This paper was converted on www.awesomepapers.org from LaTeX by an anonymous user.
Want to know more? Visit the Converter page.

Filtrations on block subalgebras of reduced universal enveloping algebras

Andrei Ionov Department of Mathematics, Massachusetts Institute of Technology, 77 Massachusetts Ave., Cambridge, MA 02139, United States; Department of Mathematics, National Research University Higher School of Economics, 6 Usacheva st., Moscow, Russian Federation, 119048 aionov@mit.edu  and  Dylan Pentland Massachusetts Institute of Technology, 77 Massachusetts Ave., Cambridge, MA 02139, United States dylanp@mit.edu
Abstract.

We study the interaction between the block decompositions of reduced universal enveloping algebras in positive characteristic, the PBW filtration, and the nilpotent cone. We provide two natural versions of the PBW filtration on the block subalgebra AλA_{\lambda} of the restricted universal enveloping algebra 𝒰χ(𝔤)\mathcal{U}_{\chi}(\mathfrak{g}) and show these are dual to each other. We also consider a shifted PBW filtration for which we relate the associated graded algebra to the algebra of functions on the Frobenius neighbourhood of 0 in the nilpotent cone and the coinvariants algebra corresponding to λ\lambda. In the case of 𝔤=𝔰𝔩2(k)\mathfrak{g}=\mathfrak{sl}_{2}(k) in characteristic p>2p>2 we determine the associated graded algebras of these filtrations on block subalgebras of 𝒰0(𝔰𝔩2)\mathcal{U}_{0}(\mathfrak{sl}_{2}). We also apply this to determine the structure of the adjoint representation of 𝒰0(𝔰𝔩2)\mathcal{U}_{0}(\mathfrak{sl}_{2}).

1. Introduction

The key feature of the representation theory of algebraic groups and Lie algebras in characteristic p>0p>0 is the linkage principle providing the block decomposition of the category of representations ([7], [13], [1], [12], [3]). In order to formulate it for a Lie algebra 𝔤\mathfrak{g} of an algebraic group GG one first decomposes the category of representations with respect to the pp-character χ𝔤\chi\in\mathfrak{g}^{*} and passes to the corresponding reduced universal enveloping algebra 𝒰χ(𝔤)\mathcal{U}_{\chi}(\mathfrak{g}). We note here that via the differential map the case χ=0\chi=0 is related to the representation theory of algebraic group GG by the equivalence of categories 𝖱𝖾𝗉(G1)𝒰0(𝔤)𝖬𝗈𝖽\mathsf{Rep}(G_{1})\simeq\mathcal{U}_{0}(\mathfrak{g})-\mathsf{Mod}, where G1G_{1} is the Frobenius kernel of GG and, therefore, is of particular importance. Finally, for 𝒰χ(𝔤)\mathcal{U}_{\chi}(\mathfrak{g}) the block decomposition could be understood as the direct sum decomposition of algebras

𝒰χ(𝔤)=λAλ,\mathcal{U}_{\chi}(\mathfrak{g})=\bigoplus_{\lambda}A_{\lambda},

indexed by certain equivalence-classes of simple 𝒰χ(𝔤)\mathcal{U}_{\chi}(\mathfrak{g})-modules. In the current paper we use the PBW filtration on 𝒰(𝔤)\mathcal{U}(\mathfrak{g}) to study the block subalgebras AλA_{\lambda}.

We study three filtrations on the block subalgebra AλA_{\lambda}. The first two are natural ways to put a PBW filtration on AλA_{\lambda}, by either pushing forward the PBW filtration on 𝒰χ(𝔤)\mathcal{U}_{\chi}(\mathfrak{g}) by the map πλ\pi_{\lambda} projecting onto AλA_{\lambda} or by intersection with the PBW filtration on 𝒰χ(𝔤)\mathcal{U}_{\chi}(\mathfrak{g}). The shifted PBW filtration is obtained from the push forward filtration by additionally assigning the generators of the Harish-Chandra center degree 11.

We realize associated graded algebra grshAλ\operatorname{{gr}}_{\mathrm{sh}}A_{\lambda} as a quotient of a tensor product k[𝒩p]kCλk[\mathcal{N}_{p}]\otimes_{k}C_{\lambda}, where 𝒩p\mathcal{N}_{p} is the Frobenius neighbourhood of 0 inside the nilpotent cone and CλC_{\lambda} is the coinvariants algebra corresponding to the block. For the trivial character this quotient is moreover GG-equivariant. We also show that the first two PBW filtrations we put on AλA_{\lambda} are dual to each other.

In the case of G=SL2(k)G=\mathrm{SL}_{2}(k), we compute explicit central idempotents for the block decomposition of 𝒰χ(𝔤)\mathcal{U}_{\chi}(\mathfrak{g}). In this case for χ=0\chi=0 or regular semisimple we are furthermore explicitly determine associated graded algebras of the filtrations as well as determining the structure of SL2\mathrm{SL}_{2}-representations on them for χ=0\chi=0. Finally, we use this to determine the structure of the adjoint representation of 𝒰0(𝔰𝔩2)\mathcal{U}_{0}(\mathfrak{sl}_{2}). Our result agrees with the main result of [20] for the small quantum group of 𝔰𝔩2\mathfrak{sl}_{2} at the pp-th root of unity.

The key ingredient of our approach is understanding the structure of GG-representation on the algebra of functions k[𝒩]k[\mathcal{N}] on the nilpotent cone, which in the case of χ=0\chi=0 can be exploited to understand block subalgebras as GG-modules. In the case of characteristic 0 the answer were provided in [16]. In the case of characteristic pp though the question is substantially less explored and in general only the existence of the good filtration on k[𝒩]k[\mathcal{N}] is known ([17], [15], §II Proposition 4.20).

This approach to the block subalgebras could possibly be applied to understanding the center of the block subalgebra. The multiplicity of the trivial SL2\mathrm{SL}_{2}-representation as a subrepresentation in AλA_{\lambda} or grAλ\operatorname{{gr}}A_{\lambda} provides an upper bound on the dimension of the center of AλA_{\lambda}. It would be interesting to understand if this method could be used in the general case to understand dimZ(Aλ)\dim Z(A_{\lambda}).

We note that AλA_{\lambda} for a block containing a single simple projective module LL, we have AλEnd(L)A_{\lambda}\simeq\mathrm{End}(L). It was communicated to us by Pavel Etingof that even in the characteristic 0 case the pushforward of the PBW filtration onto End(L)\mathrm{End}(L) for simple modules is not well-understood, despite it being an important problem.

Notation. Throughout, kk will denote an algebraically closed field of characteristic p>0p>0. We let X(1)=X×kSpeckFrobX^{(1)}=X\times_{k}\operatorname{{Spec}}k_{\mathrm{Frob}} be the Frobenius twist of an affine variety over kk, where SpeckFrob\operatorname{{Spec}}k_{\mathrm{Frob}} is a scheme Speck\operatorname{{Spec}}k with kk-algebra structure on kk given via Frob:kk,xxp\mathrm{Frob}:k\to k,x\mapsto x^{p}. We equip this with a map Fr:XX(1)\mathrm{Fr}:X\to X^{(1)} arising from the universal property of the fibre product and the absolute Frobenius XXX\to X.

By an algebraic group GG we will mean a linear algebraic group, so that as a variety it is affine. We put 𝔤\mathfrak{g} for the Lie algebra of GG. We use 𝒰(𝔤)\mathcal{U}(\mathfrak{g}) to denote the universal enveloping algebra, and 𝒰χ(𝔤)=𝒰(𝔤)/xpx[p]χ(x)p\mathcal{U}_{\chi}(\mathfrak{g})=\mathcal{U}(\mathfrak{g})/\langle x^{p}-x^{[p]}-\chi(x)^{p}\rangle to denote the reduced universal enveloping algebra for χ𝔤\chi\in\mathfrak{g}^{*}. There is an adjoint action of GG on 𝒰(𝔤)\mathcal{U}(\mathfrak{g}) induced by the adjoint action of GG on 𝔤\mathfrak{g}. For χ=0\chi=0, the map 𝒰(𝔤)𝒰0(𝔤)\mathcal{U}(\mathfrak{g})\to\mathcal{U}_{0}(\mathfrak{g}) is GG-equivariant, as we have Adg(x[p])=(Adg(x))[p]\mathrm{Ad}_{g}(x^{[p]})=(\mathrm{Ad}_{g}(x))^{[p]}. This yields a GG-action on 𝒰0(𝔤)\mathcal{U}_{0}(\mathfrak{g}).

We use 𝖱𝖾𝗉(G),𝖱𝖾𝗉(𝔤)\mathsf{Rep}(G),\mathsf{Rep}(\mathfrak{g}) for the categories of representations of GG and 𝔤\mathfrak{g} respectively. We put 𝔥𝔤\mathfrak{h}\subset\mathfrak{g} for a Cartan subalgebra, which we assume to be fixed, and WW for the corresponding Weyl group. We put \mathchoice{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\displaystyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\textstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptscriptstyle\bullet$}}}}} to denote the dot-action on the weight lattice and 𝔥\mathfrak{h}: wλ:=w(λ+ρ)ρw\mathchoice{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\displaystyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\textstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptscriptstyle\bullet$}}}}}\lambda\colon=w(\lambda+\rho)-\rho, with ρ\rho being the sum of fundamental weights.

For a graded vector space VV, we write VdV_{d} for the degree dd component. We set Vd:=ddVdV_{\leq d}:=\bigoplus_{d^{\prime}\leq d}V_{d^{\prime}}.

2. Background

This section will cover the background material on the block decomposition for 𝒰χ(𝔤)\mathcal{U}_{\chi}(\mathfrak{g}). We will begin with general background, and at the end of the section discuss how these results present themselves in the case G=SL2G=\mathrm{SL}_{2}. For further details we refer to [15], a good summary of the results is also presented in [4].

2.1. Structure of the center

Let GG be a semisimple connected simply connected algebraic group. Assume that the characteristic pp of the field is ‘very good’ as in [19]. Throughout the paper, we will need to understand the structure of the center of 𝒰(𝔤)\mathcal{U}(\mathfrak{g}) and its image under the quotient map to 𝒰χ(𝔤)\mathcal{U}_{\chi}(\mathfrak{g}).

Definition.

To describe the center Z(𝒰(𝔤))Z(\mathcal{U}(\mathfrak{g})), we will need two subalgebras of 𝒰(𝔤)\mathcal{U}(\mathfrak{g}):

  • ·

    We set ZFr:=k[xipxi[p]|i=1,,dim𝔤]Z_{\mathrm{Fr}}:=k[x_{i}^{p}-x_{i}^{[p]}|i=1,\ldots,\dim\mathfrak{g}] to be the pp-center, where the collection of elements xi𝔤x_{i}\in\mathfrak{g} is a basis of the Lie algebra as a vector space.

  • ·

    We set ZHC:=𝒰(𝔤)GZ_{\mathrm{HC}}:=\mathcal{U}(\mathfrak{g})^{G} to be the subalgebra of GG-invariant elements in 𝒰(𝔤)\mathcal{U}(\mathfrak{g}) under the adjoint action of GG on 𝒰(𝔤)\mathcal{U}(\mathfrak{g}), which is called the Harish-Chandra center.

Under our assumptions we may write the center down explicitly using the following theorem:

Theorem.

We have

Z(𝒰(𝔤))=ZFrZFrGZHCZ(\mathcal{U}(\mathfrak{g}))=Z_{\mathrm{Fr}}\otimes_{Z_{\mathrm{Fr}}^{G}}Z_{\mathrm{HC}}

where elements of ZFrGZ_{\mathrm{Fr}}^{G} are the GG-invariant elements in the pp-center.

Proof.

See Theorem 2 of [19]. ∎

Furthermore, we may make further characterizations of ZFrGZ_{\mathrm{Fr}}^{G} and ZHCZ_{\mathrm{HC}} - the Harish-Chandra isomorphism allows us to understand GG-invariant elements through the Cartan subalgebra 𝔥\mathfrak{h}.

Theorem.

We have an isomorphism

ΘHC:ZHC{\Theta_{\mathrm{HC}}:Z_{\mathrm{HC}}}S(𝔥)W,.{\mathrm{S}(\mathfrak{h})^{W,\mathchoice{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\displaystyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\textstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptscriptstyle\bullet$}}}}}}.}\scriptstyle{\simeq}

Moreover, the center ZHCZ_{\mathrm{HC}} is a polynomial algebra k[c1,,cn]k[c_{1},\ldots,c_{n}] for a set of generators c1,,cnc_{1},\ldots,c_{n} (n=rank𝔤n=\operatorname{{rank}}\mathfrak{g}). Furthermore, upon restricting to ZFrG=ZFrZHCZ_{\mathrm{Fr}}^{G}=Z_{\mathrm{Fr}}\cap Z_{\mathrm{HC}} we get an isomorphism

ZFrG{Z_{\mathrm{Fr}}^{G}}S(𝔥(1))W,.{\mathrm{S}(\mathfrak{h}^{(1)})^{W,\mathchoice{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\displaystyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\textstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptscriptstyle\bullet$}}}}}}.}\scriptstyle{\simeq}

The map S(𝔥(1))W,S(𝔥)W,\mathrm{S}(\mathfrak{h}^{(1)})^{W,\mathchoice{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\displaystyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\textstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptscriptstyle\bullet$}}}}}}\to\mathrm{S}(\mathfrak{h})^{W,\mathchoice{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\displaystyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\textstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptscriptstyle\bullet$}}}}}} is the Artin-Schreier map.

Proof.

The first claim is the main result of [21]. The second claim is Lemma 4 in [19]. ∎

When considering the image of Z(𝒰(𝔤))Z(\mathcal{U}(\mathfrak{g})) in 𝒰χ(𝔤)\mathcal{U}_{\chi}(\mathfrak{g}), we may use these results to understand this as well.

Lemma.

The image of the Z(𝒰(𝔤))Z(\mathcal{U}(\mathfrak{g})) in 𝒰χ(𝔤)\mathcal{U}_{\chi}(\mathfrak{g}) is given by

kχZFrGZHC,k_{\chi}\otimes_{Z_{\mathrm{Fr}}^{G}}Z_{\mathrm{HC}},

where kχk_{\chi} is the 1-dimensional algebra over ZFrZ_{\mathrm{Fr}} induced by the character χ\chi.

Proof.

This follows from applying the quotient map to Z(𝒰(𝔤))=ZFrZFrGZHCZ(\mathcal{U}(\mathfrak{g}))=Z_{\mathrm{Fr}}\otimes_{Z_{\mathrm{Fr}}^{G}}Z_{\mathrm{HC}}. ∎

2.2. The block decomposition

Suppose GG is a reductive algebraic group. We may decompose 𝖱𝖾𝗉(G)\mathsf{Rep}(G) as a direct sum of smaller categories, which creates the block decomposition 𝒰χ(𝔤)=λAλ\mathcal{U}_{\chi}(\mathfrak{g})=\bigoplus_{\lambda}A_{\lambda} that we study. Before stating this decomposition, we need to define the notion of a Serre subcategory.

Definition.

Let 𝒜\mathcal{A} be an abelian category. A Serre subcategory 𝒮𝒜\mathcal{S}\subseteq\mathcal{A} is a non-empty full subcategory so that for any exact sequence

0{0}A{A}B{B}C{C}0{0}

where A,C𝒮A,C\in\mathcal{S} if and only if B𝒮B\in\mathcal{S}.

Proposition 1.

Let 𝔛\mathfrak{X} denote the weight lattice of GG, 𝔛+𝔛\mathfrak{X}_{+}\subset\mathfrak{X} be the subset of positive weights, WaffW^{\mathrm{aff}} the affine Weyl group, and p\mathchoice{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\displaystyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\textstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptscriptstyle\bullet$}}}}}_{p} the pp-dilated dot action of WaffW^{\mathrm{aff}}. We have a decomposition

𝖱𝖾𝗉(G)=λ𝔛/(Waff,p)𝖱𝖾𝗉(G)λ.\mathsf{Rep}(G)=\bigoplus_{\lambda\in\mathfrak{X}/(W^{\mathrm{aff}},\mathchoice{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\displaystyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\textstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptscriptstyle\bullet$}}}}}_{p})}\mathsf{Rep}(G)_{\lambda}.

Here, 𝖱𝖾𝗉(G)λ\mathsf{Rep}(G)_{\lambda} is the Serre subcategory generated by simple modules LλL_{\lambda^{\prime}} for λ\lambda^{\prime} in (Waffpλ)𝔛+(W^{\mathrm{aff}}\mathchoice{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\displaystyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\textstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptscriptstyle\bullet$}}}}}_{p}\lambda)\cap\mathfrak{X}_{+}.

Proof.

This is shown in [8], and discussed in [4]. ∎

We note that when we refer to 𝖱𝖾𝗉(G)λ\mathsf{Rep}(G)_{\lambda} we fix a fundamental domain for 𝔛/(Waff,p)\mathfrak{X}/(W^{\mathrm{aff}},\mathchoice{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\displaystyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\textstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptscriptstyle\bullet$}}}}}_{p}). This applies to all other block decompositions as well. When explicitly needed, we will give a description of this fundamental domain.

The similar results hold for 𝖱𝖾𝗉(𝔤)\mathsf{Rep}(\mathfrak{g}).

Proposition 2.

Let 𝔛\mathfrak{X} denote the weight lattice of GG, WW the finite Weyl group, and \mathchoice{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\displaystyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\textstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptscriptstyle\bullet$}}}}} the dot action of WW. We have a decomposition

𝖱𝖾𝗉(𝔤)=λ𝔥/(W,)𝖱𝖾𝗉(𝔤)λ.\mathsf{Rep}(\mathfrak{g})=\bigoplus_{\lambda\in\mathfrak{h}^{*}/(W,\mathchoice{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\displaystyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\textstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptscriptstyle\bullet$}}}}})}\mathsf{Rep}(\mathfrak{g})_{\lambda}.

Here, 𝖱𝖾𝗉(𝔤)λ\mathsf{Rep}(\mathfrak{g})_{\lambda} is the Serre subcategory generated by the simple modules LλL_{\lambda^{\prime}} for λ\lambda^{\prime} in (Wλ)𝔥(W\mathchoice{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\displaystyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\textstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptscriptstyle\bullet$}}}}}\lambda)\subset\mathfrak{h}^{*}.

In the case λ=wμ\lambda=w\cdot\mu for wWw\in W, we say that λ,μ\lambda,\mu are WW-linked. Letting χ𝔤\chi\in\mathfrak{g}^{*} be a character of 𝔤\mathfrak{g}, we may pass to the reduced universal enveloping algebra

𝒰χ(𝔤)=𝒰(𝔤)/xpx[p]χ(x)p.\mathcal{U}_{\chi}(\mathfrak{g})=\mathcal{U}(\mathfrak{g})/\langle x^{p}-x^{[p]}-\chi(x)^{p}\rangle.

Through the universal property of 𝒰(𝔤)\mathcal{U}(\mathfrak{g}), we have a bijection

{𝔤modules}{\{\mathfrak{g}-\mathrm{modules}\}}{𝒰(𝔤)modules}.{\{\mathcal{U}(\mathfrak{g})-\mathrm{modules}\}.}

This restricts to 𝒰χ(𝔤)\mathcal{U}_{\chi}(\mathfrak{g})-modules when we consider 𝔤\mathfrak{g}-modules with pp-character χ\chi.

Restricting the result of Proposition 2 to the subcategory 𝖱𝖾𝗉(𝔤)χ\mathsf{Rep}(\mathfrak{g})_{\chi} of 𝔤\mathfrak{g}-modules with a given character pp-character χ\chi, we obtain a block decomposition of 𝖱𝖾𝗉(𝔤)χ\mathsf{Rep}(\mathfrak{g})_{\chi}. The simple modules in 𝖱𝖾𝗉(𝔤)χ\mathsf{Rep}(\mathfrak{g})_{\chi} are constructed as the quotients of the so-called baby Verma modules given by Δχ,λ:=𝒰χ(𝔤)𝒰χ(𝔟+)kλ\Delta_{\chi,\lambda}:=\mathcal{U}_{\chi}(\mathfrak{g})\otimes_{\mathcal{U}_{\chi}(\mathfrak{b}^{+})}k_{\lambda}. It is known that all simple 𝒰χ(𝔤)\mathcal{U}_{\chi}(\mathfrak{g})-modules arise in this way, see [12].

We have a block decomposition in this case, which is simply an algebraic fact. One may define a linkage relation among principal indecomposable modules for 𝒰χ(𝔤)\mathcal{U}_{\chi}(\mathfrak{g}), as in [7] §55.

Theorem 1.

We have a decomposition

𝖱𝖾𝗉(𝔤)χ=λAλ𝖬𝗈𝖽\mathsf{Rep}(\mathfrak{g})_{\chi}=\bigoplus_{\lambda}A_{\lambda}-\mathsf{Mod}

where AλA_{\lambda} is the two-sided ideal of 𝒰χ(𝔤)\mathcal{U}_{\chi}(\mathfrak{g}) equal to the sum of all principal indecomposable modules belonging to an equivalence class under the linkage relation.

Proof.

See [7], Theorem 55.2 in §55. ∎

The blocks can again be viewed as Serre subcategories for corresponding simple modules. In the case of G=SL2G=\mathrm{SL}_{2}, we know this decomposition explicitly because there is a complete understanding of the baby Verma modules and simple modules for any character χ\chi.

A more precise result is an explicit description of the blocks in terms of WW-linkage classes. We may explicitly characterize the blocks by the associated baby Verma modules. We assume 𝔤\mathfrak{g} is semisimple, and define a modified weight lattice 𝔛χ\mathfrak{X}_{\chi} as in [14] §6.2 via

𝔛χ={λ𝔥:λ(h)pλ(h[p])=χ(h)p for all h𝔥}.\mathfrak{X}_{\chi}=\{\lambda\in\mathfrak{h}^{*}:\lambda(h)^{p}-\lambda(h^{[p]})=\chi(h)^{p}\text{ for all }h\in\mathfrak{h}\}.

We have |𝔛χ|=pdim𝔥|\mathfrak{X}_{\chi}|=p^{\dim\mathfrak{h}}. This will index all of the baby Verma modules Δχ,λ\Delta_{\chi,\lambda}.

Theorem 2.

For χ𝔤\chi\in\mathfrak{g}^{*}, the blocks of 𝒰χ(𝔤)\mathcal{U}_{\chi}(\mathfrak{g}) are in natural bijection with the WW-linkage classes of weights in 𝔛χ\mathfrak{X}_{\chi}.

Proof.

See [3] §3.18. ∎

We note that the Harish-Chandra center of 𝔤\mathfrak{g} and, in particular, the elements c1,,cnc_{1},\ldots,c_{n}, act by a constant on the simple modules within a given block. For 𝔰𝔩2\mathfrak{sl}_{2} this action uniquely determines the block and thus we will sometimes refer to the block by the constant by which the generator of the Harish-Chandra center acts on the simples in the block.

It is worth noting that in characteristic pp, the differentiation functor

D:𝖱𝖾𝗉(G){D:\mathsf{Rep}(G)}𝖱𝖾𝗉(𝔤){\mathsf{Rep}(\mathfrak{g})}

induces an equivalence of categories between 𝖱𝖾𝗉(G1)\mathsf{Rep}(G_{1}) and 𝒰0(𝔤)\mathcal{U}_{0}(\mathfrak{g})-modules, so in this case Theorem 2 is an immediate consequence of a block decomposition on 𝖱𝖾𝗉(G1)\mathsf{Rep}(G_{1}). Here, G1G_{1} is the kernel of the Frobenius twist Fr:GG(1)\mathrm{Fr}:G\to G^{(1)}. This illustrates the connection between the two block decompositions.

Given this block decomposition, we may decompose the algebra 𝒰χ(𝔤)\mathcal{U}_{\chi}(\mathfrak{g}) into blocks associated to each Serre subcategory. In particular, we may write

𝒰χ(𝔤)=λ𝔛χ/(W,p)Aλ\mathcal{U}_{\chi}(\mathfrak{g})=\bigoplus_{\lambda\in\mathfrak{X}_{\chi}/(W,\mathchoice{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\displaystyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\textstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptscriptstyle\bullet$}}}}}_{p})}A_{\lambda}

where nonzero element xAλx\in A_{\lambda} if it acts nontrivially on 𝖱𝖾𝗉(𝔤)χ,λ\mathsf{Rep}(\mathfrak{g})_{\chi,\lambda} and trivially on all the other subcategories in the decomposition of Theorem 2.

For any decomposition of an algebra into direct summands, there exists a corresponding collection of central idempotents. In particular, the decomposition 𝒰χ(𝔤)=λAλ\mathcal{U}_{\chi}(\mathfrak{g})=\bigoplus_{\lambda}A_{\lambda} can be written as

𝒰χ(𝔤)=λπλ𝒰χ(𝔤),\mathcal{U}_{\chi}(\mathfrak{g})=\bigoplus_{\lambda}\pi_{\lambda}\mathcal{U}_{\chi}(\mathfrak{g}),

where πλ\pi_{\lambda} are central idempotents. Note that due to the result of [11], the central idempotents of 𝒰χ(𝔤)\mathcal{U}_{\chi}(\mathfrak{g}) lie in the image of the center of 𝒰(𝔤)\mathcal{U}(\mathfrak{g}). This allows to interpret the projection maps onto each block as multiplication by πλ\pi_{\lambda}.

Remark.

By abuse of notation we will refer to the projection maps onto blocks as well as the central idempotents in the above decomposition by πλ\pi_{\lambda}.

Recall from the introduction that there is a natural GG-action on 𝒰0(𝔤)\mathcal{U}_{0}(\mathfrak{g}) induced by the adjoint action of GG. Since the central idempotents πλ\pi_{\lambda} are GG-invariant, the corresponding projections are GG-equivariant and the adjoint action preserves the subalgebras AλA_{\lambda}.

2.3. Representation theory of SL2\mathrm{SL}_{2} and 𝔰𝔩2\mathfrak{sl}_{2}

In this subsection, we briefly review the representation theory of SL2\mathrm{SL}_{2} and 𝔰𝔩2\mathfrak{sl}_{2} in characteristic pp. A good reference for this is [18]. This is also summarized (on a less detailed level) in [12] and [14]. Throughout this subsection, we will need p>2p>2 for these results to hold.

The flag variety of SL2\mathrm{SL}_{2} is 𝐏1\mathbf{P}^{1}. This group has weight lattice 𝔛𝐙\mathfrak{X}\simeq\mathbf{Z} and ρ=1\rho=1. We construct representations of SL2\mathrm{SL}_{2} known as Weyl modules - these are defined as λ=H0(𝐏1,𝒪(λ))\nabla_{\lambda}=\mathrm{H}^{0}(\mathbf{P}^{1},\mathcal{O}(\lambda)). We can identify this with

λ=k[x,y]λ=kxλkxλ1ykxyλ1kyλ\nabla_{\lambda}=k[x,y]_{\lambda}=kx^{\lambda}\oplus kx^{\lambda-1}y\oplus\ldots\oplus kxy^{\lambda-1}\oplus ky^{\lambda}

where x,yx,y are homogeneous coordinates for 𝐏1\mathbf{P}^{1} and the subscript denotes the degree λ\lambda part of the grading on k[x,y]k[x,y]. We note that λ\nabla_{\lambda} are indexed by 𝔛+\mathfrak{X}_{+} and the Weyl modules are defined for a general reductive algebraic group in a similar fashion.

Lemma 1.

For λ<p\lambda<p, the module λ\nabla_{\lambda} is simple. For λp\lambda\geq p, it is no longer simple, with simple socle LλL_{\lambda}. We have

Lμp+λLλFrLμ.L_{\mu p+\lambda}\simeq L_{\lambda}\otimes\mathrm{Fr}^{*}L_{\mu}.

As a submodule of λ\nabla_{\lambda}, we may embed LλL_{\lambda} as GxλλG\cdot x^{\lambda}\subseteq\nabla_{\lambda}.

Next, we discuss the representations of 𝔰𝔩2\mathfrak{sl}_{2}. We first need to choose a basis, which will be fixed for the rest of the paper.

Definition.

Let e=(0100)e=\begin{pmatrix}0&1\\ 0&0\end{pmatrix}, f=(0010)f=\begin{pmatrix}0&0\\ 1&0\end{pmatrix}, and h=(1001)h=\begin{pmatrix}1&0\\ 0&-1\end{pmatrix}. These form a basis for 𝔰𝔩2\mathfrak{sl}_{2}, and have the relations

[e,f]=h,[h,f]=2f,[h,e]=2e.[e,f]=h,[h,f]=-2f,[h,e]=2e.

Because we assume p>2p>2, the trace form 4tr(xy)4\mathrm{tr}(xy) is non-degenerate and hence we have 𝔰𝔩2𝔰𝔩2\mathfrak{sl}_{2}\simeq\mathfrak{sl}_{2}^{*}. Thus, when classifying characters we may consider the associated elements in 𝔰𝔩2\mathfrak{sl}_{2}. We may divide them into three categories, up to conjugacy by SL2\mathrm{SL}_{2}:

Lemma 2.

We may divide the characters of 𝔰𝔩2\mathfrak{sl}_{2} into three cases up to conjugacy:

  1. (1)

    χ=0\chi=0.

  2. (2)

    χ0\chi\neq 0 but nilpotent. We pick χ=e\chi=e as a representative.

  3. (3)

    χ\chi regular. We pick ah/2ah/2 with a0a\neq 0 as a representative.

For each of these cases, we have a corresponding classification of simple 𝒰χ(𝔰𝔩2)\mathcal{U}_{\chi}(\mathfrak{sl}_{2}) modules, or simple 𝔰𝔩2\mathfrak{sl}_{2}-modules with pp-character χ\chi. To distinguish from the notation for SL2\mathrm{SL}_{2}-modules, we add the subscript χ\chi to denote which character we are using. We state with these the grouping into different blocks following Theorem 2.

Lemma 3.

We have three cases for the simple 𝒰χ(𝔰𝔩2)\mathcal{U}_{\chi}(\mathfrak{sl}_{2}) modules corresponding to Lemma 2.

  1. (1)

    When χ=0\chi=0, there are pp nonisomorphic simple modules L0,λL_{0,\lambda} for 0λ<p0\leq\lambda<p which are quotients of the baby Verma modules via the exact sequences

    0{0}L0,λ2{L_{0,-\lambda-2}}Δ0,λ{\Delta_{0,\lambda}}L0,λ{L_{0,\lambda}}0.{0.}

    We group L0,λ,L0,λ2L_{0,\lambda},L_{0,-\lambda-2} together in the block decomposition for 𝒰0(𝔰𝔩2)\mathcal{U}_{0}(\mathfrak{sl}_{2}), meaning we have a single block at with a single simple module at λ=p1\lambda=p-1 called the Steinberg module and (p1)/2(p-1)/2 blocks with two simple modules.

  2. (2)

    When χ=e\chi=e, all of the baby Verma modules are simple. We have (p+1)/2(p+1)/2 non-isomorphic baby Verma modules. We have Δe,λΔe,λ2\Delta_{e,\lambda}\simeq\Delta_{e,-\lambda-2} over λ𝐅p\lambda\in\mathbf{F}_{p}. Each block has a single simple module.

  3. (3)

    When χ=ah/2\chi=ah/2 is regular, we have all Δah/2,λ\Delta_{ah/2,\lambda} simple over λ\lambda roots of xpx=ax^{p}-x=a and they are non-isomorphic. In the block decomposition, each block has a single simple module.

In our computations, we will also need some understanding of the projective covers of Lχ,λL_{\chi,\lambda}.

Lemma 4.

We have three cases.

  1. (1)

    χ=0\chi=0: Each simple L0,λL_{0,\lambda} for λ𝐅p\lambda\in\mathbf{F}_{p} (as in Lemma 3) has a projective cover. The simple module L0,p1=P0,p1L_{0,p-1}=P_{0,p-1} is the unique simple projective, and every other L0,λL_{0,\lambda} has a dimension 2p2p indecomposable projective cover P0,λP_{0,\lambda} with composition factors L0,λ,L0,pλ2L_{0,\lambda},L_{0,p-\lambda-2}.

  2. (2)

    χ=e\chi=e: Each Δe,λ\Delta_{e,\lambda} has an indecomposable projective cover Pe,λP_{e,\lambda} of dimension 2p2p which is a self-extension.

  3. (3)

    χ=ah/2\chi=ah/2: Each simple module is projective.

Proof.

See §13 of [12]. ∎

The representations of SL2\mathrm{SL}_{2} and 𝔰𝔩2\mathfrak{sl}_{2} are related by differentiation functor in the following way.

Lemma 5.

We have D(Lλ)L0,λD(L_{\lambda})\simeq L_{0,\lambda} for λ<p\lambda<p, and D(FrLμ)D(\mathrm{Fr}^{*}L_{\mu}) is a trivial representation so that in general

D(Lμp+λ)L0,λμ+1.D(L_{\mu p+\lambda})\simeq L_{0,\lambda}^{\oplus\mu+1}.
Proof.

See [18] §2.4. ∎

Using the following lemma, we can determine bases for 𝒰χ(𝔰𝔩2)\mathcal{U}_{\chi}(\mathfrak{sl}_{2}) and write down the kernel of 𝒰(𝔤)𝒰χ(𝔤)\mathcal{U}(\mathfrak{g})\to\mathcal{U}_{\chi}(\mathfrak{g}).

Lemma 6.

For any character χ\chi, we have eifjhke^{i}f^{j}h^{k} for 0i,j,k<p0\leq i,j,k<p as a basis for 𝒰χ(𝔤)\mathcal{U}_{\chi}(\mathfrak{g}). Depending on the character, we have three possibilities for the ideal ker(𝒰(𝔤)𝒰χ(𝔤))\ker(\mathcal{U}(\mathfrak{g})\to\mathcal{U}_{\chi}(\mathfrak{g})).

  1. (1)

    For χ=0\chi=0, it is ep,fp,hph\langle e^{p},f^{p},h^{p}-h\rangle.

  2. (2)

    For χ=e\chi=e, it is ep,fp1,hph\langle e^{p},f^{p}-1,h^{p}-h\rangle.

  3. (3)

    For χ=ah2\chi=\frac{ah}{2}, it is ep,fp,hpha\langle e^{p},f^{p},h^{p}-h-a\rangle.

Finally, we discuss the center of 𝒰(𝔰𝔩2)\mathcal{U}(\mathfrak{sl}_{2}). As discussed above, this is generated by ZFrZ_{\mathrm{Fr}} and ZHCZ_{\mathrm{HC}}. The lemma above essentially tells us the form of ZFrZ_{\mathrm{Fr}}. As for ZHCZ_{\mathrm{HC}}, we observe that for 𝔰𝔩2\mathfrak{sl}_{2} the Cartan subalgebra 𝔥\mathfrak{h} is simply the span of hh. Then we have S(𝔥)k[h]\mathrm{S}(\mathfrak{h})\simeq k[h], and thus

ZHCk[h](W,).Z_{\mathrm{HC}}\simeq k[h]^{(W,\mathchoice{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\displaystyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\textstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptscriptstyle\bullet$}}}}})}.

The finite Weyl group for 𝔰𝔩2\mathfrak{sl}_{2} is isomorphic to 𝐙/2𝐙\mathbf{Z}/2\mathbf{Z}, and the dot action sends hh2h\mapsto-h-2. Thus, ZHCZ_{\mathrm{HC}} is isomorphic to k[(h1)2]k[(h-1)^{2}], and has a single generator. For our convenience we will denote h1h-1 by hh^{\prime}.

Lemma 7.

Under the Harish-Chandra isomorphism for 𝔰𝔩2\mathfrak{sl}_{2}, the element c=(h1)2+4efZHCc=(h-1)^{2}+4ef\in Z_{\mathrm{HC}} maps to h2h^{\prime 2} in k[h2]k[h^{\prime 2}].

This result tells us that ZHCZ_{\mathrm{HC}} for 𝔰𝔩2\mathfrak{sl}_{2} is k[c]𝒰(𝔰𝔩2)k[c]\subset\mathcal{U}(\mathfrak{sl}_{2}). This is not the usual quadratic Casimir element Ω=ef+fe+h2/2\Omega=ef+fe+h^{2}/2 for 𝔰𝔩2\mathfrak{sl}_{2}, but rather 2Ω+12\Omega+1. For the convenience of notations and computations we shift it so that it vanishes at the fixed point of the \mathchoice{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\displaystyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\textstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptscriptstyle\bullet$}}}}}-action.

3. Filtrations on block subalgebras

3.1. Filtrations of interest

We will be discussing three filtrations of interest in this section. First, recall the definition of the PBW filtration.

Definition.

The Poincaré-Birkhoff-Witt (PBW) filtration on 𝒰(𝔤)\mathcal{U}(\mathfrak{g}) is the filtration F0F1F2F_{0}\subset F_{1}\subset F_{2}\subset\ldots with FdF_{d} given by the degree d\leq d elements with the degree induced from the tensor algebra.

If we choose a basis xix_{i} of 𝔤\mathfrak{g} then we have monomial basis {ixiei}\{\prod_{i}x_{i}^{e_{i}}\} of 𝒰(𝔤)\mathcal{U}(\mathfrak{g}) as a vector space over kk by the PBW theorem. Then FdF_{d} is the subspace of 𝒰(𝔤)\mathcal{U}(\mathfrak{g}) spanned by elements ixiei\prod_{i}x_{i}^{e_{i}} with ieid\sum_{i}e_{i}\leq d. The filtration is compatible with multiplication in a sense that FiFjFi+jF_{i}\cdot F_{j}\subset F_{i+j} and is uniquely characterized by this property together with F0=k1,F1=k1+𝔤𝒰(𝔤)F_{0}=k\cdot 1,F_{1}=k\cdot 1+\mathfrak{g}\subset\mathcal{U}(\mathfrak{g}). It is also preserved by the adjoint action of GG on 𝒰(𝔤)\mathcal{U}(\mathfrak{g}). Finally, for the associated graded algebra of this filtration we have an isomorphism gr𝒰(𝔤)S(𝔤)\operatorname{{gr}}\mathcal{U}(\mathfrak{g})\simeq S(\mathfrak{g}).

We obtain a filtration on 𝒰χ(𝔤)\mathcal{U}_{\chi}(\mathfrak{g}) by applying the quotient map to each vector space in the filtration. From this point onward, we will denote this PBW filtration on 𝒰χ(𝔤)\mathcal{U}_{\chi}(\mathfrak{g}) by VdV_{d}. The associated graded algebra of this filtration is isomorphic to k[𝔤p]k[\mathfrak{g}_{p}], where 𝔤p\mathfrak{g}_{p} is the Frobenius neighbourhood of 0 inside 𝔤\mathfrak{g}, which is defined to be the preimage of 0 under the Frobenius map Fr:𝔤𝔤(1)\mathrm{Fr}:\mathfrak{g}\to\mathfrak{g}^{(1)}. Inside 𝔤\mathfrak{g} it is given by the ideal generated by the elements xipx_{i}^{p}, where xix_{i} runs through a basis of 𝔤\mathfrak{g}.

Definition 1.

There are two natural ways we put a filtration on a block AλA_{\lambda}:

  1. (1)

    The pushforward PBW filtration is given by Vipf:=πλ(Vi)V_{i}^{\mathrm{pf}}:=\pi_{\lambda}(V_{i}).

  2. (2)

    The intersection PBW filtration is given by Viint:=ViAλV_{i}^{\mathrm{int}}:=V_{i}\cap A_{\lambda}.

We note that both filtrations are compatible with multiplication and the pushforward filtration is uniquely characterized by this together with V0pf=kπλV_{0}^{\mathrm{pf}}=k\cdot\pi_{\lambda} and V1pf=kπλ+πλ𝔤V_{1}^{\mathrm{pf}}=k\cdot\pi_{\lambda}+\pi_{\lambda}\mathfrak{g}.

The last filtration we consider is a shifted PBW filtration.

Definition 2.

Define a filtration VishV_{i}^{\mathrm{sh}} on the block AλA_{\lambda} inductively via

Vish:=πλ(Vd)+Vi1sh+jcjVi1sh,V_{i}^{\mathrm{sh}}:=\pi_{\lambda}(V_{d})+V_{i-1}^{\mathrm{sh}}+\sum_{j}c_{j}V_{i-1}^{\mathrm{sh}},

where the cjc_{j} are as in §2.1.

This last filtration is also compatible with multiplication and is uniquely characterized by this together with V0sh=kπλ,V1sh=kπλ+πλ𝔤+spanj(πλcj)V_{0}^{\mathrm{sh}}=k\cdot\pi_{\lambda},V_{1}^{\mathrm{sh}}=k\cdot\pi_{\lambda}+\pi_{\lambda}\mathfrak{g}+\mathrm{span}_{j}(\pi_{\lambda}c_{j}).

The associated graded algebras for these on AλA_{\lambda} are denoted by grpfAλ,grintAλ,grshAλ\operatorname{{gr}}_{\mathrm{pf}}A_{\lambda},\operatorname{{gr}}_{\mathrm{int}}A_{\lambda},\operatorname{{gr}}_{\mathrm{sh}}A_{\lambda} respectively. Finally, note that for χ=0\chi=0 all three filtrations as well as ViV_{i} are preserved by the GG-actions.

3.2. The shifted PBW filtration and the nilpotent cone

In this subsection we study the relation between the nilpotent cone 𝒩\mathcal{N} and the associated graded algebra of AλA_{\lambda} with respect to the shifted PBW filtration VishV_{i}^{\mathrm{sh}}.

Throughout this subsection, we let GG be a semisimple connected simply connected linear algebraic group with Lie algebra 𝔤\mathfrak{g}. We additionally impose the following assumptions on GG:

  1. (1)

    The derived group 𝒟G\mathcal{D}G of GG is simply connected.

  2. (2)

    pp is odd and a good prime for GG (as in §2.1)

  3. (3)

    The Killing form on 𝔤\mathfrak{g} is non-degenerate.

Recall that 𝒟G\mathcal{D}G is the intersection of all normal algebraic subgroups NGN\leq G so that G/NG/N is commutative. It can be viewed as the algebraic group analogue to the commutator subgroup [G,G][G,G]. With these conditions on GG, we may use the relevant results for GG - we note that for G=SL2G=\mathrm{SL}_{2}, all these conditions apply, so any theorems of this section may be used for 𝔰𝔩2\mathfrak{sl}_{2} in characteristic p>2p>2.

Definition.

By abuse of notation we identify generators cic_{i} of the Harish-Chandra center with their image in the associated graded algebra S(𝔤)S(\mathfrak{g}). We define the nilpotent cone 𝒩\mathcal{N} to be a closed subscheme SpecS(𝔤)/c1,,cn\operatorname{{Spec}}\mathrm{S}(\mathfrak{g})/\langle c_{1},\ldots,c_{n}\rangle of 𝔤\mathfrak{g} considered as an affine space.

Under our assumptions on GG the set of closed points of 𝒩\mathcal{N} is the set of nilpotent elements of 𝔤\mathfrak{g} (see for example Theorem 2.6, [9]). Note also, that the adjoint GG-action preserves 𝒩\mathcal{N}.

As we work in characteristic p>0p>0, we have a morphism

Fr:𝒩{\mathrm{Fr}:\mathcal{N}}𝒩(1).{\mathcal{N}^{(1)}.}

We define the Frobenius neighborhood of 0 in 𝒩\mathcal{N}, denoted by 𝒩p\mathcal{N}_{p}, to be the preimage of a point 0𝒩(1)0\in\mathcal{N}^{(1)} under this map. This can be written as 𝒩pSpeck[𝔤p]/c1,,cn\mathcal{N}_{p}\simeq\operatorname{{Spec}}k[\mathfrak{g}_{p}]/\langle c_{1},\ldots,c_{n}\rangle.

For this subsection, we fix a block AλA_{\lambda} throughout. Let αi\alpha_{i} be the constant by which the generator of the center cic_{i} acts on the simple modules associated to the block AλA_{\lambda}.

We put CλC_{\lambda} for the image of the center of 𝒰(𝔤)\mathcal{U}(\mathfrak{g}) in AλA_{\lambda}, which is known as the algebra of coinvariants.

For a root μ\mu of GG let 𝔤μ\mathfrak{g}_{\mu} be a corresponding root space. For a positive root μ\mu of GG we let hμ[𝔤μ,𝔤μ]h_{\mu}\in[\mathfrak{g}_{\mu},\mathfrak{g}_{-\mu}] to be the unique element of 𝔥\mathfrak{h} so that μ(hμ)=2\mu(h_{\mu})=2 (recall p>2p>2). We now have the following lemma, which is a combination of results from [19] and [3].

Lemma 8.

The algebra CλC_{\lambda} is a local ring. Moreover,

  1. (1)

    For χ\chi nilpotent, assigning degree 11 to the elements πλ(ciαi)\pi_{\lambda}(c_{i}-\alpha_{i}) provides a grading on CλC_{\lambda}.

  2. (2)

    We have Cλ=kC_{\lambda}=k if and only if we have χ,λ\chi,\lambda, such that (λ+ρ)(hμ)𝐅p×(\lambda+\rho)(h_{\mu})\not\in\mathbf{F}_{p}^{\times} for all simple roots μ\mu. In particular, we will endow it with the trivial grading.

Proof.

Let 𝔛\mathfrak{X} denote the weight lattice of GG. Let W(λ)W(\lambda) be the stabilizer of λ\lambda under the action of the finite Weyl group WW, and W(λ+𝔛)W(\lambda+\mathfrak{X}) the stabilizer of λ+𝔛\lambda+\mathfrak{X}, consisting of wWw\in W so wλλ𝔛w\lambda-\lambda\in\mathfrak{X}. Given χ𝔤\chi\in\mathfrak{g}^{*}, χp\chi^{p} is a character of the Frobenius twist 𝔤(1)\mathfrak{g}^{*(1)}. As discussed in [19], this ppth power has a Jordan decomposition χp=χs+χn\chi^{p}=\chi_{s}+\chi_{n}. In particular, by the result of [19] and the discussion of §3.8 in [3] we have an isomorphism

CλS(𝔥(1))W(λ)S(𝔥(1))W(λ+𝔛)kχs.C_{\lambda}\simeq\mathrm{S}(\mathfrak{h}^{(1)})^{W(\lambda)}\otimes_{\mathrm{S}(\mathfrak{h}^{(1)})^{W(\lambda+\mathfrak{X})}}k_{\chi_{s}}.

As W(λ+𝔛)W(\lambda+\mathfrak{X}) fixes χs\chi_{s} this will be a local ring. Now further suppose χ\chi is nilpotent. This identification shows that the algebra of coinvariants is graded because χs=0\chi_{s}=0 in this case. Explicitly identifying generators, we see that the grading is the degree grading in ciαic_{i}-\alpha_{i}.

The second case follows from the theorem of §3.10 of [3], since the condition of part (2) of the theorem is equivalent to the algebra of coinvariants being kk. ∎

Remark.

For a regular semisimple character each block satisfies the condition of case (2) of the Lemma. The singular block (stabilized by the WW-action) satisfies the condition of case (2) of the Lemma as well.

In either case, the above Lemma implies that the inclusion CλAλC_{\lambda}\to A_{\lambda} after passing to associated graded algebra becomes an injective map CλgrshAλC_{\lambda}\to\operatorname{{gr}}_{\mathrm{sh}}A_{\lambda} of graded algebras. In the situation of case (2) we have Vish=VipfV_{i}^{\mathrm{sh}}=V_{i}^{\mathrm{pf}}, since the coinvariant algebra is trivial and so πλcj\pi_{\lambda}c_{j} is a scalar element of AλA_{\lambda}.

Since we have πλ(Vi)Vish\pi_{\lambda}(V_{i})\subset V_{i}^{\mathrm{sh}}, there is a well defined map gr𝒰χ(𝔤)grshAλ\operatorname{{gr}}\mathcal{U}_{\chi}(\mathfrak{g})\to\operatorname{{gr}}_{\mathrm{sh}}A_{\lambda}. Note that, since GG is semisimple, the images of the central elements cic_{i} have smaller degree with respect to the shifted filtration then with respect to pushforward filtration and, thus, the image of the ideal c1,,cn\langle c_{1},\ldots,c_{n}\rangle in gr𝒰χ(𝔤)\operatorname{{gr}}\mathcal{U}_{\chi}(\mathfrak{g}) lies in the kernel of the map. It follows that the above map quotients through k[𝒩p]k[𝔤p]/c1,,cnk[\mathcal{N}_{p}]\simeq k[\mathfrak{g}_{p}]/\langle c_{1},\ldots,c_{n}\rangle since k[𝔤p]gr𝒰χ(𝔤)k[\mathfrak{g}_{p}]\simeq\operatorname{{gr}}\mathcal{U}_{\chi}(\mathfrak{g}). We then obtain a map

k[𝒩p]{k[\mathcal{N}_{p}]}grshAλ.{\operatorname{{gr}}_{\mathrm{sh}}A_{\lambda}.}

Furthermore, recall from the end of §2.2 that if χ=0\chi=0 there are GG-actions on 𝒰χ(𝔤)\mathcal{U}_{\chi}(\mathfrak{g}) and AλA_{\lambda} and the map 𝒰χ(𝔤)Aλ\mathcal{U}_{\chi}(\mathfrak{g})\to A_{\lambda} is GG-equivariant and then so is the map k[𝒩p]grshAλk[\mathcal{N}_{p}]\to\operatorname{{gr}}_{\mathrm{sh}}A_{\lambda}.

Putting these maps together, we obtain a map from k[𝒩p]kCλk[\mathcal{N}_{p}]\otimes_{k}C_{\lambda} to grshAλ\operatorname{{gr}}_{\mathrm{sh}}A_{\lambda}. We may then show the following theorem.

Theorem 3.

Assume we are in either case (1) or (2) of Lemma 8. We have a well defined surjective map

k[𝒩p]kCλ{k[\mathcal{N}_{p}]\otimes_{k}C_{\lambda}}grshAλ,{\operatorname{{gr}}_{\mathrm{sh}}A_{\lambda},}

of graded algebras. In particular, in case (2) of the above Lemma, we get a surjective map

k[𝒩p]{k[\mathcal{N}_{p}]}grshAλ=grpfAλ.{\operatorname{{gr}}_{\mathrm{sh}}A_{\lambda}=\operatorname{{gr}}_{\mathrm{pf}}A_{\lambda}.}

Furthermore, for χ=0\chi=0 the map is GG-equivariant, with the GG-action on CλC_{\lambda} defined to be trivial.

Proof.

It remains to prove the surjectivity. The algebra grshAλ\operatorname{{gr}}_{\mathrm{sh}}A_{\lambda} is generated by the images of cjc_{j} and 𝔤𝒰(𝔤)\mathfrak{g}\subset\mathcal{U}(\mathfrak{g}) in it. The first ones lie in the image of CλC_{\lambda} and the second ones lie in the image of k[𝒩p]k[\mathcal{N}_{p}] as degrees of cjc_{j} are bigger then 11 and so c1,,cn𝔤=0\langle c_{1},\ldots,c_{n}\rangle\cap\mathfrak{g}=0. ∎

Given that CλC_{\lambda} is by definition a quotient of a polynomial kk-algebra ZHCS(𝔥)W,Z_{\mathrm{HC}}\simeq\mathrm{S}(\mathfrak{h})^{W,\mathchoice{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\displaystyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\textstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptscriptstyle\bullet$}}}}}}, we may interpret its spectrum as a subscheme XλX_{\lambda} of the affine space 𝔥/W\mathfrak{h}/W. Given that 𝒩\mathcal{N} and hence 𝒩p\mathcal{N}_{p} are affine schemes, we can interpret the tensor product as a fibre product of these schemes. The surjection onto the associated graded algebra tells us that

Spec(grshAλ)𝒩p×kXλ\operatorname{{Spec}}(\operatorname{{gr}}_{\mathrm{sh}}A_{\lambda})\subset\mathcal{N}_{p}\times_{k}X_{\lambda}

can be realized as a closed subscheme of 𝒩p×kXλ\mathcal{N}_{p}\times_{k}X_{\lambda}. Note that for case (2) of Lemma 8 XλX_{\lambda} is a point and for a nilpotent character it is the spectrum of a local ring, so it has a unique closed point.

Let WλW^{\lambda} be the set of minimal coset representatives for the subgroup W(λ)W(\lambda) (the stabilizer of λ\lambda). By [3] §3.19, we, in addition, know the Hilbert series for CλC_{\lambda}, namely

H(Xλ,t)=wWλt(w).H(X_{\lambda},t)=\sum_{w\in W^{\lambda}}t^{\ell(w)}.

In particular, we have dimCλ=[W(λ+𝔛):W(λ)]\dim C_{\lambda}=[W(\lambda+\mathfrak{X}):W(\lambda)].

In the case of 𝔤=𝔰𝔩2\mathfrak{g}=\mathfrak{sl}_{2} the scheme XλX_{\lambda} is equal to Speck\operatorname{{Spec}}k or Speck[ε]/ε2\operatorname{{Spec}}k[\varepsilon]/\varepsilon^{2}, with 𝒩p×kXλ\mathcal{N}_{p}\times_{k}X_{\lambda} being either 𝒩p\mathcal{N}_{p} or a first order thickening of it. Geometrically, we aim to explicitly describe the ideal sheaves of grAλ\operatorname{{gr}}A_{\lambda} as subschemes in the case of χ=0\chi=0. This is the same as determining the kernel of the map in Theorem 3, which in the χ=0\chi=0 case is GG-invariant. Once we decompose the ring of functions on the nilpotent cone into GG-modules we may compute k[𝒩p]kCλk[\mathcal{N}_{p}]\otimes_{k}C_{\lambda} as a GG-module.

3.3. Duality between pushforward and intersection PBW filtrations

In this section we show that the filtrations VipfV_{i}^{\mathrm{pf}} and ViintV_{i}^{\mathrm{int}} have a simple relationship, allowing us to only focus on the pushforward filtration.

The precise relation between these filtrations requires us to provide a non-degenerate associative bilinear form

b:𝒰χ(𝔤)×𝒰χ(𝔤)k.b:\mathcal{U}_{\chi}(\mathfrak{g})\times\mathcal{U}_{\chi}(\mathfrak{g})\to k.

In [2], the case χ=0\chi=0 is treated. In [10] it is generalized to arbitrary χ\chi. We will sketch the construction of this bilinear form in the following lemma.

Let xix_{i} be a basis for 𝔤\mathfrak{g}, so ixiei\prod_{i}x_{i}^{e_{i}} for ei{0,1,,p1}e_{i}\in\{0,1,\ldots,p-1\} form a basis for 𝒰0(𝔤)\mathcal{U}_{0}(\mathfrak{g}). We define SS as the span of ixiei\prod_{i}x_{i}^{e_{i}} where the eie_{i} are not all p1p-1. The bilinear form bb constructed in [2] is defined as b(u,v)=φ0(uv)b(u,v)=\varphi_{0}(uv), where the linear map φ0\varphi_{0} is given by φ0|S=0\varphi_{0}|_{S}=0 and φ0(ixip1)=1\varphi_{0}(\prod_{i}x_{i}^{p-1})=1. The same definition works in the general case.

Lemma 9 ([10]).

There exists a non-degenerate associative bilinear form

b:𝒰χ(𝔤)×𝒰χ(𝔤)k.b:\mathcal{U}_{\chi}(\mathfrak{g})\times\mathcal{U}_{\chi}(\mathfrak{g})\to k.
Proof.

We claim that there is a ZFrZ_{\mathrm{Fr}}-bilinear pairing

𝒰(𝔤)ZFr𝒰(𝔤)ZFr,\mathcal{U}(\mathfrak{g})\otimes_{Z_{\mathrm{Fr}}}\mathcal{U}(\mathfrak{g})\to Z_{\mathrm{Fr}},

defined via the pairing bb on 𝒰0(𝔤)\mathcal{U}_{0}(\mathfrak{g}). The algebra 𝒰(𝔤)\mathcal{U}(\mathfrak{g}) is known to be a free module over ZFrZ_{\mathrm{Fr}} as a consequence of the PBW theorem (see [14]). The elements ixiei\prod_{i}x_{i}^{e_{i}} for ei{0,1,,p1}e_{i}\in\{0,1,\ldots,p-1\} form a basis for 𝒰(𝔤)\mathcal{U}(\mathfrak{g}) as a ZFrZ_{\mathrm{Fr}}-algebra. Define a lifted map Φ0\Phi_{0} in the same way as φ0\varphi_{0}, as the ZFrZ_{\mathrm{Fr}}-linear map given by

Φ0(ixiei)={1 if (e1,,en)=(p1,,p1)0 otherwise.\Phi_{0}(\prod_{i}x_{i}^{e_{i}})=\begin{cases}1\text{ if }(e_{1},\ldots,e_{n})=(p-1,\ldots,p-1)\\ 0\text{ otherwise.}\end{cases}

We define the pairing as b~(x,y)=Φ0(xy)\widetilde{b}(x,y)=\Phi_{0}(xy). The same argument as in [2] is applicable and shows non-degeneracy and associativity.

Let kχk_{\chi} be the one dimensional ZFrZ_{\mathrm{Fr}}-algebra determined by the character (as a map 𝔤k\mathfrak{g}\to k). Noting that 𝒰χ(𝔤)=𝒰(𝔤)ZFrkχ\mathcal{U}_{\chi}(\mathfrak{g})=\mathcal{U}(\mathfrak{g})\otimes_{Z_{\mathrm{Fr}}}k_{\chi}, upon a base change ZFrkχZ_{\mathrm{Fr}}\to k_{\chi} we see b~\widetilde{b} induces the desired pairing on any 𝒰χ(𝔤)\mathcal{U}_{\chi}(\mathfrak{g}). ∎

If we let N=dimk𝔤N=\dim_{k}\mathfrak{g} and ViV_{i} be as in §3.1 we have a filtration of length N(p1)+1N(p-1)+1 on 𝒰χ(𝔤)\mathcal{U}_{\chi}(\mathfrak{g})

0V0V1VN(p1)=𝒰χ(𝔤).0\subset V_{0}\subset V_{1}\subset\ldots\subset V_{N(p-1)}=\mathcal{U}_{\chi}(\mathfrak{g}).

Here, 0 denotes the trivial vector space. From the competibility of the filtration with multiplication and the definition of the bilinear form bb we see that

Vi=VN(p1)i1,V_{i}^{\perp}=V_{N(p-1)-i-1},

where \perp denotes the orthogonal complement with respect to bb.

Additionally, suppose we have a block decomposition 𝒰χ(𝔤)=λAλ\mathcal{U}_{\chi}(\mathfrak{g})=\bigoplus_{\lambda}A_{\lambda}. The AλA_{\lambda} are mutually orthogonal with respect to the algebra structure of 𝒰χ(𝔤)\mathcal{U}_{\chi}(\mathfrak{g}), and hence we deduce that the bilinear form bb restricts to bλ:Aλ×Aλkb_{\lambda}:A_{\lambda}\times A_{\lambda}\to k which is still a non-degenerate associative pairing. We denote the orthogonal complement in AλA_{\lambda} with respect to bλb_{\lambda} by λ\perp_{\lambda}.

Theorem 4.

Let V=ViV=V_{i} for some ii. Then VV^{\perp} is also a term of the PBW-filtration, and

πλ(V)λ=AλV.\pi_{\lambda}(V)^{\perp_{\lambda}}=A_{\lambda}\cap V^{\perp}.

In particular, we have dimπλ(V)+dimAλV=dimAλ\dim\pi_{\lambda}(V)+\dim A_{\lambda}\cap V^{\perp}=\dim A_{\lambda}.

Proof.

The assertion πλ(V)λ=AλV\pi_{\lambda}(V)^{\perp_{\lambda}}=A_{\lambda}\cap V^{\perp} is equivalent to πλ(V)=(AλV)λ\pi_{\lambda}(V)=(A_{\lambda}\cap V^{\perp})^{\perp_{\lambda}}. We have

(AλV)λ=(AλV)Aλ=(Aλ+V)Aλ.(A_{\lambda}\cap V^{\perp})^{\perp_{\lambda}}=(A_{\lambda}\cap V^{\perp})^{\perp}\cap A_{\lambda}=(A_{\lambda}^{\perp}+V)\cap A_{\lambda}.

Now we recall that the map πλ\pi_{\lambda} is a projection map as it is a central idempotent, and also that the kernel is precisely AλA_{\lambda}^{\perp}. This is due to the definition of bb, since if uv=0uv=0 we have b(u,v)=0b(u,v)=0. Thus, we have kerπλ=λλAλ=Aλ\ker\pi_{\lambda}=\bigoplus_{\lambda^{\prime}\neq\lambda}A_{\lambda^{\prime}}=A_{\lambda}^{\perp}.

Since πλ|Aλ=id\pi_{\lambda}|_{A_{\lambda}}=\mathrm{id} we have

πλ((Aλ+V)Aλ)=(Aλ+V)Aλ.\pi_{\lambda}((A_{\lambda}^{\perp}+V)\cap A_{\lambda})=(A_{\lambda}^{\perp}+V)\cap A_{\lambda}.

Knowing the kernel of πλ\pi_{\lambda}, the left side is πλ(V)\pi_{\lambda}(V). Thus πλ(V)=(AλV)λ\pi_{\lambda}(V)=(A_{\lambda}\cap V^{\perp})^{\perp_{\lambda}}. ∎

Due to this result, it suffices to study just one of the filtrations of Definition 1. In what follows we understand the pushforward filtration using its relation to the shifted filtration.

4. The case of 𝔤=𝔰𝔩2\mathfrak{g}=\mathfrak{sl}_{2}

Notation. Throughout this section we will refer to the block by the action of the central element cc (defined by Lemma 7) on the simple modules in the block, which is a constant we denote by α\alpha (similar to the αi\alpha_{i} of §3.2). We also assume p>2p>2 throughout.

4.1. Central idempotents

We start by providing explicit formulas for the central idempotents corresponding to the block and defining the projections πα:𝒰χ(𝔤)Aα\pi_{\alpha}:\mathcal{U}_{\chi}(\mathfrak{g})\to A_{\alpha}. In order to do this, we compute the image of ZHCZ_{\mathrm{HC}} in 𝒰χ(𝔰𝔩2)\mathcal{U}_{\chi}(\mathfrak{sl}_{2}). We will denote this image by ZZ.

Proposition 3.

We have

  1. (1)

    When χ=0\chi=0 or χ=e\chi=e the image of the center is

    Zk[c]/cp2c(p+1)/2+c.Z\simeq k[c]/\langle c^{p}-2c^{(p+1)/2}+c\rangle.
  2. (2)

    When χ=ah/2\chi=ah/2 the image of the center is

    Zk[c]/cp2c(p+1)/2+ca2.Z\simeq k[c]/\langle c^{p}-2c^{(p+1)/2}+c-a^{2}\rangle.
Proof.

By results of 2.1 we have

Z=kχZFrGZHC.Z=k_{\chi}\otimes_{Z_{\mathrm{Fr}}^{G}}Z_{\mathrm{HC}}.

We identify ZHCZ_{\mathrm{HC}} with k[(h1)2]=k[h2]k[(h-1)^{2}]=k[h^{\prime 2}] via Lemma 7. As this is a PID we need only find the relation induced by the tensor product. We may identify

ZFrGS(𝔥(1))W,=k[hph]W,=k[(hph)2].Z_{\mathrm{Fr}}^{G}\simeq\mathrm{S}(\mathfrak{h}^{(1)})^{W,\mathchoice{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\displaystyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\textstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptscriptstyle\bullet$}}}}}}=k[h^{\prime p}-h^{\prime}]^{W,\mathchoice{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\displaystyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\textstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptstyle\bullet$}}}}}{\mathbin{\vbox{\hbox{\scalebox{0.5}{$\scriptscriptstyle\bullet$}}}}}}=k[(h^{\prime p}-h^{\prime})^{2}].

Knowing this, we see that once we expand we get the relation h2p2hp+1+h2=0h^{\prime 2p}-2h^{\prime p+1}+h^{\prime 2}=0 in case (1) of the proposition. Using our preimage cc of the generator h2h^{\prime 2}, once we reverse the Harish-Chandra isomorphism we get k[c]/cp2c(p+1)/2+ck[c]/\langle c^{p}-2c^{(p+1)/2}+c\rangle for the center.

In the same way in case (2) we get the relation (hph)2a2=0(h^{\prime p}-h^{\prime})^{2}-a^{2}=0 for hh^{\prime} since hphh^{\prime p}-h^{\prime} acts by aa on kk, and hence

Zk[c]/cp2c(p+1)/2+ca2.Z\simeq k[c]/\langle c^{p}-2c^{(p+1)/2}+c-a^{2}\rangle.

Now we are ready to compute the central idempotents πα\pi_{\alpha} for the block decompositions of 𝒰χ(𝔰𝔩2)\mathcal{U}_{\chi}(\mathfrak{sl}_{2}).

Theorem 5.

As in Proposition 3, we have two cases for the central idempotents of the block decomposition:

  1. (1)

    Set Φ(c)=cp2c(p+1)/2+c\Phi(c)=c^{p}-2c^{(p+1)/2}+c. When χ=0\chi=0 or ee, the block decomposition becomes

    𝒰χ(𝔰𝔩2)=(αp)1πα𝒰χ(𝔰𝔩2)\mathcal{U}_{\chi}(\mathfrak{sl}_{2})=\bigoplus_{\genfrac{(}{)}{}{}{\alpha}{p}\neq-1}\pi_{\alpha}\mathcal{U}_{\chi}(\mathfrak{sl}_{2})

    where π0=Φ(c)/c\pi_{0}=\Phi(c)/c and πα=2(c+α)Φ(c)(cα)2\pi_{\alpha}=\frac{2(c+\alpha)\Phi(c)}{(c-\alpha)^{2}} for α0\alpha\neq 0 a quadratic residue modulo pp.

  2. (2)

    Set Φa(c)=cp2c(p+1)/2+ca2\Phi_{a}(c)=c^{p}-2c^{(p+1)/2}+c-a^{2} for αk×\alpha\in k^{\times}. We have for χ=ah/2\chi=ah/2 the block decomposition

    𝒰χ(𝔰𝔩2)=Φa(α)=0πα𝒰χ(𝔰𝔩2),\mathcal{U}_{\chi}(\mathfrak{sl}_{2})=\bigoplus_{\Phi_{a}(\alpha)=0}\pi_{\alpha}\mathcal{U}_{\chi}(\mathfrak{sl}_{2}),

    where πα=καΦa(c)cα\pi_{\alpha}=\kappa_{\alpha}\frac{\Phi_{a}(c)}{c-\alpha}, where κα\kappa_{\alpha} is a normalizing constant so that πα(α)=1\pi_{\alpha}(\alpha)=1.

Here, we abuse notation by writing the idempotents πα\pi_{\alpha} as elements of k[c]k[c], and then passing to k[c]/Φ(c)k[c]/\langle\Phi(c)\rangle or k[c]/Φa(c)k[c]/\langle\Phi_{a}(c)\rangle to obtain the actual idempotents.

We will break the proof of this theorem into several parts.

Lemma 10.

Dividing by cases in Theorem 5, we have:

  1. (1)

    When χ=0\chi=0 or ee, if α𝐅p\alpha^{\prime}\in\mathbf{F}_{p} is a square and we view πα\pi_{\alpha} as an element of k[c]k[c] then πα(α)=0\pi_{\alpha}(\alpha^{\prime})=0 unless α=α\alpha^{\prime}=\alpha, in which case we get 11.

  2. (2)

    When χ=ah/2\chi=ah/2 for ak×a\in k^{\times} and α\alpha^{\prime} is a root of Φa\Phi_{a}, we have πα(α)=0\pi_{\alpha}(\alpha^{\prime})=0 unless α=α\alpha^{\prime}=\alpha, in which case we get 11.

Proof.

We begin with case (1). A helpful observation in this case is that cp2c(p+1)/2+cc^{p}-2c^{(p+1)/2}+c already factors completely over 𝐅pk\mathbf{F}_{p}\subset k as c(αp)=1(cα)2c\prod_{\genfrac{(}{)}{}{}{\alpha}{p}=1}(c-\alpha)^{2}. Then we have

π0=(αp)=1(cα)2,\pi_{0}=\prod_{\genfrac{(}{)}{}{}{\alpha}{p}=1}(c-\alpha)^{2},

and so for any nonzero square we get π0(α)=0\pi_{0}(\alpha^{\prime})=0. At 0 we get a product of squares of quadratic residues. This is 11, because k=1p12k2(1)p12(p1)!(1)p12(modp)\prod_{k=1}^{\frac{p-1}{2}}k^{2}\equiv(-1)^{\frac{p-1}{2}}(p-1)!\equiv(-1)^{\frac{p-1}{2}}\pmod{p} by Wilson’s theorem. For α0\alpha\neq 0, we can use the factorization to obtain

πα=2c(c+α)αα,(αp)=1(cα)2.\pi_{\alpha}=2c(c+\alpha)\prod_{\alpha^{\prime}\neq\alpha,\genfrac{(}{)}{}{}{\alpha^{\prime}}{p}=1}(c-\alpha^{\prime})^{2}.

Obviously, this implies the value is 0 at any square not equal to α\alpha. Note that as a polynomial in k[c]k[c] we have

πα(α)=4α2αα,(αp)=1(αα)2=4α2αp3α1,(αp)=1(1α)24α1,(αp)=1(1α)2.\pi_{\alpha}(\alpha)=4\alpha^{2}\prod_{\alpha\neq\alpha^{\prime},\genfrac{(}{)}{}{}{\alpha^{\prime}}{p}=1}(\alpha-\alpha^{\prime})^{2}=4\alpha^{2}\alpha^{p-3}\prod_{\alpha^{\prime}\neq 1,\genfrac{(}{)}{}{}{\alpha^{\prime}}{p}=1}(1-\alpha^{\prime})^{2}\equiv 4\prod_{\alpha^{\prime}\neq 1,\genfrac{(}{)}{}{}{\alpha^{\prime}}{p}=1}(1-\alpha^{\prime})^{2}.

This is equal to 4Φ(c)c(c1)2|14\frac{\Phi(c)}{c(c-1)^{2}}\big{|}_{1}. This can be computed explicitly over 𝐙\mathbf{Z} and the value at 11 is 4(p12)24\left(\frac{p-1}{2}\right)^{2}, and so reducing to 𝐅p[c]k[c]\mathbf{F}_{p}[c]\subset k[c] we see that the value is equal to 11.

In case (2), by definition Φa(c)=Φa(α)(cα)\Phi_{a}(c)=\prod_{\Phi_{a}(\alpha)}(c-\alpha) and all roots have multiplicity 11. The statement now immediately follows from the definition of κα\kappa_{\alpha} and πα\pi_{\alpha}. ∎

Lemma 11.

The elements πα\pi_{\alpha} in all cases are central idempotents, and απα=1\sum_{\alpha}\pi_{\alpha}=1.

Proof.

By construction πα\pi_{\alpha} are central. Consider first the case χ=0\chi=0 or ee.

Let us check πα2=πα\pi_{\alpha}^{2}=\pi_{\alpha}. For α=0\alpha=0, we observe that

π02=(Φ(c)απ0)1cα(αp)=1(cα)2.\pi_{0}^{2}=(\Phi(c)-\alpha\pi_{0})\frac{1}{c-\alpha}\prod_{\genfrac{(}{)}{}{}{\alpha}{p}=1}(c-\alpha)^{2}.

Reducing modulo Φ(c)\Phi(c) and repeatedly applying this relation we get ((αp)=1α2)π0=π0(modΦ(c))\left(\prod_{\genfrac{(}{)}{}{}{\alpha}{p}=1}\alpha^{2}\right)\pi_{0}=\pi_{0}\pmod{\Phi(c)}. Thus, π02=π0\pi_{0}^{2}=\pi_{0}. Using a similar reduction method, we can show πα\pi_{\alpha} is idempotent.

Now we show απα=1\sum_{\alpha}\pi_{\alpha}=1. We claim that this relation holds already in k[c]k[c]. By the previous lemma, as a polynomial in k[c]k[c] the element απα\sum_{\alpha}\pi_{\alpha} on each quadratic residue modulo pp has value 11. For nonresidues η,η𝐅p\eta,\eta^{\prime}\in\mathbf{F}_{p} and any α\alpha we have

πα(η)=π(η/η)α(η).\pi_{\alpha}(\eta)=\pi_{(\eta^{\prime}/\eta)\alpha}(\eta^{\prime}).

To see this, note that in 𝐅p\mathbf{F}_{p} for a nonresidue η\eta we have (αp)=1(ηα)2=(ηp)=1(1η)2=4\prod_{\genfrac{(}{)}{}{}{\alpha}{p}=1}(\eta-\alpha)^{2}=\prod_{\genfrac{(}{)}{}{}{\eta^{\prime}}{p}=-1}(1-\eta^{\prime})^{2}=4. This gives the claim for α=0\alpha=0. The rest comes from the relation 2η(η+αηη)=(η/η)22η(η+α)2\eta^{\prime}(\eta^{\prime}+\alpha\frac{\eta^{\prime}}{\eta})=(\eta/\eta^{\prime})^{2}2\eta(\eta+\alpha), since upon pulling this factor into the product α(η/η)α(ηα)2\prod_{\alpha^{\prime}\neq(\eta^{\prime}/\eta)\alpha}(\eta^{\prime}-\alpha^{\prime})^{2} in the factorization of π(η/η)α(η)\pi_{(\eta^{\prime}/\eta)\alpha}(\eta^{\prime}) we get πα(η)\pi_{\alpha}(\eta). We conclude that

απα(η)=απ(η/η)α(η)=απα(η).\sum_{\alpha}\pi_{\alpha}(\eta)=\sum_{\alpha}\pi_{(\eta^{\prime}/\eta)\alpha}(\eta^{\prime})=\sum_{\alpha}\pi_{\alpha}(\eta^{\prime}).

Hence, we may deduce that απαk[c]\sum_{\alpha}\pi_{\alpha}\in k[c] is a polynomial of degree <p1<p-1 which is constant on the set of quadratic residues and on the set of nonresidues modulo pp. The bound on the degree holds because we know that the leading coefficients of the πα\pi_{\alpha} sum to 0 in 𝐅pk\mathbf{F}_{p}\subset k.

Due to its degree, the residue modulo (c(p1)/21)(c(p1)/2+1)(c^{(p-1)/2}-1)(c^{(p-1)/2}+1) is uniquely determined. By the Chinese remainder theorem, its residues modulo (c(p1)/2±1)(c^{(p-1)/2}\pm 1) uniquely determine the result. That is, we have

απα=x(c(p1)/21)+y(c(p1)/2+1).\sum_{\alpha}\pi_{\alpha}=x(c^{(p-1)/2}-1)+y(c^{(p-1)/2}+1).

Now evaluating on a quadratic residue gives 2y=12y=1, so y12(modp)y\equiv\frac{1}{2}\pmod{p}. We can evaluate at c=0c=0 to get the constant term as 11, so we force x=yx=-y. This implies απα=1\sum_{\alpha}\pi_{\alpha}=1 as desired.

Since in case (2) the polynomial Φa(c)\Phi_{a}(c) has simple roots the claim follows from the previous lemma and the Chinese remainder theorem. ∎

We may now prove the theorem.

Proof of Theorem 5.

The previous lemma shows that in any case the πα\pi_{\alpha} are central idempotents. It is easy to check that they are mutually orthogonal (via Proposition 3), and since they sum to 11 they define a direct sum decomposition

𝒰χ(𝔰𝔩2)=απα𝒰χ(𝔰𝔩2).\mathcal{U}_{\chi}(\mathfrak{sl}_{2})=\bigoplus_{\alpha}\pi_{\alpha}\mathcal{U}_{\chi}(\mathfrak{sl}_{2}).

What remains to check is that this is indeed the block decomposition. For a block corresponding to α\alpha, by definition the action of cc on the simples in the block is equal to α\alpha. It follows that for a constant βα\beta\neq\alpha the action of cβc-\beta is invertible on the block, by the definition of the Serre subcategory. We claim that (cα)dα(c-\alpha)^{d_{\alpha}} acts by 0 on this block, where dαd_{\alpha} is the degree of the factor cαc-\alpha in Φ(c)\Phi(c). Indeed, the action of Φ(c)\Phi(c) on the object in the block is equal up to the invertible element to the multiplication by (cα)dα(c-\alpha)^{d_{\alpha}} but on the other hand it is 0 by Proposition 3. Alternatively, this may be seen from the construction of Theorem 1, because the action of (cα)dα(c-\alpha)^{d_{\alpha}} is 0 on the indecomposable projective covers for the block (see Lemma 4).

It follows that πα\pi_{\alpha} vanishes on the blocks other then the one corresponding to α\alpha. We conclude that πα𝒰χ(𝔰𝔩2)Aα\pi_{\alpha}\mathcal{U}_{\chi}(\mathfrak{sl}_{2})\subset A_{\alpha}. The statement follows by a dimension argument. ∎

An immediate corollary of Theorem 5 is an understanding of the algebra of coinvariants for every block, as we now know the maps πα\pi_{\alpha} and the image of the Harish-Chandra center explicitly.

Corollary 1.

We have two results corresponding to the cases of the previous theorem.

  1. (1)

    For χ=0\chi=0 or ee, the algebra of coinvariants for the block AαA_{\alpha} (indexed by squares in 𝐅p\mathbf{F}_{p}) is k[c](cα)2\frac{k[c]}{(c-\alpha)^{2}} for (αp)=1\genfrac{(}{)}{}{}{\alpha}{p}=1 and k[c]c\frac{k[c]}{c} for α=0\alpha=0.

  2. (2)

    For χ=ah/2\chi=ah/2 regular, the algebra of coinvariants for AαA_{\alpha} (indexed by roots of Φa\Phi_{a}) is k[c]cα\frac{k[c]}{c-\alpha}.

Proof.

The statement follows immediately from the fact that CαπαZC_{\alpha}\simeq\pi_{\alpha}Z. ∎

This is consistent with Lemma 8, since these are all local rings and graded (all characters of 𝔰𝔩2\mathfrak{sl}_{2} are either regular or nilpotent). We also conclude that for χ\chi regular Aα=ker(cα)A_{\alpha}=\ker(c-\alpha), and for χ=0\chi=0 or ee it is A0=kercA_{0}=\ker c and Aα=ker(cα)2A_{\alpha}=\ker(c-\alpha)^{2} for α0\alpha\neq 0.

4.2. Determining the associated graded algebras

Throughout this and next sections we will assume χ=0\chi=0 unless the opposite is specified explicitly.

Recall that under this assumption Theorem 3 provide an SL2\mathrm{SL}_{2}-equivariant map

k[𝒩p]kCα{k[\mathcal{N}_{p}]\otimes_{k}C_{\alpha}}grshAα.{\operatorname{{gr}}_{\mathrm{sh}}A_{\alpha}.}

We determined CαC_{\alpha} in the previous section. Let us now describe k[𝒩p]k[\mathcal{N}_{p}] as a representation of SL2\mathrm{SL}_{2} and a graded algebra.

Consider a matrix A=(abca)A=\begin{pmatrix}a&b\\ c&-a\end{pmatrix} in 𝔰𝔩2\mathfrak{sl}_{2}. It lies in the nilpotent cone if and only if A2=0A^{2}=0, which happens if and only if a2+bc=0a^{2}+bc=0. Thus, we have

𝒩=Speck[a,b,c]/a2+bc.\mathcal{N}=\operatorname{{Spec}}k[a,b,c]/\langle a^{2}+bc\rangle.

Recall that the Frobenius neighborhood of the nilpotent cone, 𝒩p\mathcal{N}_{p}, is defined as the preimage of 0 under the map Fr:𝒩𝒩(1)\mathrm{Fr}:\mathcal{N}\to\mathcal{N}^{(1)}. Thus, for 𝔰𝔩2\mathfrak{sl}_{2} we can write

k[𝒩p]=k[a,b,c]/ap,bp,cp,a2+bc.k[\mathcal{N}_{p}]=k[a,b,c]/\langle a^{p},b^{p},c^{p},a^{2}+bc\rangle.

There is an SL2\mathrm{SL}_{2}-action on 𝒩\mathcal{N} via the adjoint action on 𝔤\mathfrak{g}. This induces an action on 𝒩p\mathcal{N}_{p}, and the structure sheaf becomes an equivariant sheaf for this action so that k[𝒩p]k[\mathcal{N}_{p}] itself is an SL2\mathrm{SL}_{2}-module. The action is compatible with the degree, so we may decompose the degree dd component of k[𝒩p]k[\mathcal{N}_{p}] as an SL2\mathrm{SL}_{2}-module.

Proposition 4.

We have

k[𝒩p]d=2dk[\mathcal{N}_{p}]_{d}=\nabla_{2d}

for d<pd<p, and for pp through 3(p1)/23(p-1)/2 (inclusive) it is L4p2d2L_{4p-2d-2} or 0 after this point. That is, the dimensions of graded components in the associated graded algebra are

1,3,,2p1,2p2,2p6,,41,3,\ldots,2p-1,2p-2,2p-6,\ldots,4

so that dimk[𝒩p]=p2+p212\dim k[\mathcal{N}_{p}]=p^{2}+\frac{p^{2}-1}{2}.

Proof.

The ideal ap,bp,cp\langle a^{p},b^{p},c^{p}\rangle is concentrated in degree p\geq p. Hence, for d<pd<p the graded components of k[𝒩p]k[\mathcal{N}_{p}] are the same as in k[𝒩]k[\mathcal{N}]. We claim these are 2d\nabla_{2d}.

Consider the isomorphism

Speck[x,y]/{±1}{\operatorname{{Spec}}k[x,y]/\{\pm 1\}}𝒩{\mathcal{N}}\scriptstyle{\simeq}

where ±1\pm 1 act by scalars, given by ±(x,y)(xyy2x2xy)\pm(x,y)\mapsto\begin{pmatrix}xy&-y^{2}\\ x^{2}&-xy\end{pmatrix}. It is compatible with the SL2\mathrm{SL}_{2}-action and preserves grading up to rescaling by 22. The ±\pm-invariants on k[x,y]k[x,y] are exactly even graded components, which are 2d\nabla_{2d} as SL2\mathrm{SL}_{2}-representations.

In degree pp the elements ap,bp,cpa^{p},b^{p},c^{p} generating the kernel ideal of the map k[𝒩]k[𝒩p]k[\mathcal{N}]\to k[\mathcal{N}_{p}] form a GG-submodule L2pFrL2L_{2p}\simeq\mathrm{Fr}^{*}L_{2}. For pd3(p1)/2p\leq d\leq 3(p-1)/2, we have an exact sequence

0{0}L2d{L_{2d}}2d{\nabla_{2d}}L4p2d2{L_{4p-2d-2}}0{0}FrL2L2d2p{\mathrm{Fr}^{*}L_{2}\otimes L_{2d-2p}}\scriptstyle{\simeq}

The isomorphism L2dFrL2L2d2pL_{2d}\simeq\mathrm{Fr}^{*}L_{2}\otimes L_{2d-2p} follows via Lemma 1 and this simple submodule is precisely the image of multiplication of the elements in k[𝒩]dpk[\mathcal{N}]_{d-p} by the generators of the ideal. Hence we conclude

k[𝒩p]d=L4p2d2k[\mathcal{N}_{p}]_{d}=L_{4p-2d-2}

for dd in this range. At d=3(p1)2+1d=\frac{3(p-1)}{2}+1, we have an isomorphism

FrL2p1{\mathrm{Fr}^{*}L_{2}\otimes\nabla_{p-1}}3p1{\nabla_{3p-1}}\scriptstyle{\sim}

since the dimension of the left side is (dimFrL2)(dimp1)=3p=dim3p1(\dim\mathrm{Fr}^{*}L_{2})(\dim\nabla_{p-1})=3p=\dim\nabla_{3p-1} and the map is an inclusion. Hence, the graded components are 0 from this point onward. ∎

Remark.

In characteristic 0 the description of the GG-representation structure on k[𝒩]k[\mathcal{N}] for general GG is provided in [16]. In particular, for G=SL2G=\mathrm{SL}_{2} the description is identical to ours.

Consider a block subalgebra AαA_{\alpha} of 𝒰0(𝔰𝔩2)\mathcal{U}_{0}(\mathfrak{sl}_{2}). We put simply cα\langle c-\alpha\rangle for the ideal (cα)Aα(c-\alpha)A_{\alpha} To understand the map

k[𝒩p]kCλ{k[\mathcal{N}_{p}]\otimes_{k}C_{\lambda}}grshAα.{\operatorname{{gr}}_{\mathrm{sh}}A_{\alpha}.}

we will use a map k[𝒩p]grshAα/cαk[\mathcal{N}_{p}]\to\operatorname{{gr}}_{\mathrm{sh}}A_{\alpha}/\langle c-\alpha\rangle and the multiplication by (cα)(c-\alpha) map

grshAα/cα{\operatorname{{gr}}_{\mathrm{sh}}A_{\alpha}/\langle c-\alpha\rangle}grshcα,{\operatorname{{gr}}_{\mathrm{sh}}\langle c-\alpha\rangle,}(cα)\scriptstyle{\cdot(c-\alpha)}

which is well defined since (cα)2=0(c-\alpha)^{2}=0 and shifts degree by 11. We note here that the grading on the ideal cα\langle c-\alpha\rangle is given by intersecting the ideal with the filtration on AαA_{\alpha}.

Lemma 12.

We have a surjective map SL2\mathrm{SL}_{2}-equivariant map

k[𝒩p]{k[\mathcal{N}_{p}]}grshAα/cα.{\operatorname{{gr}}_{\mathrm{sh}}A_{\alpha}/\langle c-\alpha\rangle.}

When χ0\chi\neq 0, this is still well-defined and surjective but need not be SL2\mathrm{SL}_{2}-equivariant.

Proof.

This is a direct consequence of Theorem 3 and its proof. ∎

In terms of the generators a,b,ca,b,c the above map is given explicitly by

aπα(h)¯,bπα(2e)¯,cπα(2f)¯,a\mapsto\overline{\pi_{\alpha}(h)},b\mapsto\overline{\pi_{\alpha}(2e)},c\mapsto\overline{\pi_{\alpha}(2f)},

where we put the overline to denote the image of the element in Aα/cαA_{\alpha}/\langle c-\alpha\rangle and then passing to the associated graded algebra. Note that the images of a,b,ca,b,c generate grshAα/cα\operatorname{{gr}}_{\mathrm{sh}}A_{\alpha}/\langle c-\alpha\rangle, so this map is surjective.

In the case of α=0\alpha=0 for the trivial character, we know πα(cα)=0\pi_{\alpha}(c-\alpha)=0 by Corollary 1. Thus, cα=0\langle c-\alpha\rangle=0. The following theorem shows in the rest of the cases that this and the multiplication by cαc-\alpha maps together suffice to understand the map of Theorem 3.

Theorem 6.

Fix a block AαA_{\alpha} for χ=0,e,\chi=0,e, or ah/2ah/2 as in Lemma 2. with algebra of coinvariants k[c]/(cα)2k[c]/\langle(c-\alpha)^{2}\rangle. Consider the surjective map

k[𝒩p]kk[c](cα)2{k[\mathcal{N}_{p}]\otimes_{k}\frac{k[c]}{(c-\alpha)^{2}}}grshAα{\operatorname{{gr}}_{\mathrm{sh}}A_{\alpha}}

of Theorem 3. A pure tensor x1x\otimes 1 for xx homogeneous is in the kernel when xx is in the kernel of k[𝒩p]grshAα/cαk[\mathcal{N}_{p}]\to\operatorname{{gr}}_{\mathrm{sh}}A_{\alpha}/\langle c-\alpha\rangle. A pure tensor x(cα)x\otimes(c-\alpha) for xx homogeneous is in the kernel if xx is in the kernel of the composite map

k[𝒩p]{k[\mathcal{N}_{p}]}grshAα/cα{\operatorname{{gr}}_{\mathrm{sh}}A_{\alpha}/\langle c-\alpha\rangle}grshcα.{\operatorname{{gr}}_{\mathrm{sh}}\langle c-\alpha\rangle.}(cα)\scriptstyle{\cdot(c-\alpha)}

This describes the kernel restricted to k[𝒩p]1k[\mathcal{N}_{p}]\otimes 1 and k[𝒩p](cα)k[\mathcal{N}_{p}]\otimes(c-\alpha). The kernel is a direct sum of these kernels as vector spaces.

Proof.

From the construction of the map and the proof of Theorem 3 it follows that the image of k[𝒩p]k[\mathcal{N}_{p}] does not intersect the image of the ideal cα\langle c-\alpha\rangle in the associated graded. This implies the assertion about the elements x1x\otimes 1.

By construction of the map, the element (cα)(c-\alpha) in the coinvariants algebra CαC_{\alpha} maps to the image of πα(cα)\pi_{\alpha}(c-\alpha) in the associated graded. Then x(cα)x\otimes(c-\alpha) maps to the image of xx under

k[𝒩p]{k[\mathcal{N}_{p}]}grshAα/cα{\operatorname{{gr}}_{\mathrm{sh}}A_{\alpha}/\langle c-\alpha\rangle}grshcα.{\operatorname{{gr}}_{\mathrm{sh}}\langle c-\alpha\rangle.}(cα)\scriptstyle{\cdot(c-\alpha)}

and assertion about such elements follows.

The restrictions of the kernel to k[𝒩p]1k[\mathcal{N}_{p}]\otimes 1 and k[𝒩p](cα)k[\mathcal{N}_{p}]\otimes(c-\alpha) do not intersect and generate the kernel. This yields the splitting. ∎

We apply Theorem 6 in the case of χ=0\chi=0 and α0\alpha\neq 0, because here we can exploit the SL2\mathrm{SL}_{2}-invariance of the kernel to compute it. With this theorem, we have reduced the problem to understanding the multiplication by (cα)(c-\alpha) maps and the map k[𝒩p]grshAα/cαk[\mathcal{N}_{p}]\to\operatorname{{gr}}_{\mathrm{sh}}A_{\alpha}/\langle c-\alpha\rangle. We will understand grshcα\operatorname{{gr}}_{\mathrm{sh}}\langle c-\alpha\rangle first.

Lemma 13.

Let α0\alpha\neq 0. In AαA_{\alpha}, we have

epω(cα)=0e^{p-\omega}(c-\alpha)=0

where we pick ω\omega such that ω2=α\omega^{2}=\alpha and 1ωp121\leq\omega\leq\frac{p-1}{2}.

Proof.

We may decompose the block subalgebra AαA_{\alpha} into indecomposable projectives over itself as i𝒫i\bigoplus_{i}\mathcal{P}_{i}, since it is Artinian (it has finite dimension over kk). Each of these will be a projective cover of a simple module. On each 𝒫i\mathcal{P}_{i}, the image of multiplication by (cα)(c-\alpha) will be an irreducible module so that (cα)𝒫i=L(c-\alpha)\mathcal{P}_{i}=L or 0, where LL is a simple module for AαA_{\alpha}. This follows from Lemma 4 and that cαc-\alpha annihilates the baby Verma modules in the corresponding block.

There are two isomorphism classes of projective covers for simple modules of AαA_{\alpha}, which are related to each other by the action of the Weyl group W=𝐙/2𝐙W=\mathbf{Z}/2\mathbf{Z} ([6], appendix). This action preserves cαc-\alpha, so if cα=0c-\alpha=0 on one isomorphism class it is 0 on the other. As it does not act by 0 on the block and has a nontrivial kernel, we conclude (cα)𝒫i=L(c-\alpha)\mathcal{P}_{i}=L. We know there are two such simple modules up to isomorphism via the block decomposition, namely L0,pω1L_{0,p-\omega-1} and L0,ω1L_{0,\omega-1}. Then in either case epωL=0e^{p-\omega}L=0, from which the identity follows. ∎

Lemma 14.

Resume the notation and assumptions of the previous lemma. We have dimcα=ω2+(pω)2\dim\langle c-\alpha\rangle=\omega^{2}+(p-\omega)^{2} and an isomorphism

Aα/Ann(cα){A_{\alpha}/\operatorname{{Ann}}(c-\alpha)}Endk(L0,ω1)Endk(L0,pω1).{\mathrm{End}_{k}(L_{0,\omega-1})\oplus\mathrm{End}_{k}(L_{0,p-\omega-1}).}\scriptstyle{\sim}
Proof.

We start by constructing a map

Aα/Ann(cα){A_{\alpha}/\operatorname{{Ann}}(c-\alpha)}Endk(L0,ω1)Endk(L0,pω1).{\mathrm{End}_{k}(L_{0,\omega-1})\oplus\mathrm{End}_{k}(L_{0,p-\omega-1}).}

We may again make a direct sum decomposition into indecomposable projectives Aα=i𝒫iA_{\alpha}=\bigoplus_{i}\mathcal{P}_{i}. This shows (cα)Aα=iLi(c-\alpha)A_{\alpha}=\bigoplus_{i}L_{i} where LiL_{i} are simple 𝔰𝔩2\mathfrak{sl}_{2}-modules which are either L0,ω1L_{0,\omega-1} or L0,pω1L_{0,p-\omega-1}. The multiplicity of each equals their dimension by the results stated in [10], and hence dimcα=ω2+(pω)2\dim\langle c-\alpha\rangle=\omega^{2}+(p-\omega)^{2}.

These are both simple modules for Aα/Ann(cα)cαA_{\alpha}/\operatorname{{Ann}}(c-\alpha)\simeq\langle c-\alpha\rangle due to being simple 𝔰𝔩2\mathfrak{sl}_{2}-modules - we may explicitly define the action of an element of Aα/Ann(cα)A_{\alpha}/\operatorname{{Ann}}(c-\alpha) through the corresponding action under the multiplication by (cα)(c-\alpha) map on (cα)𝒫i(c-\alpha)\mathcal{P}_{i}. These are all the simple modules for Aα/Ann(cα)A_{\alpha}/\operatorname{{Ann}}(c-\alpha) because they are the only simple modules for AαA_{\alpha}.

Now we show the map Aα/Ann(cα)End(L0,ω1)End(L0,pω1)A_{\alpha}/\operatorname{{Ann}}(c-\alpha)\to\mathrm{End}(L_{0,\omega-1})\oplus\mathrm{End}(L_{0,p-\omega-1}) is an isomorphism. The simple Aα/Ann(cα)A_{\alpha}/\operatorname{{Ann}}(c-\alpha)-modules L0,ω1,L0,pω1L_{0,\omega-1},L_{0,p-\omega-1} are projective because they are direct summands of Aα/Ann(cα)A_{\alpha}/\operatorname{{Ann}}(c-\alpha). Then all of the simple modules are projective, which implies that Aα/Ann(cα)A_{\alpha}/\operatorname{{Ann}}(c-\alpha) is a semisimple algebra. The claim follows from the Artin-Wedderburn theorem. ∎

Remark.

When χ=e\chi=e, we have AαMatp(Cα)A_{\alpha}\simeq\mathrm{Mat}_{p}(C_{\alpha}) where Cα=k[c]/(cα)2C_{\alpha}=k[c]/(c-\alpha)^{2} is the algebra of coinvariants from Corollary 1 by [3] §3.19. Then dimkAα=2p2\dim_{k}A_{\alpha}=2p^{2}, and dimkcα=p2\dim_{k}\langle c-\alpha\rangle=p^{2}. We may also use the same argument as above to show Aα/Ann(cα)Endk(Δe,α)A_{\alpha}/\operatorname{{Ann}}(c-\alpha)\simeq\mathrm{End}_{k}(\Delta_{e,\alpha}) - the only difference is that Δe,α\Delta_{e,\alpha} is the only simple that appears.

These observations will allow us to obtain the following result.

Proposition 5.

For the trivial character, via the map of Lemma 12 we have an isomorphism

grshAα/cαk[𝒩p]<p+ω.\operatorname{{gr}}_{\mathrm{sh}}A_{\alpha}/\langle c-\alpha\rangle\simeq k[\mathcal{N}_{p}]_{<p+\omega}.

Given α\alpha we choose ω\omega so α=ω2\alpha=\omega^{2} for 0ωp120\leq\omega\leq\frac{p-1}{2}.

Proof.

In degrees p\geq p we identify all graded components with simple SL2\mathrm{SL}_{2}-modules in k[𝒩p]k[\mathcal{N}_{p}] in Proposition 4. Because the kernel can be checked to be SL2\mathrm{SL}_{2}-invariant by Lemma 12, if there is a nontrivial kernel in some degree dpd\geq p then the kernel includes all degrees d\geq d.

Now we show the map of Lemma 12 is an isomorphism in degrees below pp. If there was a kernel in degree below pp, this would yield a nontrivial kernel in degree p1p-1 so that we get the simple quotient L0L_{0} of 2p2\nabla_{2p-2} in the image.

Note that grshAα/cα\operatorname{{gr}}_{\mathrm{sh}}A_{\alpha}/\langle c-\alpha\rangle is generated by its first graded component L2L_{2} and, thus the multiplication map from L2L0L_{2}\otimes L_{0} is surjective on the pp-th graded component. On the other hand the pp-th graded component is a quotient of k[𝒩p]p=L2p2k[\mathcal{N}_{p}]_{p}=L_{2p-2}, which is an irreducible SL2\mathrm{SL}_{2}-representation and consequently vanishes.

We deduce that a nontrivial kernel in degree p1p-1 yields grshAα/cα\operatorname{{gr}}_{\mathrm{sh}}A_{\alpha}/\langle c-\alpha\rangle vanishing in degrees p\geq p. By dimension count we see that dimAα/cα<p2\dim A_{\alpha}/\langle c-\alpha\rangle<p^{2}. This contradicts our earlier dimension findings in Lemma 14, so in degrees below pp the map of Lemma 12 is an isomorphism. Thus, we deduce that grAα/cα\mathrm{gr}A_{\alpha}/\langle c-\alpha\rangle is k[𝒩p]<dαk[\mathcal{N}_{p}]_{<d_{\alpha}} for some dαpd_{\alpha}\geq p. Determining this dαd_{\alpha} amounts to computing the dimensions of both objects as vector spaces over kk.

We first consider the case of α0\alpha\neq 0. The block AαA_{\alpha} has dimension 2p22p^{2}. Using identification Aα/Ann(cα)(cα)AαA_{\alpha}/\operatorname{{Ann}}(c-\alpha)\simeq(c-\alpha)A_{\alpha} and Lemma 14, we conclude that the dimension of grshAα/cα\operatorname{{gr}}_{\mathrm{sh}}A_{\alpha}/\langle c-\alpha\rangle is

2p2dimkEndk(L0,ω1)Endk(L0,pω1)\displaystyle 2p^{2}-\dim_{k}\mathrm{End}_{k}(L_{0,\omega-1})\oplus\mathrm{End}_{k}(L_{0,p-\omega-1}) =2p2(ω)2(pω)2\displaystyle=2p^{2}-\left(\omega\right)^{2}-\left(p-\omega\right)^{2}
=(p+ω)23(ω)2.\displaystyle=(p+\omega)^{2}-3(\omega)^{2}.

This expands as p2+2ω(pω)p^{2}+2\omega(p-\omega). At ω=p12\omega=\frac{p-1}{2} this is maximized, and matches the dimension of k[𝒩p]k[\mathcal{N}_{p}]. Picking 1ωp121\leq\omega\leq\frac{p-1}{2} to correspond to each block, we see that having ω\omega for our block AαA_{\alpha} means dα=p1+ωd_{\alpha}=p-1+\omega.

In the case of α=0\alpha=0, the block AαA_{\alpha} corresponds to 𝖱𝖾𝗉(𝔰𝔩2)0,0\mathsf{Rep}(\mathfrak{sl}_{2})_{0,0} generated by a single simple projective module LL and A0Endk(L)A_{0}\simeq\mathrm{End}_{k}(L) has dimension p2p^{2}. The result follows from Proposition 4 by summing the dimensions up to degree p1p-1 to get p2p^{2}. This yields the claimed decomposition for ω=0\omega=0. ∎

Remark.

For χ=ah/2\chi=ah/2 and ak×a\in k^{\times}, a block in this case is isomorphic to Endk(Δah/2,λ)\mathrm{End}_{k}(\Delta_{ah/2,\lambda}) so it has dimension p2p^{2}. Additionally, by Corollary 1 we see that cα=0c-\alpha=0 in AαA_{\alpha}, so this tells us the algebra structure of a block as a quotient of k[𝒩p]k[\mathcal{N}_{p}] if we understand the kernel of Lemma 12. In this case, one may explicitly argue there is no kernel in degrees below pp. It is sufficient to check this for the map 𝒰χ(𝔤)/cαAα\mathcal{U}_{\chi}(\mathfrak{g})/\langle c-\alpha\rangle\to A_{\alpha} induced by πα\pi_{\alpha}. From the block decomposition we know precisely which elements are annihilated by πα\pi_{\alpha}, so we can conclude the injectivity in degrees below pp. We then know that k[𝒩p]/k[𝒩p]pk[\mathcal{N}_{p}]/\langle k[\mathcal{N}_{p}]_{p}\rangle injects into grshAα=grpfAα\operatorname{{gr}}_{\mathrm{sh}}A_{\alpha}=\operatorname{{gr}}_{\mathrm{pf}}A_{\alpha}, and as it also has dimension p2p^{2} this is an isomorphism of algebras.

Next, we use Lemma 13 to deduce the structure of cα\langle c-\alpha\rangle for χ=0\chi=0. When α=0\alpha=0, we note this is trivial by Corollary 1.

Proposition 6.

Let α0\alpha\neq 0. We have

(grshcα)d={2(d1) for 1dpωL2p2d for pω<dp0 otherwise.(\operatorname{{gr}}_{\mathrm{sh}}\langle c-\alpha\rangle)_{d}=\begin{cases}\nabla_{2(d-1)}\text{ for }1\leq d\leq p-\omega\\ L_{2p-2d}\text{ for }p-\omega<d\leq p\\ 0\text{ otherwise}\end{cases}.
Proof.

We have a surjective map

grshAα/cα{\operatorname{{gr}}_{\mathrm{sh}}A_{\alpha}/\langle c-\alpha\rangle}grshcα.{\operatorname{{gr}}_{\mathrm{sh}}\langle c-\alpha\rangle.}(cα)\scriptstyle{\cdot(c-\alpha)}

This is because the map of algebras Aα/cαcαA_{\alpha}/\langle c-\alpha\rangle\to\langle c-\alpha\rangle is surjective and respects the filtrations. Thus, we indeed have a surjective map on the associated graded algebras. It is also a map of graded SL2\mathrm{SL}_{2}-representations, since (cα)(c-\alpha) is invariant under the adjoint action of SL2\mathrm{SL}_{2}.

In terms of degrees, since we are in the context of the shifted PBW filtration this sends

(grshAα/cα)d{(\operatorname{{gr}}_{\mathrm{sh}}A_{\alpha}/\langle c-\alpha\rangle)_{d}}gr((cα)Aα)d+1.{\mathrm{gr}((c-\alpha)A_{\alpha})_{d+1}.}

We have a map k[𝒩]d1=2(d1)grsh((cα)Aα)dk[\mathcal{N}]_{d-1}=\nabla_{2(d-1)}\to\operatorname{{gr}}_{\mathrm{sh}}((c-\alpha)A_{\alpha})_{d} for 1dp1\leq d\leq p as 2(d1)=k[𝒩p]d1\nabla_{2(d-1)}=k[\mathcal{N}_{p}]_{d-1} for dd in this range. As a result, the image in the degree d+1d+1 components for dd in this range may be written as quotients of 2(d1)\nabla_{2(d-1)}. Using SL2\mathrm{SL}_{2}-invariance, they are then either 2(d1),L2p2(d1)2=L2p2d\nabla_{2(d-1)},L_{2p-2(d-1)-2}=L_{2p-2d}, or 0.

We showed in Lemma 13 that we have epω(cα)=0e^{p-\omega}(c-\alpha)=0 in AαA_{\alpha}. We deduce that starting at the degree pω+1p-\omega+1 the kernel of

(grshAα/cα)d{(\operatorname{{gr}}_{\mathrm{sh}}A_{\alpha}/\langle c-\alpha\rangle)_{d}}grsh((cα)Aα)d+1{\operatorname{{gr}}_{\mathrm{sh}}((c-\alpha)A_{\alpha})_{d+1}}

is nontrivial. By the same argument as in the first part of the proof of Proposition 5 as the nontrivial kernel in degrees below pp yields vanishing in degrees starting from pp.

As a result we have a surjection

0<dpω2(d1)pω<dpL2p2d{\bigoplus_{0<d\leq p-\omega}\nabla_{2(d-1)}\oplus\bigoplus_{p-\omega<d\leq p}L_{2p-2d}}grshcα{\operatorname{{gr}}_{\mathrm{sh}}\langle c-\alpha\rangle}

of SL2\mathrm{SL}_{2}-modules. By summing up the dimensions of the summands the dimension of the left handside equals to ω2+(pω)2\omega^{2}+(p-\omega)^{2}. From the Weyl modules, we get (pω)2(p-\omega)^{2} and from the simple modules, we get ω2\omega^{2}: starting at d=pd=p, we get the odd numbers starting at 1=dimkL2p2p1=\dim_{k}L_{2p-2p} for the dimensions. The above lemma shows this is exactly the dimension of cαAα/Ann(cα)\langle c-\alpha\rangle\simeq A_{\alpha}/\operatorname{{Ann}}(c-\alpha), so we conclude this is an isomorphism of SL2\mathrm{SL}_{2}-modules and the statement follows.

These results additionally allow us to write down the SL2\mathrm{SL}_{2}-module structure of grshAα\operatorname{{gr}}_{\mathrm{sh}}A_{\alpha} when χ=0\chi=0. Combined with Theorem 6 we may also describe the algebra structure.

Corollary 2.

As an SL2\mathrm{SL}_{2}-module, grshAα\operatorname{{gr}}_{\mathrm{sh}}A_{\alpha} is a direct sum of SL2\mathrm{SL}_{2}-modules for each graded component where

(grshAα)d(grshcα)d(grshAα/cα)d.(\operatorname{{gr}}_{\mathrm{sh}}A_{\alpha})_{d}\simeq(\operatorname{{gr}}_{\mathrm{sh}}\langle c-\alpha\rangle)_{d}\oplus(\operatorname{{gr}}_{\mathrm{sh}}A_{\alpha}/\langle c-\alpha\rangle)_{d}.

This also determines the dimensions of each graded component. For the algebra structure, we have two cases:

  1. (1)

    Let α=0\alpha=0. Then grshAα=Aα/cαk[𝒩p]<p\operatorname{{gr}}_{\mathrm{sh}}A_{\alpha}=A_{\alpha}/\langle c-\alpha\rangle\simeq k[\mathcal{N}_{p}]_{<p}.

  2. (2)

    Take α0\alpha\neq 0. The kernel ideal of the map of Theorem 6 is generated by elements in degree p+ωp+\omega and pω+1p-\omega+1 respectively corresponding to two options of Theorem 6.

Proof.

We know that we have an exact sequence of graded vector spaces

0{0}grshcα{\operatorname{{gr}}_{\mathrm{sh}}\langle c-\alpha\rangle}grshAα{\operatorname{{gr}}_{\mathrm{sh}}A_{\alpha}}grshAα/cα{\operatorname{{gr}}_{\mathrm{sh}}A_{\alpha}/\langle c-\alpha\rangle}0.{0.}

We claim that it splits as the sequence of graded SL2\mathrm{SL}_{2}-representations. From Proposition 1 we know that representations from different blocks do not have nontrivial extensions between them. We observe that on each graded component modules in grshcα\operatorname{{gr}}_{\mathrm{sh}}\langle c-\alpha\rangle and grshAα/cα\operatorname{{gr}}_{\mathrm{sh}}A_{\alpha}/\langle c-\alpha\rangle lie in the different blocks with the exception of the degree pp component because of the shift in indexes induced by surjective map (cα)\cdot(c-\alpha) between them. In degree pp, we have Ext1(L0,L2p2)=0\mathrm{Ext}^{1}(L_{0},L_{2p-2})=0 (by [5]) so we must have a direct sum in this case.

Now let us consider the claims about the algebra structure. In case (1) we have cα=0\langle c-\alpha=0\rangle by Corollary 1 and the claim follows from Proposition 5. Now we consider the claims about generators in case (2). The map k[𝒩p]grshcαk[\mathcal{N}_{p}]\to\operatorname{{gr}}_{\mathrm{sh}}\langle c-\alpha\rangle is the composite map

k[𝒩p]{k[\mathcal{N}_{p}]}grshAα/cα{\operatorname{{gr}}_{\mathrm{sh}}A_{\alpha}/\langle c-\alpha\rangle}grshcα.{\operatorname{{gr}}_{\mathrm{sh}}\langle c-\alpha\rangle.}(cα)\scriptstyle{\cdot(c-\alpha)}

The first map has kernel generated in degree p+ωp+\omega by Proposition 5 and the second map has kernel generated in degree pω+1p-\omega+1 by Proposition 6. The rest follows from Proposition 5. ∎

Remark.

We observe that as a subrepresentation of grshAα\operatorname{{gr}}_{\mathrm{sh}}A_{\alpha} for α0\alpha\neq 0 the trivial module L0L_{0} occurs with the multiplicity 33. This provide an upper bound on the dimension of the center Z(Aα)Z(A_{\alpha}), which is known to be exact in this case.

Two of these dimension comes from CαC_{\alpha}. The third copy of L0L_{0} appears as the image of πα(cα)\pi_{\alpha}(c-\alpha) in degree p+1p+1.

Through the methods similar to the above one may also describe the pushforward filtration.

Proposition 7.

We have an exact sequence

0{0}grpfcα{\operatorname{{gr}}_{\mathrm{pf}}\langle c-\alpha\rangle}grpfAα{\operatorname{{gr}}_{\mathrm{pf}}A_{\alpha}}grpfAα/cα{\operatorname{{gr}}_{\mathrm{pf}}A_{\alpha}/\langle c-\alpha\rangle}0,{0,}

where grpfAα/cα=grshAα/cα\operatorname{{gr}}_{\mathrm{pf}}A_{\alpha}/\langle c-\alpha\rangle=\operatorname{{gr}}_{\mathrm{sh}}A_{\alpha}/\langle c-\alpha\rangle and (grpfcα)d+1=(grshcα)d(\operatorname{{gr}}_{\mathrm{pf}}\langle c-\alpha\rangle)_{d+1}=(\operatorname{{gr}}_{\mathrm{sh}}\langle c-\alpha\rangle)_{d}. As with the shifted PBW filtration, as an exact sequence of SL2\mathrm{SL}_{2}-modules this splits in each degree.

Proof.

The existence of such an exact sequence is clear, since we induce this by passing to the associated graded algebras as the maps in the corresponding exact sequence of algebras respect the filtration VipfV_{i}^{\mathrm{pf}}.

The first claim grpfAα/cα=grshAα/cα\operatorname{{gr}}_{\mathrm{pf}}A_{\alpha}/\langle c-\alpha\rangle=\operatorname{{gr}}_{\mathrm{sh}}A_{\alpha}/\langle c-\alpha\rangle holds because these two filtrations agree on the quotient. The second claim about grpf(cα)Aα\operatorname{{gr}}_{\mathrm{pf}}(c-\alpha)A_{\alpha} follows the exact same argument, except the multiplication by (cα)(c-\alpha) map shifts the degree by 22 instead of 11 and as a result just shifts components in the associated graded algebra.

By the same method as with grshAα\operatorname{{gr}}_{\mathrm{sh}}A_{\alpha}, the block decomposition tells us that there are no nontrivial extensions of SL2\mathrm{SL}_{2}-modules appearing in the exact sequence of Proposition 7 so we understand the structure as an SL2\mathrm{SL}_{2}-module. ∎

Remark.

By virtue of Theorem 4, we also understand the dimensions of graded components of grintAα\operatorname{{gr}}_{\mathrm{int}}A_{\alpha}.

Example.

Let 𝔤=𝔰𝔩2\mathfrak{g}=\mathfrak{sl}_{2}, and suppose char(k)=5\mathrm{char}(k)=5. The following table summarizes the dimensions as computed by Proposition 7 for Vipf,ViintV_{i}^{\mathrm{pf}},V_{i}^{\mathrm{int}} on the blocks A0,A1,A2A_{0},A_{1},A_{2} of dimensions 25,5025,50 and 5050.

First, we consider Vipf=πα(Vi)V_{i}^{\mathrm{pf}}=\pi_{\alpha}(V_{i}). We let * denote the trivial vector space.

ii 0 1 2 3 4 5 6
dimπ0(Vi)\dim\pi_{0}(V_{i}) 1 4 9 16 25 25 25
dimπ1(Vi)\dim\pi_{1}(V_{i}) 1 4 10 20 34 49 50
dimπ2(Vi)\dim\pi_{2}(V_{i}) 1 4 10 20 34 45 50

For α=0\alpha=0, we get the dimensions of the filtration on k[𝒩]k[\mathcal{N}] which are the squares. The other blocks have contributions from both graded algebras in the exact sequence. Next, we put down the dimensions for Viint=ViAαV_{i}^{\mathrm{int}}=V_{i}\cap A_{\alpha}.

ii \ldots 5 6 7 8 9 10 11 12
dimViA0\dim V_{i}\cap A_{0} 0 0 0 0 9 16 21 24 25
dimViA1\dim V_{i}\cap A_{1} 0 0 1 16 30 40 46 49 50
dimViA2\dim V_{i}\cap A_{2} 0 0 5 16 30 40 46 49 50

As can be seen, the dimensions in the two tables sum in pairs to the total dimension of the block due to Theorem 4.

Let us discuss the algebraic structure of grpfAα\operatorname{{gr}}_{\mathrm{pf}}A_{\alpha}. Due to the projection πα:𝒰χ(𝔰𝔩2)grpfAα\pi_{\alpha}:\mathcal{U}_{\chi}(\mathfrak{sl}_{2})\to\operatorname{{gr}}_{\mathrm{pf}}A_{\alpha}, we have a map

gr𝒰χ(𝔰𝔩2)S(𝔰𝔩2)/ep,fp,hp{\operatorname{{gr}}\mathcal{U}_{\chi}(\mathfrak{sl}_{2})\simeq\mathrm{S}(\mathfrak{sl}_{2})/\langle e^{p},f^{p},h^{p}\rangle}grpfAα.{\operatorname{{gr}}_{\mathrm{pf}}A_{\alpha}.}

We wish to determine the kernel of this map using our previous results. By Proposition 5, when α=0\alpha=0 we already understand the kernel is generated by the degree pp component along with cαc-\alpha because we may write this as the composition

gr𝒰χ(𝔰𝔩2)S(𝔰𝔩2)/ep,fp,hp{\operatorname{{gr}}\mathcal{U}_{\chi}(\mathfrak{sl}_{2})\simeq\mathrm{S}(\mathfrak{sl}_{2})/\langle e^{p},f^{p},h^{p}\rangle}k[𝒩p]{k[\mathcal{N}_{p}]}grpfAα.{\operatorname{{gr}}_{\mathrm{pf}}A_{\alpha}.}

For χ=0\chi=0 and α0\alpha\neq 0 the kernel S(𝔰𝔩2)/ep,fp,hpgrpfAα\mathrm{S}(\mathfrak{sl}_{2})/\langle e^{p},f^{p},h^{p}\rangle\to\operatorname{{gr}}_{\mathrm{pf}}A_{\alpha} is generated by (cα)2(c-\alpha)^{2} which has degree 44 and elements in degree p+ωp+\omega and pω+2p-\omega+2. The additional +1+1 comes from (cα)(c-\alpha) now having degree two and shifting degrees in Proposition 6, as discussed in Proposition 7. We can see this using the diagram

grpfAα{\operatorname{{gr}}_{\mathrm{pf}}A_{\alpha}}gr𝒰χ(𝔰𝔩2){\operatorname{{gr}}\mathcal{U}_{\chi}(\mathfrak{sl}_{2})}grpfAα/cα{\operatorname{{gr}}_{\mathrm{pf}}A_{\alpha}/\langle c-\alpha\rangle}πα\scriptstyle{\pi_{\alpha}}

where the bottom map has kernel generated by cαc-\alpha and elements in degree p+ωp+\omega. Through our understanding of the all maps besides πα\pi_{\alpha}, we deduce the stated kernel.

4.3. The adjoint representation

Having computed the structure of grshAα\operatorname{{gr}}_{\mathrm{sh}}A_{\alpha} and grpfAα\operatorname{{gr}}_{\mathrm{pf}}A_{\alpha} as SL2\mathrm{SL}_{2}-modules for χ=0\chi=0, we can use these results to determine the structure of the adjoint representation for 𝒰0(𝔰𝔩2)\mathcal{U}_{0}(\mathfrak{sl}_{2}). We define it as the result of applying the differentiation functor DD to the adjoint action of SL2\mathrm{SL}_{2} on 𝒰0(𝔰𝔩2)\mathcal{U}_{0}(\mathfrak{sl}_{2}). More explicitly, we extend the adjoint representation of 𝔰𝔩2\mathfrak{sl}_{2} to 𝒰0(𝔰𝔩2)\mathcal{U}_{0}(\mathfrak{sl}_{2}) via the Leibnitz rule, and consider the corresponding 𝒰0(𝔰𝔩2)\mathcal{U}_{0}(\mathfrak{sl}_{2})-representation.

Proposition 8.

As an SL2\mathrm{SL}_{2}-module we have

A0i=0(p1)/2P2iA_{0}\simeq\bigoplus_{i=0}^{(p-1)/2}P_{2i}

where P2iP_{2i} is an indecomposable SL2\mathrm{SL}_{2}-module, such that D(P2i)=P0,2iD(P_{2i})=P_{0,2i} for projective modules of Lemma 4.

Proof.

Recall that we have

grpfA0d<p2d\operatorname{{gr}}_{\mathrm{pf}}A_{0}\simeq\bigoplus_{d<p}\nabla_{2d}

in this case. Note that among the presented Weyl modules only pairs of 2j\nabla_{2j} and 2p22j\nabla_{2p-2-2j} lie in the same block as SL2\mathrm{SL}_{2}-representations and can form a nontrivial extension. We aim to show that when possible, we do have a nontrivial extension in this decomposition.

Note that A0=End(L0,p1)=L0,p1L0,p1=L0,p1L0,p1A_{0}=\mathrm{End}(L_{0,p-1})=L_{0,p-1}\otimes L_{0,p-1}^{*}=L_{0,p-1}\otimes L_{0,p-1} as an 𝔰𝔩2\mathfrak{sl}_{2}-representation. In particular, it is a projective 𝔰𝔩2\mathfrak{sl}_{2}-module. Since, indecomposable projective 𝔰𝔩2\mathfrak{sl}_{2}-modules have dimension pp or 2p2p, extensions between D(2j)D(\nabla_{2j}) and D(2p22j)D(\nabla_{2p-2-2j}) are all necessarily nontrivial and, hence, the same is true for 2j\nabla_{2j} and 2p22j\nabla_{2p-2-2j}. We identify the corresponding projective 𝔰𝔩2\mathfrak{sl}_{2}-module as being exactly P0,2iP_{0,2i} by noticing that its socle is equal to the socle of D(2j)D(\nabla_{2j}), which in turn equals to D(L2j)=L0,2jD(L_{2j})=L_{0,2j} for j(p1)/2j\leq(p-1)/2.

The following lemma allows us to extend the calculation for this block to other blocks for the trivial character.

Lemma 15.

In Aα/cαA_{\alpha}/\langle c-\alpha\rangle, the SL2\mathrm{SL}_{2}-submodule Vp1pf¯\overline{V_{p-1}^{\mathrm{pf}}} is independent of α\alpha, where the bar denotes reduction modulo cα\langle c-\alpha\rangle.

Proof.

We have a map

𝒰(𝔰𝔩2)/cα{\mathcal{U}(\mathfrak{sl}_{2})/\langle c-\alpha\rangle}Aα/cα,{A_{\alpha}/\langle c-\alpha\rangle,}

which after passing to the associated graded algebras for the PBW filtration and pushforward PBW filtration on AαA_{\alpha} provide a map

S(𝔰𝔩2)/c{\mathrm{S}(\mathfrak{sl}_{2})/\langle c\rangle}grpfAα/cα,{\operatorname{{gr}}_{\mathrm{pf}}A_{\alpha}/\langle c-\alpha\rangle,}

The quotient S(𝔰𝔩2)/c\mathrm{S}(\mathfrak{sl}_{2})/\langle c\rangle is identified with k[𝒩]k[\mathcal{N}] as an algebra and SL2\mathrm{SL}_{2}-module and, thus, we know that the second map is isomorphism in degrees below pp. It follows that the first map is also an isomorphism in degrees below pp.

Note now that the algebra 𝒰(𝔰𝔩2)\mathcal{U}(\mathfrak{sl}_{2}) is free as a module over its Harish-Chandra center ZHCk[c]Z_{\mathrm{HC}}\simeq k[c]. By the definition SL2\mathrm{SL}_{2} acts trivially on ZHCZ_{\mathrm{HC}}. It follows that the SL2\mathrm{SL}_{2}-module structure on 𝒰(𝔰𝔩2)/cα\mathcal{U}(\mathfrak{sl}_{2})/\langle c-\alpha\rangle does not depend on α\alpha. This implies the claim. ∎

Corollary.

There is an isomorphism of SL2\mathrm{SL}_{2}-representations (Aα/cα)<pA0(A_{\alpha}/\langle c-\alpha\rangle)_{<p}\simeq A_{0}.

From this, we may deduce the 𝔰𝔩2\mathfrak{sl}_{2}-module structure of both Aα/cαA_{\alpha}/\langle c-\alpha\rangle and (cα)Aα(c-\alpha)A_{\alpha}.

Proposition 9.

For all α\alpha, we have a decomposition of 𝔰𝔩2\mathfrak{sl}_{2}-modules

Aα/cα=0i(p1)/2P0,2ipi<p+ωL0,3p2i22.A_{\alpha}/\langle c-\alpha\rangle=\bigoplus_{0\leq i\leq(p-1)/2}P_{0,2i}\oplus\bigoplus_{p\leq i<p+\omega}L_{0,3p-2i-2}^{\oplus 2}.

For (cα)Aα(c-\alpha)A_{\alpha} when α0\alpha\neq 0, we have a decomposition

ωip12P0,2ipω<ipL0,2p2i2.\bigoplus_{\omega\leq i\leq\frac{p-1}{2}}P_{0,2i}\oplus\bigoplus_{p-\omega<i\leq p}L_{0,2p-2i}^{\oplus 2}.
Proof.

The result on Aα/cαA_{\alpha}/\langle c-\alpha\rangle can be deduced by using Proposition 5. In degrees <p<p we have a projective 𝔰𝔩2\mathfrak{sl}_{2}-submodule, which, hence splits off as a direct summand. Remaining simple SL2\mathrm{SL}_{2}-modules belong to different blocks and, hence, do not have nontrivial extensions between them. It remains to observe that D(L4p2i2)=L0,3p2i22D(L_{4p-2i-2})=L_{0,3p-2i-2}^{\oplus 2}.

The decomposition of (cα)Aα(c-\alpha)A_{\alpha} comes from applying the multiplication by (cα)(c-\alpha) map to (Aα/cα)<pA0(A_{\alpha}/\langle c-\alpha\rangle)_{<p}\simeq A_{0}. By Proposition 6 we know that in degrees pω\leq p-\omega it is an isomorphism. Hence for ωip12\omega\leq i\leq\frac{p-1}{2} the modules P2iP_{2i} map isomorphically from (Aα/cα)<p(A_{\alpha}/\langle c-\alpha\rangle)_{<p} onto its image in (cα)Aα(c-\alpha)A_{\alpha}. The resulting sum ωip12P0,2i\bigoplus_{\omega\leq i\leq\frac{p-1}{2}}P_{0,2i} is a projective module and consequently splits off as a direct summand. In degrees >pω>p-\omega the multiplication by (cα)(c-\alpha) map is not an isomorphism, and so we are left with a collection of simple modules L0,2p2i=D(L2p2i)L_{0,2p-2i}=D(L_{2p-2i}) for pω<ipp-\omega<i\leq p with two copies each as possible subquotients. Different such modules belong to different blocks and, therefore, have no nontrivial extensions. The two copies of L0,2p2iL_{0,2p-2i} appear as a direct sum because prior to applying DD the modules L2p2iL_{2p-2i} appear as a direct sum as they have no nontrivial extensions by [5]. They lie in different blocks than the other SL2\mathrm{SL}_{2}-modules which appear, and so each remaining simple enters the module as a direct summand. ∎

Lemma 16.

For α0\alpha\neq 0 as an 𝔰𝔩2\mathfrak{sl}_{2}-module, we have

Aα=(cα)AαAα/cα.A_{\alpha}=(c-\alpha)A_{\alpha}\oplus A_{\alpha}/\langle c-\alpha\rangle.
Proof.

As seen above there are surjective morphisms of 𝔰𝔩2\mathfrak{sl}_{2}-representations

𝒰(𝔰𝔩2){\mathcal{U}(\mathfrak{sl}_{2})}𝒰(𝔰𝔩2)/cα{\mathcal{U}(\mathfrak{sl}_{2})/\langle c-\alpha\rangle}i=0(p1)/2P0,2i.{\bigoplus_{i=0}^{(p-1)/2}P_{0,2i}.}

Let II be the kernel of the composition.

Consider a short exact sequence of 𝔰𝔩2\mathfrak{sl}_{2}-representations

0{0}𝒰(𝔰𝔩2)/I{\mathcal{U}(\mathfrak{sl}_{2})/I}𝒰(𝔰𝔩2)/(cα)I{\mathcal{U}(\mathfrak{sl}_{2})/(c-\alpha)I}𝒰(𝔰𝔩2)/cα{\mathcal{U}(\mathfrak{sl}_{2})/\langle c-\alpha\rangle}0.{0.}(cα)\scriptstyle{(c-\alpha)\cdot}

As 𝒰(𝔰𝔩2)/I\mathcal{U}(\mathfrak{sl}_{2})/I is a projective 𝔰𝔩2\mathfrak{sl}_{2}-module the sequence splits.

Note further that we know that the projection 𝒰(𝔰𝔩2)Aα\mathcal{U}(\mathfrak{sl}_{2})\to A_{\alpha} quotients through 𝒰(𝔰𝔩2)/(cα)I\mathcal{U}(\mathfrak{sl}_{2})/(c-\alpha)I with (cα)𝒰(𝔰𝔩2)/(cα)I(c-\alpha)\mathcal{U}(\mathfrak{sl}_{2})/(c-\alpha)I mapping onto (cα)Aα(c-\alpha)A_{\alpha}. Hence we also have the splitting of the sequence

0{0}(cα)Aα{(c-\alpha)A_{\alpha}}Aα{A_{\alpha}}Aα/cα{A_{\alpha}/\langle c-\alpha\rangle}0{0}

and the statement follows. ∎

With these results, we have now determined the structure of AαA_{\alpha} as a direct summand in the adjoint representation of 𝒰0(𝔰𝔩2)\mathcal{U}_{0}(\mathfrak{sl}_{2}).

Theorem 7.

The structure of a block A0i=0(p1)/2P0,2iA_{0}\simeq\bigoplus_{i=0}^{(p-1)/2}P_{0,2i} as an 𝔰𝔩2\mathfrak{sl}_{2}-module. For α0\alpha\neq 0 the adjoint representation AαA_{\alpha} is the direct sum of the two components in Proposition 9.

Proof.

Follows from the previous results. ∎

Remark.

The decomposition matches with the decomposition of the adjoint representation for the small quantum group 𝔰𝔩2\mathfrak{sl}_{2} at the ppth root of unity established in [20].

5. Acknowledgments

The authors thank Roman Bezrukavnikov for introducing the problem and many helpful suggestions. The authors are grateful to the MIT SPUR program and its organizers and, especially, its advisors Ankur Moitra and David Jerison for helpful conversations. The first author was funded by RFBR, project number 19-31-90078.

References

  • [1] Andersen, H. H. The strong linkage principle. Journal für die reine und angewandte Mathematik 1980, 315 (1980), 53–59.
  • [2] Berkson, A. The uu-algebra of a restricted Lie algebra is Frobenius. Proceedings of the American Mathematical Society 15, 1 (1964), 14–15.
  • [3] Brown, K., and Gordon, I. The ramification of centres: Lie algebras in positive characteristic and quantised enveloping algebras. Mathematische Zeitschrift 238, 4 (2001), 733–779.
  • [4] Ciappara, J., and Williamson, G. Lectures on the geometry and modular representation theory of algebraic groups. https://arxiv.org/pdf/2004.14791.pdf, 2020.
  • [5] Cline, E. Ext1\mathrm{Ext}^{1} for SL2\mathrm{SL}_{2}. Communications in Algebra 7, 1 (1979), 107–111.
  • [6] Cline, E. T., Parshall, B. J., and Scott, L. L. On injective modules for infinitesimal algebraic groups, i. Journal of the London Mathematical Society 2, 2 (1985), 277–291.
  • [7] Curtis, C., and Reiner, I. Representation theory of finite groups and associative algebras, vol. 356. American Mathematical Soc., 1966.
  • [8] Donkin, S. The blocks of a semisimple algebraic group. Journal of Algebra 67, 1 (1980), 36–53.
  • [9] Friedlander, E., and Parshall, B. Cohomology of lie algebras and algebraic groups. American Journal of Mathematics 108, 1 (1986), 235–253.
  • [10] Friedlander, E. M., and Parshall, B. J. Modular representation theory of lie algebras. American Journal of Mathematics 110, 6 (1988), 1055–1093.
  • [11] Goldie, A. Localization in non-commutative Noetherian rings. Journal of Algebra 5, 1 (1967), 89–105.
  • [12] Humphreys, J. Modular representations of simple lie algebras. Bulletin of the American Mathematical Society 35, 2 (1998), 105–122.
  • [13] Humphreys, J., and Jantzen, J. C. Blocks and indecomposable modules for semisimple algebraic groups. Journal of Algebra 54, 2 (1978), 494–503.
  • [14] Jantzen, J. C. Representations of lie algebras in prime characteristic. In Representation theories and algebraic geometry. Springer, 1998, pp. 185–235.
  • [15] Jantzen, J. C. Representations of algebraic groups. No. 107. American Mathematical Soc., 2007.
  • [16] Kostant, B. Lie group representations on polynomial rings. American Journal of Mathematics 85, 3 (1963), 327–404.
  • [17] Kumar, S., Lauritzen, N., and Thomsen, J. F. Frobenius splitting of cotangent bundles of flag varieties. Inventiones mathematicae 136, 3 (1999), 603–621.
  • [18] Losev, I. Representation theory of SL2(F)\mathrm{SL}_{2}({F}) and 𝔰𝔩2(F)\mathfrak{sl}_{2}({F}). https://gauss.math.yale.edu/~il282/RT/RT4.pdf.
  • [19] Mirković, I., and Rumynin, D. Centers of reduced enveloping algebras. Mathematische Zeitschrift 231, 1 (1999), 123–132.
  • [20] Ostrik, V. Decomposition of the adjoint representation of the small quantum 𝔰𝔩2\mathfrak{sl}_{2}. https://arxiv.org/pdf/q-alg/9512026.pdf, 1995.
  • [21] Weisfeiler, B. Coadjoint action of a semi-simple algebraic group and the center of the enveloping algebra in characteristic p. In Indag. math (1976), Citeseer.