Critical level representations of affine Kac Moody algebras

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Critical level representations of affine Kac Moody algebras Peter Fiebig Emmy Noether Zentrum Universität Erlangen Nürnberg Isle of Skye May 2010

Affine Kac Moody algebras Let g be a complex simple Lie algebra of finite dimension. We define g = g C C[t, t 1 ], the loop algebra, ĝ = g CK CD the affine Kac Moody algebra. The bracket is given by [K, ] = 0 [D, x t n ] = nx t n [x t n, y t m ] = [x, y] t m+n + nδ m, n κ(x, y)k, where κ: g g C denotes the Killing-form.

Simple highest weight modules We fix g b h, a Borel and a Cartan subalgebra. The corresponding affine Borel and Cartan subalgebras are b := g tc[t] b CK CD, ĥ := h CK CD. To any λ ĥ = Hom C (ĥ, C) we associate the simple module L(λ) with highest weight λ. We want to calculate its character char L(λ) = µ h dim C L(λ) µ e µ. Here, L(λ) µ denotes the µ-eigenspace of the ĥ-action.

Simple highest weight modules The affine Weyl group Ŵ acts on ĥ. Let ρ ĥ be an element with ρ, α = 1 for each simple coroot α. The dot-action of Ŵ on ĥ is given by w.λ = w(λ + ρ) ρ. It does not depend on the choice of ρ. Definition The critical hyperplane is {λ ĥ λ, K = ρ, K }.

Known instances The character of L(λ) is known if λ is non-critical (Kashiwara & Tanisaki), if λ Ŵ.( ρ + ρ) (Frenkel & Gaitsgory), if λ is critical and generic (Feigin & Frenkel), if λ is subgeneric (Arakawa & ).

Category O The category O ĝ-mod contains all modules M with a semisimple ĥ-action, a locally finite b-action. We have an abstract block decomposition O = Λ O Λ. We identify each index Λ with the set {λ ĥ L(λ) O Λ }.

Blocks We call O Λ critical if Λ contains a critical weight. This is the case if and only if each weight in Λ is critical. Let Λ be a block index and set Ŵ Λ = s α α is an affine real root with λ, α Z for some/all λ Λ Theorem (Deodhar & Gabber & Kac, Kac & Kazhdan) If Λ is non-critical, then Λ = ŴΛ.λ. If Λ is critical, then Λ = ŴΛ.λ + Zδ. Here, δ ĥ is the smallest positive imaginary root. It is given by δ(d) = 1, δ(h CK) = 0.

Block indices Negative level Critical level Positive level

Problems (?) Let Λ be critical. Λ is not an orbit. There is no highest or lowest weight in Λ. The partial order on each orbit in Λ is not compatible with the Bruhat order. We are going to address these problems.

The affine Weyl group and the set of alcoves Let A be the set of alcoves and A e A the base alcove. We identify Ŵ A w w(a e ). Ŵ carries the Bruhat order. A carries the generic Bruhat order. The above map is not order preserving. We now think of Ŵ and A as partially ordered sets being acted upon by simple reflections from the right. The above map intertwines these actions.

The affine Hecke algebra and its periodic module We denote by Ĥ = w Ŵ Z[v, v 1 ]T w the affine Hecke algebra. For any simple reflection we set H s := vt s + vt e. It satisfies { v 1 T ws + v 1 T w, if ws w, T w H s = vt ws + vt w, if w ws. We denote by M = A A Z[v, v 1 ]A the periodic Ĥ-module. It satisfies { A ws + v 1 A w, if A ws A w, A w H s = A ws + va w, if A w A ws.

The Hecke algebra vs. its periodic module The Hecke algebra governs Iwahori-constructible simple perverse sheaves with C-coefficients on the affine flag variety, Non-critical level representations of ĝ. The periodic module governs restricted representations of g k, char k 0 (conjecturally, char k > h), representations of the small quantum group at an l-th root of unity for l > h, critical level representations (conjecturally).

Block indices Negative level Critical level Positive level

Critical blocks The simple highest weight module L(δ) is one-dimensional and invertible, i.e. L(δ) L( δ) = C triv. We define the shift functor T : O O M M L(δ). It is an autoequivalence with inverse T 1 = L( δ). Observation A block O Λ is critical if and only if it is preserved by T, i.e. if and only if T (O Λ ) O Λ.

The graded center Now we fix a critical block O Λ. For n Z we denote by Mor(id, T n ) the set of natural transformations between the functors id, T n : O Λ O Λ. We define { A n := z Mor(id, T n ) for all M O Λ we have T l (z M ) = z T l M : T l M T n+l M Then A := n Z A n carries a canonical C-algebra structure. It is commutative and associative and HUGE. }

Restricted critical representations Definition We say that M O Λ is restricted if z M = 0 for all z A n, n 0. We denote by O Λ O Λ the subcategory of restricted modules. Each M O Λ has a largest restricted quotient M M, a largest restricted submodule M M. Let (λ) and (λ) be the Verma and the dual Verma module associated to λ Λ. The restricted Verma and the restricted dual Verma module are (λ) and (λ).

The subgeneric situation Suppose that Λ is subgeneric, i.e. Ŵ Λ is isomorphic to the affine Weyl group of type A 1, and regular. In this case, each ŴΛ-orbit is a totally ordered set and we can define the successor bijection α : Λ Λ. Theorem (with T. Arakawa) Each L(λ), λ Λ, admits a projective cover P(λ) in O Λ. It fits into a short exact sequence 0 (α λ) P(λ) (λ) 0. We have [ (λ) : L(µ)] = { 1, if λ {µ, α µ}, 0, else.

Restricted block decomposition Let O O be the full critical restricted subcategory and denote by O = Γ O Γ the abstract block decomposition. Again, we identify Γ with the set {γ ĥ L(γ) O Γ }. For any J ĥ that is open, i.e. J = { γ}, γ J we define O J Γ O Γ as the full subcategory of objects that have weights only in J.

More results Theorem (with T. Arakawa) Let Γ be a restricted index, let J be open and fix γ Γ J. The simple object L(γ) has a projective cover P J (γ) in O J Γ. Each projective in O J Γ has a restricted Verma flag and we have (P J (γ) : (ν)) = [ (ν) : L(γ)] for all ν Γ J (Restricted BGG-reciprocity). [ (λ) : L(ν)] 0 implies ν ŴΓ.λ (Restricted Linkage principle).

Restricted blocks are orbits Negative level Critical level Positive level

The Feigin Frenkel conjecture Each restricted critical index Γ is now a ŴΓ-orbit. As a partially ordered set it carries a variant of the generic Bruhat order. Hence, we expect the representation theory to be governed by the periodic module. Conjecture Suppose that Γ is sufficiently generic. Let γ Γ be dominant for the finite Weyl group action. For any x, y ŴΓ we have [ (x.γ) : L(y.γ)] = p Ax,A y (1), where p, denotes the periodic polynomial associated to ŴΓ. Known for γ = 0 (Frenkel & Gaitsgory) and in the subgeneric cases (Arakawa & ).

Conjectural links Categorifications of Ĥ Categorifications of M Intersection cohomologies of Schubert varieties Non-critical representations of affine Kac Moody algebras W V BMP sheaves on moment graphs AJS & AJS &? Representations of the small quantum group Representations of modular Lie algebras Critical representations of affine Kac Moody algebras