saturated fusion systems as stable retracts of groups
play

Saturated fusion systems as stable retracts of groups Sune Precht - PowerPoint PPT Presentation

m i t m a t h e m a t i c s Massachusetts Institute of Technology Department of Mathematics Saturated fusion systems as stable retracts of groups Sune Precht Reeh MIT Topology Seminar, September 28, 2015 Slide 1/24 m i t m a t h e m a t i c


  1. m i t m a t h e m a t i c s Massachusetts Institute of Technology Department of Mathematics Saturated fusion systems as stable retracts of groups Sune Precht Reeh MIT Topology Seminar, September 28, 2015 Slide 1/24

  2. m i t m a t h e m a t i c s Outline 1 Bisets as stable maps 2 Fusion systems and idempotents 3 An application to HKR character theory (with T. Schlank & N. Stapleton) Notes on the blackboard are in red . Slide 2/24

  3. m i t m a t h e m a t i c s Bisets Let S, T be finite p -groups. An ( S, T )-biset is a finite set equipped with a left action of S and a free right action of T , such that the actions commute. Transitive bisets: [ Q, ψ ] T S := S × T/ ( sq, t ) ∼ ( s, ψ ( q ) t ) for Q ≤ S and ψ : Q → T . Q and ψ are determined up to preconjugation in S and postconjugation in T . ( S, T )-bisets form an abelian monoid with disjoint union. The group completion is the Burnside biset module A ( S, T ), consisting of “virtual bisets” , i.e. formal differences of bisets. The [ Q, ψ ] form a Z -basis for A ( S, T ) . Example for D 8 with subgroup diagram. With V 1 as one of the Klein four groups, Q 1 as a reflection contained in V 1 , and Slide 3/24

  4. m i t m a t h e m a t i c s Bisets 2 Z as the centre/half-rotation of D 8 , we for example have [ V 1 , id ] − 2[ Q 1 , Q 1 → Z ] as an element of A ( D 8 , D 8 ) . We can compose bisets ⊙ : A ( R, S ) × A ( S, T ) → A ( R, T ) given by X ⊙ Y := X × S Y when X, Y are actual bisets. A ( S, S ) is the double Burnside ring of S . A special case of the composition formula: [ Q, ψ ] T S ⊙ [ T, ϕ ] R T = [ Q, ϕψ ] R S . We can think of ( S, T ) -bisets as being a sort of morphism from S to T . Slide 4/24

  5. m i t m a t h e m a t i c s Bisets as stable maps Theorem (Segal conjecture. Carlsson, . . . ) For p -groups S, T : p ∼ [Σ ∞ + BS, Σ ∞ + BT ] ≈ A ( S, T ) ∧ = { X ∈ A ( S, T ) ∧ p | | X | / | T | ∈ Z } . Corollary (?) For p -groups S, T : p ] ∼ [(Σ ∞ + BS ) ∧ p , (Σ ∞ + BT ) ∧ = A ( S, T ) ∧ p . Slide 5/24

  6. m i t m a t h e m a t i c s Fusion systems A fusion system over a finite p -group S is a category F where the objects are the subgroups P ≤ S and the morphisms satisfy: • Hom S ( P, Q ) ⊆ F ( P, Q ) ⊆ Inj( P, Q ) for all P, Q ≤ S . • Every ϕ ∈ F ( P, Q ) factors in F as an isomorphism P → ϕP followed by an inclusion ϕP ֒ → Q . A saturated fusion system satisfies a few additional axioms that play the role of Sylow’s theorems. The canonical example of a saturated fusion system is F S ( G ) defined for S ∈ Syl p ( G ) with morphisms Hom F S ( G ) ( P, Q ) := Hom G ( P, Q ) . for P, Q ≤ S . Slide 6/24

  7. m i t m a t h e m a t i c s Fusion systems 2 Example for D 8 ≤ Σ 4 : If V 1 consists of the double transpositions in Σ 4 , then the fusion system F = F D 8 (Σ 4 ) gains an automorphism α of V 1 of order 3, and Q 1 ≤ V 1 becomes conjugate in F to Z ≤ V 1 . Slide 7/24

  8. m i t m a t h e m a t i c s Characteristic bisets If G induces a fusion system on S , we can ask what properties G has as an ( S, S )-biset in relation to F S ( G ). Linckelmann-Webb wrote down the essential properties as the following definition: An element Ω ∈ A ( S, S ) ∧ p is said to be F -characteristic if • Ω is left F -stable: res ϕ Ω = res P Ω in A ( P, S ) ∧ p for all P ≤ S and ϕ ∈ F ( P, S ). • Ω is right F -stable. • Ω is a linear combination of transitive bisets [ Q, ψ ] S S with ψ ∈ F ( Q, S ). • | Ω | / | S | is invertible in Z ( p ) . Slide 8/24

  9. m i t m a t h e m a t i c s Characteristic bisets 2 G , as an ( S, S )-biset, is F S ( G )-characteristic. Σ 4 as a ( D 8 , D 8 ) -biset is isomorphic to Σ 4 ∼ = [ D 8 , id ] + [ V 1 , α ] . This biset is F D 8 (Σ 4 ) -characteristic. On the other hand, the previous example [ V 1 , id ] − 2[ Q 1 , Q 1 → Z ] is generated by elements [ Q, ψ ] with ψ ∈ F , but it is not F -stable and hence not characteristic. We prefer a characteristic element that is idempotent in A ( S, S ) ∧ p . Slide 9/24

  10. m i t m a t h e m a t i c s Characteristic bisets 3 Theorem (Ragnarsson-Stancu) Every saturated fusion system F over S has a unique F -characteristic idempotent ω F ∈ A ( S, S ) ( p ) ⊆ A ( S, S ) ∧ p , and ω F determines F . For the fusion system F = F D 8 (Σ 4 ) , the characteristic idempotent takes the form ω F = [ D 8 , id ] + 1 3 [ V 1 , α ] − 1 3 [ V 1 , id ] . Slide 10/24

  11. m i t m a t h e m a t i c s B F as a stable retract of BS The characteristic idempotent ω F ∈ A ( S, S ) ∧ p for a saturated fusion system F defines an idempotent selfmap ω F Σ ∞ → Σ ∞ + BS − − + BS. This splits off a direct summand W of Σ ∞ + BS , with properties: • If F = F S ( G ), then W ≃ Σ ∞ + ( BG ∧ p ). • Each F has a “classifying space” B F , and W ≃ Σ ∞ + B F . We have B F ≃ BG ∧ p when F = F S ( G ) . • Have maps i : Σ ∞ + BS → Σ ∞ + B F and tr: Σ ∞ + B F → Σ ∞ + BS s.t. i ◦ tr = id Σ ∞ + B F and tr ◦ i = ω F . Slide 11/24

  12. m i t m a t h e m a t i c s B F as a stable retract of BS Each saturated fusion system F over a p -group S corresponds to the retract Σ ∞ + B F of Σ ∞ + BS . Strategy • Consider known results for finite p -groups. • Apply ω F everywhere. • Get theorems for saturated fusion systems, and p -completed classifying spaces. Slide 12/24

  13. m i t m a t h e m a t i c s HKR character theory Hopkins-Kuhn-Ravenel constructed a generalization of group characters in Morava E-theory: χ n : E ∗ n ( BG ) → Cl n,p ( G ; L ( E ∗ n )) . L ( E ∗ n ) is a certain algebra over E ∗ n . Cl n,p ( G ; L ( E ∗ n )) contains functions valued in L ( E ∗ n ) defined on G-conjugacy classes of n -tuples of commuting elements in G of p -power order. Theorem (Hopkins-Kuhn-Ravenel) n ( BG ) ≃ L ( E ∗ n E ∗ → Cl n,p ( G ; L ( E ∗ n ) ⊗ E ∗ − n )) . Slide 13/24

  14. m i t m a t h e m a t i c s A further generalization by Stapleton gives character maps n (Λ n − t E ∗ n L K ( t ) E ∗ n ( BG ) → C t ⊗ L K ( t ) E 0 BG ) . p C t is of chromatic height t and an algebra over L K ( t ) E 0 n (and E 0 n ). The r -fold free loop space Λ r BG decomposes as a disjoint union of centralizers: Λ r BG ≃ � C G ( α ) . α commuting r -tuple in G up to G -conj Λ r p BG is the collection of components for commuting r -tuples of elements of p -power order. Slide 14/24

  15. m i t m a t h e m a t i c s Theorem (Stapleton) n ( BG ) ≃ n (Λ n − t n E ∗ n L K ( t ) E ∗ C t ⊗ E 0 − → C t ⊗ L K ( t ) E 0 BG ) . p The case t = 0 is the HKR character map. Slide 15/24

  16. m i t m a t h e m a t i c s HKR character theory for fusion systems joint with Tomer Schlank & Nat Stapleton We consider the character map for p -groups n (Λ n − t BS ) E ∗ n L K ( t ) E ∗ n ( BS ) → C t ⊗ L K ( t ) E 0 and try to make ω F act on both sides in a way that commutes with the character map. If successful, we get: Conjecture/Pretheorem (R.-Schlank-Stapleton) For every saturated fusion system F we have n ( B F ) ≃ n (Λ n − t B F ) . n E ∗ n L K ( t ) E ∗ C t ⊗ E 0 − → C t ⊗ L K ( t ) E 0 For F = F S ( G ) this recovers the theorem for finite groups. Slide 16/24

  17. m i t m a t h e m a t i c s The proof Let Λ := Z /p k for k ≫ 0. Think of Λ as emulating S 1 . The character map can be decomposed as n ( BS ) ev ∗ n ( B Λ n − t × Λ n − t BS ) E ∗ → E ∗ − − ≃ E ∗ n ( B Λ n − t ) ⊗ E ∗ n E ∗ n (Λ n − t BS ) n (Λ n − t BS ) n E ∗ → C t ⊗ E 0 n (Λ n − t BS ) n L K ( t ) E ∗ → C t ⊗ L K ( t ) E 0 The first map is induced by the evaluation map ev : B Λ n − t × Λ n − t BS → BS . Slide 17/24

  18. m i t m a t h e m a t i c s The proof 2 With the decomposition Λ r BS ≃ � BC S ( a ) , Commuting r -tuples a in S up to S -conjugation the evaluation map can be described algebraically as ( Z /p k ) r × C S ( a ) → S given by ( t 1 , . . . , t r , s ) �→ ( a 1 ) t 1 · · · ( a r ) t r · z. Slide 18/24

  19. m i t m a t h e m a t i c s Consider functoriality of the evalutation map ev ev B Λ r × Λ r BS BS f ? ev B Λ r × Λ r BT BT If f is a map BS → BT of spaces, then we can just plug in id × Λ r ( f ) into the square. However, if f is a stable map, such as ω F , we can’t apply Λ r ( − ) to f . Slide 19/24

  20. m i t m a t h e m a t i c s Pretheorem (R.-S.-S.) There is a functor M defined on suspension spectra of p -groups and saturated fusion systems, such that for each stable map f : Σ ∞ BS → Σ ∞ BT the following square commutes: ev B Λ r × Λ r BS BS M ( f ) f ev B Λ r × Λ r BT BT : Stable maps Note: M ( f ) maps between coproducts of p -groups and fusion systems, so M ( f ) is a matrix of virtual bisets. Slide 20/24

  21. m i t m a t h e m a t i c s For most stable maps f , it is impossible for M ( f ) to have the form id ( Z /p k ) r × (?) . Hence the cyclic factor needs to be used nontrivially. The free loop space Λ r B F for a saturated fusion system, also decomposed as a disjoint union of centralizers: Proposition (Broto-Levi-Oliver) Λ r B F ≃ � BC F ( a ) Commuting r -tuples a in S up to F -conjugation If AF p is the category of formal coproducts of p-groups and fusion systems, where maps a matrices of virtual bisets, then M is a functor from AF p to itself. Slide 21/24

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