α ∈ Z 2 ( Γ , S 1 ) defined by �� x 1 �� � � y 1 = exp ( 2 π i α( x 1 y 2 − x 2 y 1 )) Ω α , x 2 y 2 on Q 2 and extended to Γ by SL ( 2 , Q ) -invariance. Moreover, the II 1 factor M remembers ( X 0 , µ 0 ) and α . 2/20

  3. Other results and plan of talk ◮ Introduce finite index bimodules and fusion algebra of II 1 factors. ◮ Present the first explicit computations of fusion algebras of II 1 factors : • Identification with Hecke algebras. • Crucial ingredients : Popa’s deformation/rigidity and cocycle superrigidity. ◮ Theorem (V, 2007, generalizing Popa – V, 2006). Every countable group arises as the outer automorphism group of a II 1 factor. 3/20

  4. Connes’ correspondences A representation theory of II 1 factors Let M be a type II 1 factor with trace τ . ◮ A right M -module is a Hilbert space with a right action of M . Example : L 2 ( M , τ) M . � i ∈ I p i L 2 ( M ) ◮ Always, H M ≅ � and one defines dim ( H M ) = i τ( p i ) ∈ [ 0 , +∞ ] . Complete invariant of right M -modules. Definition An M - M -bimodule of finite Jones index, is an M - M -bimodule M H M dim ( H M ) < ∞ dim ( M H ) < ∞ . satisfying and Denote FAlg ( M ) the set of (equiv. classes) of finite index bimodules. 4/20

  5. The structure of the fusion algebra FAlg( M ) Example : let α ∈ Aut ( M ) and define the M - M -bimodule H (α) on L 2 ( M ) by a · ξ · b = a ξα( b ) Precisely those M H M with dim ( M H ) = 1 = dim ( H M ) . Example : let M ⊂ M 1 be a finite index subfactor. Then, M L 2 ( M 1 ) M belongs to FAlg ( M ) . In general, FAlg( M ) carries the following structure. ◮ Direct sum of bimodules. ◮ Identity element : M L 2 ( M ) M . ◮ Connes’ tensor product H ⊗ M K . Example : H (α) ⊗ M H (β) ≅ H (α ◦ β) . ◮ Contragredient M H M of M H M . FAlg ( M ) consists of the generalized symmetries of M . 5/20

  6. Group-like elements in FAlg( M ) We call M H M group-like if H ⊗ M H is the identity. Example of group-like element M H M : ◮ H = L 2 ( M ) p . ◮ α : M → pMp an isomorphism. ◮ a · ξ · b = a ξα( b ) . Set Out ( M ) = Aut ( M ) Inn ( M ) . Observation We have a short exact sequence e → Out ( M ) → { group-like bimodules } → F ( M ) → e where F ( M ) is the fundamental group of M . 6/20

  7. Abstract fusion algebras Definition A fusion algebra A is a free N -module N [ G ] , equipped with � ◮ an associat. distribut. product : x ∗ y = mult ( z , x ∗ y ) z , z ∈G ◮ a multiplicative neutral element e ∈ G , ◮ a contragredient map x ֏ x which is ..., such that Frobenius reciprocity holds : for all x , y , z ∈ G , we have mult ( z , x ∗ y ) = mult ( x , z ∗ y ) = mult ( y , x ∗ z ) Examples ◮ N [ Γ ] for a group Γ . ◮ Rep ( G ) , the finite dim. unitary rep. of a compact group G . ◮ FAlg ( M ) of a II 1 factor M . 7/20

  8. Fusion algebra of a Hecke pair [ Γ : g Γ g − 1 ∩ Γ ] < ∞ for all g ∈ G . Let Γ < G be a Hecke pair, i.e. Hecke fusion algebra H ( Γ < G ) = { ξ : Γ \ G / Γ → N | ξ has finite support } � ξ( h ) η( h − 1 g ) (ξ ∗ η)( g ) = h ∈ G / Γ Γ \ G / Γ is the set of irreducibles with fusion rules ... Example Let T be k -valent tree and G < Aut ( T ) countable dense subgroup. Choose a vertex e and set Γ = Stab e . Identify Γ \ G / Γ = Γ \ T ≅ N via the distance to e . Then, mult ( n , a ∗ b ) = # { t ∈ T | | et | = a , | ts | = b } when | es | = n . A way to understand the Hecke fusion algebra of PSL ( 2 , Z ) < PSL ( 2 , Q ) . 8/20

  9. Computations of FAlg( M ) Data : action of Γ on a countable set I , base probability space ( X 0 , µ 0 ) . Action : Γ ↷ ( X , µ) = ( X 0 , µ 0 ) I . II 1 factor : M = L ∞ ( X ) ⋊ Γ . Theorem (V, 2007) Under the right conditions on Γ ↷ I and for ( X 0 , µ 0 ) atomic with distinct weights, we have � → � → H ( Γ < G ) Rep fin ( Γ ) FAlg ( M ) where G = Comm Perm I ( Γ ) = commensurator of Γ inside Perm I . For every Hecke pair Γ < G , one defines H rep ( Γ < G ) . Then, FAlg ( M ) ≅ H rep ( Γ < G ) . 9/20

  10. Concrete examples Recall : M = L ∞ ( X ) ⋊ Γ Γ ↷ ( X , µ) = ( X 0 , µ 0 ) I . and FAlg ( M ) Γ ↷ I SL n ( Z ) ⋉ Q n Q n for n ≥ 2. H rep ( SL n ( Z ) < GL n ( Q )) ↷ H rep ( Λ < Comm PGL n ( Q ) ( Λ )) . Λ < PSL n ( Q ) proper subgroup, relative ICC, Γ = Λ × PSL n ( Q ) ↷ PSL n ( Q ) by left-right action. H rep ( R ∗ ⋉ R < Q ∗ ⋉ Q ) Z < R < Q strict inclusions of rings, i.e. R = Z [ P − 1 ] Relation with Bost- Write some Λ 0 < Λ = SL 2 ( Q )⋉ Q 2 . Connes Hecke algebra. Take Λ 0 × Λ ↷ Λ . Add 2-cocycle. SL 2 ( Q ) ⋉ Q 2 ↷ Q 2 Trivial. Add 2-cocycle. 10/20

  11. M = L ∞ ( X ) ⋊ Γ Γ ↷ ( X , µ) = ( X 0 , µ 0 ) I . We continue with and FAlg ( M ) ≅ H rep ( Γ < Comm Perm I ( Γ )) Our isomorphism works for Good actions of good groups A condition on the group Γ : ◮ Γ admits an infinite, almost normal subgroup with relative (T). Some conditions on the action Γ ↷ I : ◮ Transitivity. ◮ Stab i 0 acts with infinite orbits on I − { i 0 } . ◮ Minimal condition on stabilizers : no infinite sequence ( i n ) with Stab ( i 0 , . . . , i n ) strictly decreasing. ◮ A faithfulness condition of Γ → Perm I . About the minimal condition on stabilizers. Automatic if Γ ↷ I embeds in GL ( V ) ⋉ V ↷ V for fin.dim. V . For left-right action Λ × Λ ↷ Λ : equivalent with minimal condition on centralizers of Λ . 11/20

  12. How to find all finite index M - M - bimodules Take Γ ↷ I a good action of a good group. M = L ∞ ( X ) ⋊ Γ Γ ↷ ( X , µ) = ( X 0 , µ 0 ) I . Let and Take a finite index M - M -bimodule M H M . 1 The bimodule H contains a finite index L ( Γ ) - L ( Γ ) -subbimodule. Main ingredients : Popa’s deformation/rigidity and the minimal condition on stabilizers. 2 The bimodule H contains a finite index L ∞ ( X ) - L ∞ ( X ) -subbimodule. 3 The bimodule H belongs to H rep ( Γ < Comm Aut ( X ,µ) ( Γ )) Main ingredient : Popa’s cocycle superrigidity. 4 Identification of Comm Aut ( X ,µ) ( Γ ) and Comm Perm I ( Γ ) Main ingredient : Stab i 0 acts with infinite orbits on I − { i 0 } . Attention : two difficult slides follow with steps 1 and 2. 12/20

  13. Every bimodule is L ( Γ ) -preserving (Step 1) M = L ∞ ( X ) ⋊ Γ Γ ↷ ( X , µ) = ( X 0 , µ 0 ) I . Let and Take a finite index M - M -bimodule M H M . Simplifying assumptions : H = H (ψ) for ψ ∈ Aut ( M ) and Γ has property (T). Aim : ψ( L ( Γ )) and L ( Γ ) are unitarily conjugate. ◮ Popa’s malleability (roughly) : • flow (α t ) t ∈ R on L ∞ ( X × X ) , • commuting with diagonal Γ -action, • connecting id = α 0 with flip = α 1 . ◮ Extend α t to L ∞ ( X × X ) ⋊ Γ . Set P = ψ( L ( Γ )) ⊂ ( L ∞ ( X ) ⊗ 1 ) ⋊ Γ . By property (T), α 0 ( P ) and α 1 ( P ) are unitarily conjugate. Then, ψ( L ( Γ )) and L ( Γ ) are unitarily conjugate. ◮ Popa proves this for Γ ↷ ( X , µ) mixing (meaning here that Stab i is finite for all i ∈ I ) Mixing is replaced by minimal condition on stabilizers. 13/20

  14. Every L ( Γ ) -preserving bimodule is Cartan-preserving (Step 2) M = L ∞ ( X ) ⋊ Γ Γ ↷ ( X , µ) = ( X 0 , µ 0 ) I . Let and Take a finite index M - M -bimodule M H M . Simplifying assumptions : H = H (ψ) for ψ ∈ Aut ( M ) and ψ( L ( Γ )) = L ( Γ ) (because of Step 1). Aim : ψ( L ∞ ( X )) and L ∞ ( X ) are unitarily conjugate. ◮ Fix i 0 ∈ I and set Γ 0 = Stab i 0 . Recall : Stab i 0 acts with infinite orbits on I − { i 0 } . First aim : ψ( L ( Γ 0 )) and L ( Γ 0 ) are unitarily conjugate. ◮ If not, ψ( L ( Γ 0 )) will be far from L ( Γ 0 ) leading to ψ( L ( Γ 0 )) ′ ∩ M ⊂ L ( Γ ) . Contradiction. ◮ So, we may assume ψ( L ( Γ 0 )) = L ( Γ 0 ) . Take relative commutants : � L ∞ � ( X 0 , µ 0 ) { i 0 } � � = L ∞ � ( X 0 , µ 0 ) { i 0 } � ψ ⋊ Γ 0 ⋊ Γ 0 . ◮ Play a game to get ψ( L ∞ ( X )) and L ∞ ( X ) conjugate. 14/20

  15. Cartan preserving bimodules and cocycle superrigidity M = L ∞ ( X ) ⋊ Γ Γ ↷ ( X , µ) = ( X 0 , µ 0 ) I . Let and Take a finite index M - M -bimodule M H M . Simplifying assumptions : H = H (ψ) for ψ ∈ Aut ( M ) and ψ( L ∞ ( X )) = L ∞ ( X ) (because of Step 2). Restriction of ψ to L ∞ ( X ) yields an orbit equivalence ∆ : X → X : ∆ ( Γ · x ) = Γ · ∆ ( x ) a.e. Associated Zimmer 1-cocycle : ∆ ( g · x ) = ω( g , x ) · ∆ ( x ) . Cocycle superrigidity theorem (Popa, 2005) Let Γ ↷ ( X , µ) = ( X 0 , µ 0 ) I . Assume ◮ H < Γ almost normal and relative (T), ◮ H acts with infinite orbits on I , ◮ G either a countable or a compact group. Every 1-cocycle for Γ ↷ ( X , µ) with values in G , is cohomologous with a homomorphism Γ → G . 15/20

Download Presentation
Download Policy: The content available on the website is offered to you 'AS IS' for your personal information and use only. It cannot be commercialized, licensed, or distributed on other websites without prior consent from the author. To download a presentation, simply click this link. If you encounter any difficulties during the download process, it's possible that the publisher has removed the file from their server.

Recommend


More recommend