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NON-PERVERSE PARITY SHEAVES ON THE FLAG VARIETY

Published online by Cambridge University Press:  23 August 2022

PETER J. MCNAMARA*
Affiliation:
School of Mathematics and Statistics The University of Melbourne Parkville, VIC, 3010 Australia [email protected]
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Abstract

We give examples of non-perverse parity sheaves on Schubert varieties for all primes.

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This is an Open Access article, distributed under the terms of the Creative Commons Attribution-NonCommercial-ShareAlike licence (https://creativecommons.org/licenses/by-nc-sa/4.0/), which permits non-commercial re-use, distribution, and reproduction in any medium, provided the same Creative Commons licence is included and the original work is properly cited. The written permission of Cambridge University Press must be obtained for commercial re-use.
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© The Author(s), 2022. Published by Cambridge University Press on behalf of Foundation Nagoya Mathematical Journal

1 Introduction

The notion of a parity sheaf was introduced in [Reference Juteau, Mautner and WilliamsonJMW] and has since become an important object in modular geometric representation theory. An even/odd sheaf on a complex variety X with coefficients in a field k is an object of $D^b_c(X;k)$ Footnote 1 whose star and shriek restrictions to all points only have even/odd cohomology. A parity sheaf is a direct sum of an even and an odd sheaf. (We only consider parity sheaves for the zero pariversity in this paper.)

In this paper, we take X to be the variety of all complete flags in $\mathbb {C}^n$ , and only consider sheaves which are constructible with respect to the stratification by Schubert varieties. Then, by [Reference Juteau, Mautner and WilliamsonJMW, Th. 4.6], for each $w\in S_n$ , there exists a unique indecomposable parity sheaf $\mathcal {E}_w$ whose support is the Schubert variety $X_w$ , up to an overall homological shift. Up to homological shift, these constitute all indecomposable Borel-constructible parity sheaves on the flag variety X. We normalize this shift such that when restricted to the Schubert cell, $\mathcal {E}_w$ is the constant sheaf shifted by $\dim (X_w)$ . This ensures that when the characteristic of k is zero, that $\mathcal {E}_w$ is isomorphic to the intersection cohomology sheaf $IC(X_w;k)$ . We call such parity sheaves normalized.

Let p be the characteristic of k. We provide the first examples of normalised parity sheaves on Schubert varieties which are not perverse for primes $p>2$ . Examples for $p=2$ were recently constructed in [Reference Libedinsky and WilliamsonLW]. Our family of examples also includes parity sheaves which are arbitrarily non-perverse. We are not able to provide examples with p greater than the Coxeter number, but we expect that such examples exist. One geometric consequence is that by Theorem 5.1, the non-perverseness of these sheaves proves that these Schubert varieties do not have any semi-small resolutions. Examples of non-perverse parity sheaves are also of representation-theoretic interest thanks to [Reference Achar and RicheAR].

Our examples generalize constructions of Kashiwara and Saito [Reference Kashiwara and SaitoKS], Polo (unpublished), and McNamara and Williamson [Reference McNamara and WilliamsonMW]. We have phrased things in terms of parity sheaves as that is the more traditional formulation, although the construction of Theorem 5.1 is more general. Despite this more general construction, we rely on some of the theory of parity sheaves in our proof.

2 Statement of the result

Let p be a prime. Let d and l be positive integers such that $p^d\geq l\geq 3$ . Let $q=p^d$ . Define the following permutation $y\in S_{q(l+2)}$ :

$$\begin{align*}y(j)=\begin{cases} (l+1)q, &\text{if } j=1, \\ q+2-j, &\text{if } 2\leq j\leq q, \\ (l+2)q, &\text{if } j=q+1, \\ (l+2)q+1-j, &\text{if } q+2\leq j<(l+1)q \text{ and } j\not\equiv0,1\pmod q, \\ (l+2)q-j, &\text{if } q+2\leq j<(l+1)q \text{ and } j\equiv 0\pmod q, \\ (l+2)q+2-j, &\text{if } q+2\leq j<(l+1)q \text{ and } j\equiv 1\pmod q, \\ 1, &\text{if } j=(l+1)q, \\ (2l+3)q-j, &\text{if } (l+1)q<j<(l+2)q, \\ q+1, &\text{if } j=(l+2)q. \end{cases} \end{align*}$$

Let $\mathcal {E}_y$ be the indecomposable parity sheaf supported on the Schubert variety $X_y$ with coefficients in $\mathbb {F}_p$ , extending the constant sheaf shifted by $\dim (X_y)$ . Our theorem is the following.

Theorem 2.1.

$$\begin{align*}\mathcal{E}_y\not\cong {^p}\tau_{\leq l-3}(\mathcal{E}_y). \end{align*}$$

Here, ${^p}\tau _{\leq l-3}$ is the perverse truncation operator. Since $l\geq 3$ , this implies that $\mathcal {E}_y$ is not perverse.

3 Intersection forms

If A is an indecomposable object in a Krull–Schmidt category and X is any object, write $m(A,X)$ for the number of times A appears as a direct summand of X.

Our main tool is the following result, which computes the multiplicities of a direct summand via the rank of a bilinear form.

Proposition 3.1 [Reference Juteau, Mautner and WilliamsonJMW, Prop. 3.2].

Let k be a local ring. Let $\pi \,{:}\,\widetilde {Y}\!\longrightarrow \!Y$ be a proper resolution of singularities. Let $y\in Y$ , and suppose that the fiber $F=\pi ^{-1}(y)$ is smooth. Write i for the inclusion of y in Y. Let n be the dimension of $\widetilde {Y}$ , let d be the dimension of F, and let m be an integer. Let B be the pairing

(3.1) $$ \begin{align} H^{2d-n-m}(F)\times H^{2d-n+m}(F) \to H^{2d}(F) \end{align} $$

given by $B(\alpha ,\beta )=\alpha \cup \beta \cup e$ , where e is the Euler class of the normal bundle to F in Y. Then

$$\begin{align*}m(i_*\underline{k}[m],\pi_*\underline{k}[n])=\operatorname{rank}(B). \end{align*}$$

Proof. By general results about multiplicities of indecomposable objects in Krull–Schmidt categories, the multiplicity $m(i_*\underline {k}[m],\pi _*\underline {k}[n])$ is equal to the rank of the pairing

(3.2) $$ \begin{align} \operatorname{Hom}(i_*\underline{k}[m],\pi_*\underline{k}_{\widetilde{Y}}[n])\times \operatorname{Hom}(\pi_*\underline{k}_{\widetilde{Y}}[n],i_*\underline{k}[m])\to \operatorname{End}(i_*\underline{k}[m])\cong k. \end{align} $$

The following commutative diagram appears in the proof of [Reference Juteau, Mautner and WilliamsonJMW, Lem. 3.4] and arises through applying base change and adjunctions. The pairing $B'$ arises through composition with the canonical map from $\omega _F[-n]$ to $\underline {k}_F[n]$ (which comes from applying the canonical natural transformation $i^!\to i^*$ to $\underline {k}_{\widetilde {Y}}$ ), whereas the pairing (3.2) appears along the bottom row.

Since F is smooth, $\omega _F\cong \underline {k}_F[2d]$ and the canonical morphism from $\omega _F[-n]$ to $\underline {k}_F[n]$ is identified with the Euler class e. Therefore, the pairing (3.2) is identified with the one stated in the proposition, completing the proof.

4 Geometry

Let x be the permutation

where J is the $q\times q$ antidiagonal matrix.

We compute the slice to the Schubert variety $X_x$ in $X_y$ through the point x. Using the techniques discussed in the proof of [Reference WilliamsonW, Prop. 3.2], this is given by matrices of the form

subject to the conditions

(4.1) $$ \begin{align} B_i J A_i=0, \quad \operatorname{rank}\begin{pmatrix} A_l \\ \vdots \\ A_1 \end{pmatrix}\leq 1, \quad \operatorname{rank}\begin{pmatrix} B_1 & \cdots & B_l \end{pmatrix}\leq 1 \end{align} $$

for all i. Here, each $A_i$ and $B_i$ is a $q\times q$ matrix. Let Y be this slice. So Y is the space of all $(2l)$ -tuples of $q\times q$ matrices $A_1,\ldots ,A_l,B_1,\ldots B_l$ subject to the conditions (4.1).

Let

$$ \begin{align*} &\ \ \widetilde{Y}=\{ (h,\ell_1,\ldots,\ell_l,\ell,A_1,\ldots,A_l,C_1,\ldots,C_l)\mid h\in Gr(q-1,q), \\ &\ell_1,\dots,\ell_l,\ell\in Gr(1,q), A_i\in \operatorname{Hom}(\mathbb{C}^q/h,\ell_i),B_i\in \operatorname{Hom}(\mathbb{C}^q/\ell_i,\ell) \} \end{align*} $$

and $\pi \,{:}\,\widetilde {Y}\!\longrightarrow \!Y$ be defined by

(4.2) $$ \begin{align} \pi(h,\ell_1,\ldots,\ell_l,\ell,A_1,\ldots,A_l,C_1,\ldots,C_l)=(A_1,\ldots,A_l,C_1J,\ldots,C_lJ). \end{align} $$

This is a resolution of singularities of Y, and $\widetilde {Y}$ is the total space of a vector bundle $\mathcal {E}$ on $Z:=(\mathbb {P}^{q-1})^{l+2}$ .

We have

$$\begin{align*}H^*(Z) \cong \mathbb{Z}[w]/(w^q)\otimes ( \bigotimes_{i=1}^l \mathbb{Z}[a_i]/(a_i^q) )\otimes \mathbb{Z}[z]/(z^q), \end{align*}$$

where the variables w and z come from the factors of Z corresponding to the choices of h and $\ell $ in $\widetilde {Y}$ , respectively, whereas the $a_i$ come from the choice of $\ell _i$ .

Lemma 4.1. The Euler class of $\mathcal {E}$ is given by

(4.3) $$ \begin{align} e(\mathcal{E}) =\prod_{i=1}^l \left((a_i+w)\sum_{j=0}^{q-1}a_i^j z^{q-1-j}\right). \end{align} $$

Proof. The bundle $\mathcal {E}$ is naturally a direct sum of $2l$ vector bundles

$$\begin{align*}\mathcal{E}\cong \bigoplus_{i=1}^l \mathcal{A}_i \oplus \bigoplus_{i=1}^l \mathcal{C}_i, \end{align*}$$

where the bundles $\mathcal {A}_i$ and $\mathcal {C}_i$ correspond to the choice of $A_i$ and $C_i$ in $\widetilde {Y}$ . The bundle $\mathcal {A}_i$ is a line bundle with first Chern class $a_i+w$ .

On $\mathbb {P}^{q-1}$ , write $\mathcal {L}$ for the tautological line bundle, and $\mathcal {T}$ for the trivial vector bundle of rank q. Then, restricted to the appropriate $\mathbb {P}^{q-1}\times \mathbb {P}^{q-1}$ , we have

$$\begin{align*}\mathcal{C}_i\cong p_1^*(\mathcal{T}/\mathcal{L})^* \otimes p_2^* \mathcal{L}. \end{align*}$$

The total Chern class of $(\mathcal {T}/\mathcal {L})^*$ is given by

$$\begin{align*}c((\mathcal{T}/\mathcal{L})^*)=\sum_{j=1}^\infty a_i^j. \end{align*}$$

The computation of $e(\mathcal {C}_i)$ proceeds via (4.4), whose proof follows easily using the splitting principle:

Let V be a rank n vector bundle, and let L be a line bundle. Then

(4.4) $$ \begin{align} e(V\otimes L)=\sum_{i=0}^n c_i(V) c_1(L)^{n-i}. \end{align} $$

Using this, we obtain

$$\begin{align*}e(\mathcal{C}_i)=\sum_{j=0}^{q-1}a_i^j z^{q-1-j}. \end{align*}$$

Together with the formula for the Euler class (=first Chern class) of $\mathcal {A}_i$ , this implies the formula in the lemma.

Motivated by Proposition 3.1, we consider the pairing

$$\begin{align*}\langle \cdot,\cdot\rangle \,{:}\,H^{2(q-l)}(Z)\times H^{2(q-2)}(Z)\!\longrightarrow\!H^{2(l+2)(q-1)}(Z) \end{align*}$$

given by

$$\begin{align*}\langle \sigma,\tau\rangle = \sigma \cup \tau \cup e(\mathcal{E}). \end{align*}$$

The ring $H^*(Z)$ has a basis consisting of monomials in the variables $w,a_i,z$ , where the exponent of each variable is less than q. When computing the intersection pairing $\langle \cdot ,\cdot \rangle $ between two of these monomials in $H^*(Z)$ , one notices that it only depends on the power of w in their product. If this power is j, then the pairing takes the value ${l \choose q-1-j}$ , for this is the number of ways of choosing terms in the product formula (4.3) for $e(\mathcal {E})$ which produce the right power of w, and once these choices are made, the rest are uniquely determined.

Deleting duplicate rows that are irrelevant for computing the rank, the matrix for our intersection form with respect to the monomial basis becomes

(4.5) $$ \begin{align} M= \left(\begin{array}{cccccccccccc} l & {l \choose 2} & {l \choose 3} & \cdots & & l & 1 & & & & \\[3pt] 1 & l & {l \choose 2} & {l \choose 3} & \cdots & & l & 1 & & & \\ & 1 & l & {l \choose 2} & & & & \ddots & \ddots & & \\ & & \ddots & \ddots & \ddots & & & & l & 1 & \\ & & & 1 & l & {l \choose 2} & \cdots & && l & 1 \\ & & & & 1 & l & {l \choose 2} & \cdots && & l \end{array} \right). \end{align} $$

This matrix has $q-1$ columns, corresponding to the powers of w between $0$ and $q-2$ inclusive that appear in $H^{2(q-2)}(Z)$ and $q-l+1$ rows, corresponding to the powers of w between $0$ and $q-l$ inclusive that appear in $H^{2(q-l)}(Z)$ .

5 Reduction to the slice

This section is likely to be of independent interest. We require the following result about direct summands of a pushforward sheaf. The same proof works when k is a local ring, but for simplicity we assume that k is a field.

Theorem 5.1. Let X be an irreducible complex analytic space. Let k be a field. Then there exists a unique indecomposable object $\mathcal {E}(X;k)\in D^b_c(X;k)$ which restricts to the constant sheaf shifted by $\dim X$ on an open subset of X, and is a direct summand of $\sigma _*\underline {k}_Y[\dim X]$ for any proper resolution of singularities $\sigma :Y\to X$ .

Proof. Let $\sigma :Y\to X$ and $\pi :Z\to X$ be two proper resolutions of singularities. Consider $\operatorname {Hom}(\sigma _*\underline {k}_Y,\pi _*\underline {k}_Z)\cong H^{BM}_{2d}(Y\times _X Z)$ , where $H^{BM}_*$ stands for Borel–Moore homology and $d=\dim _{\mathbb {C}}(X)$ . Let U be a connected open dense subset of X such that $\sigma $ and $\pi $ are isomorphisms over U. Write $j:U\to X$ for the inclusion. As $\sigma $ and $\pi $ are isomorphisms over U, there is a canonical inclusion of U into $Y\times _X Z$ . The closure $\overline U$ of U in $Y\times _XZ$ is an irreducible component of $Y\times _XZ$ , and hence defines a fundamental classFootnote 2 $\alpha :=[\overline {U}]\in H^{BM}_{2d}(Y\times _XZ)\cong \operatorname {Hom}(\sigma _*\underline {k}_Y,\pi _*\underline {k}_Z)$ . This class satisfies $j^*\alpha =\mbox {id}\in \operatorname {Hom}(\underline {k}_U,\underline {k}_U)$ .

Similarly, we define $\beta \in \operatorname {Hom}(\pi _*\underline {k}_Z,\sigma _*\underline {k}_Y)$ with $j^*\beta =\mbox {id}\in \operatorname {Hom}(\underline {k}_U,\underline {k}_U)$ .

The category $D^b_c(X;k)$ is Krull–Schmidt. Therefore, since $\underline {k}_U$ is indecomposable and $j^*(\sigma _*\underline {k}_Y)\cong \underline {k}_U$ , we can write $\sigma _*\underline {k}_Y\cong A\oplus C$ where A is indecomposable and $j^*C=0$ . Similarly, we have $\pi _*\underline {k}_Z\cong B\oplus D$ with B indecomposable and $j^*D=0$ . Using these direct sum decompositions, consider the components of $\alpha $ and $\beta $ . They induce morphisms which by abuse of notation we call $\alpha :A\to B$ and $\beta :B\to A$ .

Consider $\beta \alpha \in \operatorname {End}(A)$ . Under the ring homomorphism $j^*:\operatorname {End}(A)\to \operatorname {End}(\underline {k}_U)\cong \underline {k}$ , we have $j^*(\beta \alpha )=1$ . As A is indecomposable, $\operatorname {End}(A)$ is local. This implies that $\beta \alpha $ is a unit in $\operatorname {End}(A)$ . Similarly, $\alpha \beta $ is a unit in $\operatorname {End}(B)$ . We thus have two indecomposable objects A and B, with morphisms between them $\alpha $ and $\beta $ , whose compositions in each direction are isomorphisms. This is enough to conclude $A\cong B$ . This completes the proof, with $\mathcal {E}(X;k)=A[\dim X]$ . Note that $\mathcal {E}(X;k)$ always exists because a resolution of singularities always exists.

Remark 5.2. For a Schubert variety $X_y$ , the sheaf $\mathcal {E}(X_y;\mathbb {F}_p)$ is the same as the parity sheaf $\mathcal {E}_y$ , by considering a Bott–Samelson resolution of $X_y$ [Reference Juteau, Mautner and WilliamsonJMW, Prop. 4.11].

Now, we show how to use this result to restrict our attention to slices. Let X be an irreducible complex analytic space. Let $Z\subset X$ be a closed analytic subset. Let Y be a slice to Z in X. This implies that there exists an open subset $U\subset X$ and smooth V such that $U\cong Y\times V$ and under this isomorphism the copy of Y in X gets sent to $Y\times \{v\}$ for some $v\in V$ .

Let $Y'\to Y$ be a resolution of Y. Then $Y'\times V\to U$ is a resolution of U. The sheaf $\mathcal {E}(Y;k)\boxtimes \underline {k}_V[\dim V]$ on U is an indecomposable direct summand of the pushforward of the shifted constant sheaf under this resolution which is generically constant, and hence by the above theorem is isomorphic to $\mathcal {E}(U;k)$ .

Let $j\,{:}\,U\!\longrightarrow \!X$ denote the inclusion. Pulling back a resolution of X to U via j shows that $\mathcal {E}(U;k)$ is a direct summand of $j^\ast \mathcal {E}(X;k)$ .

Therefore, $\mathcal {E}(Y;k)\boxtimes \underline {k}_V[\dim V]$ is a direct summand of $j^\ast \mathcal {E}(X;k)$ . So, if we can show that $\mathcal {E}(Y;k)\not \cong {}^p\tau _{\leq l-3}(\mathcal {E}(Y;k))$ , then that will imply that $\mathcal {E}(X;k)\not \cong {}^p\tau _{\leq l-3}(\mathcal {E}(X;k))$ . This is the method by which we can restrict our attention to the slice.

6 Fin

Lemma 6.1. The matrix M from (4.5) has rank $q-l+1$ over $\mathbb {Q}$ and $q-l$ over $\mathbb {F}_p$ .

Proof. Identify the rows of M with the sequence of polynomials

$$ \begin{align*} &(1+x)^l-1 \\ x&(1+x)^l \\ x^2&(1+x)^l \\ & \vdots \\ x^{q-l-1}&(1+x)^l \\ x^{q-l}&(1+x)^l -x^q. \end{align*} $$

If there is a linear dependence, then $A+Bx^q$ is divisible by $(1+x)^l$ for some constants A and B. Over $\mathbb {Q}$ , this is impossible since $A+Bx^q$ has distinct roots over $\mathbb {C}$ . This computes the rank over $\mathbb {Q}$ .

Over $\mathbb {F}_p$ , the polynomial $(1+x)^l$ divides $x^q+1$ , which easily leads to a linear dependence among the rows of M. It is obvious that the rank is at least $q-l$ , completing the proof in this case.

Recall the resolution $\pi \,{:}\,\widetilde {Y}\!\longrightarrow \!Y$ defined in §4. Let $Z=\widetilde {Y}\times _Y\widetilde {Y}.$

Lemma 6.2. The Borel–Moore homology groups $H_i^{BM}(Z;\mathbb {Z})$ are free over $\mathbb {Z}$ and vanish when i is odd.

Proof. The variety Z is

$$ \begin{align*} Z&=\{(A_1,\ldots,A_l,B_1,\ldots,B_l,h,h',\ell_1,\ldots,\ell_l,\ell_1'\ldots\ell^{\prime}_l,\ell,\ell')\mid \\ &\quad A_i,B_i\in \operatorname{Hom}(\mathbb{C}^q,\mathbb{C}^q);\ h,h'\in Gr(q-1,q);\ \ell_1,\ldots,\ell_l,\ell_1'\ldots\ell^{\prime}_l,\ell,\ell'\in Gr(1,q); \\ &\qquad\qquad\qquad\qquad\qquad\qquad h,h'\subset \ker(A_i);\ \operatorname{im}(A_i)\subset \ell_i,\ell_i'\subset \ker B_i;\ \operatorname{im}(B_i)\subset \ell,\ell' \}. \end{align*} $$

We now construct a stratification of Z. For each $I\subset \{1,2,\ldots ,l\}\sqcup \{s,t\}$ , we define a stratum $Z_I$ consisting of tuples $(A_1,\ldots ,A_l,B_1,\ldots ,B_l,h,h',\ell _1,\ldots ,\ell _l,\ell _1'\ldots \ell ^{\prime }_l,\ell ,\ell ')\in Z$ subject to the conditions $\ell _i=\ell _i'$ if $i\in I$ , $h=h'$ if $s\in I$ , $\ell =\ell '$ if $t\in I$ , $\ell _i\neq \ell _i'$ if $i\notin I$ , $h\neq h'$ if $s\notin I$ , and $\ell \neq \ell '$ if $t\notin I$ .

Each stratum $Z_I$ is a vector bundle over a product of spaces that are either $\mathbb {P}^{q-1}$ or $(\mathbb {P}^{q-1}\times \mathbb {P}^{q-1})\setminus \Delta $ , where $\Delta $ is the diagonal. Therefore, $H_i^{BM}(Z_I;\mathbb {Z})$ is free over $\mathbb {Z}$ and vanishes when i is odd. Since the $Z_I$ stratify Z, the same is true for the Borel–Moore homology of Z.

Reimagine Y as a subspace of the space of representations of the following quiver Q, where there are l vertices in the central column.

The representations have dimension vector:

The group $G=GL_q(\mathbb {C})^{l+2}$ acts on Y in a manner such that $[Y/G]$ is a substack of the moduli stack of representations of Q.

Lemma 6.3. The map $\pi \,{:}\,\widetilde {Y}\!\longrightarrow \!Y$ defined in (4.2) is a proper evenFootnote 3 G-equivariant resolution of singularities, stratified with respect to a stratification $Y=\sqcup Y_\lambda $ such that $H^*_G(Y_\lambda ;\mathcal {L})$ vanishes in odd degrees for all G-equivariant local systems $\mathcal {L}$ on $Y_\lambda $ .

Remark 6.4. This lemma allows us to have access to the parity sheaf machinery from [Reference Juteau, Mautner and WilliamsonJMW] for G-equivariant sheaves on Y.

Proof. Let I and J be two subsets of $\{1,2,\ldots ,l\}$ . Let

(6.1) $$ \begin{align} Y_{I,J}=\{(A_1,\ldots,A_l,B_1,\ldots,B_l)\in Y\mid A_i=0 \iff i\in I,\ B_j=0\iff j\in J\}. \end{align} $$

This is the stratification of Y into G-orbits. We show that this gives the desired stratification of Y. In the moduli interpretation of Y, inside each G-orbit, there is a unique representation $M_{IJ}$ of Q, up to isomorphism.

The module $M_{IJ}$ decomposes as a direct sum $M_{IJ}=X_I\oplus Y_J\oplus Z$ , where $X_I$ is an indecomposable with dimension 1 at the leftmost vertex, $Y_J$ is an indecomposable with dimension 1 at the rightmost vertex, and Z is a direct sum of simple modules, except when $I=\{1,2,\ldots ,l\}$ or $J=\{1,2,\ldots ,l\}$ , when $X_I$ or $Y_J$ , respectively, do not appear in the decomposition.

Put an order on these indecomposables where the simple at the leftmost vertex comes earliest in the order, then $X_I$ , then the simples at the middle vertices, then $Y_J$ , then the simple at the rightmost vertex. With this ordering, we can decompose $M_{IJ}$ into indecomposables, $M_{IJ}=\oplus _{i=1}^m M_i^{\oplus n_i}$ where $\operatorname {Hom}_Q(M_i,M_j)=0$ if $i<j$ .

Therefore, $\operatorname {End}_Q(M_{IJ})^\times $ surjects onto $\prod _i \operatorname {Mat}_{n_i}(\operatorname {End}_Q(M_i))^\times $ with unipotent kernel. Each $\operatorname {End}_Q(M_i)$ is isomorphic to $\mathbb {C}$ .

The quotient stack $[Y_{IJ}/G]$ is isomorphic to $[\mathrm {pt}/\operatorname {End}_Q(M_{IJ})^\times ]$ . This shows that $H^*_G(Y_{IJ};\mathcal {L})$ is a free k-module and vanishes in odd degrees since these properties hold for the stack $[\mathrm {pt}/GL_n(\mathbb {C})]$ .

It is clear that $\pi $ is a proper G-equivariant resolution of singularities, and thus is stratified for the stratification into G-orbits. It is even because every fiber of $\pi $ is a product of projective spaces.

We now come to the proof of Theorem 2.1.

Proof. Let $n=(q-1)(l+2)+ql$ be the common dimension of Y and $\widetilde {Y}$ . Decompose $\pi _*\underline {\mathbb {Z}}_p[n]$ into indecomposables

$$\begin{align*}\pi_*\underline{\mathbb{Z}}_p[n]\cong \bigoplus_t \mathcal{E}_t^{n_t}. \end{align*}$$

The endomorphism ring of $\pi _*\underline {\mathbb {Z}}_p[n]$ is $\operatorname {End}(\pi _*\underline {\mathbb {Z}}_p[n])\cong H_{2n}^{BM}(Z;\mathbb {Z}_p)$ , which governs the decomposition into irreducibles.

The spectral sequence with $E_2^{p,q}=H^p(BG;H_{-q}^{BM}(Z))$ converges to the G-equivariant Borel–Moore homology $H_*^G(Z)$ . This spectral sequence is concentrated in even degrees by Lemma 6.2 and hence degenerates at the $E_2$ page. Therefore, $H_{2n}^G(Z)$ surjects onto $H_{2n}^{BM}(Z)$ . As a consequence, each $\mathcal {E}_t$ is the deequivariantization of an indecomposable G-equivariant sheaf, which is an equivariant parity sheaf by Lemma 6.3.

Again by Lemma 6.2, the convolution algebra $H_{2n}^{BM}(Z;\mathbb {Z}_p)$ surjects onto $H_{2n}^{BM}(Z;\mathbb {F}_p)$ . Therefore, each $\mathcal {E}_t\otimes \mathbb {F}_p$ is also indecomposable.

Let i be the inclusion of $\{0\}$ in Y. By Proposition 3.2 and Lemma 6.1, the multiplicity of $i_*\underline {k}[l-2]$ in $\pi _*\underline {k}[n]$ is $q-l+1$ when $k=\mathbb {Q}_p$ and $q-l$ when $k=\mathbb {F}_p$ . Therefore, there exists a unique t such that

(6.2) $$ \begin{align} m(i_*\underline{\mathbb{Q}}_p[l-2],\mathcal{E}_t\otimes \mathbb{Q}_p)=1 \end{align} $$

and $\mathcal {E}_t$ is not a skyscraper sheaf at 0.

This setup is symmetric under the action of the symmetric group $S_l$ which permutes the indices $\{1,2,\ldots ,l\}$ of elements of Y. So, by uniqueness of t, $\mathcal {E}_t$ is $S_l$ -invariant. From the classification of equivariant parity sheaves in [Reference Juteau, Mautner and WilliamsonJMW], $\mathcal {E}_t$ is up to homological shift the parity extension of a constant sheaf on an $S_l$ -invariant G-orbit on Y.

There are only two $S_l$ -invariant intermediate G-orbits in Y. They are $Y_{\{1,2,\ldots ,l\},\emptyset }$ and $Y_{\emptyset ,\{1,2,\ldots ,l\}}$ in the notation of (6.1).

Let W be the closure of $Y_{\{1,2,\ldots ,l\},\emptyset }$ . Let us assume that $\mathcal {E}_t$ has support W. Define

$$\begin{align*}\widetilde{W}=\{(\ell,B_1,B_2,\ldots ,B_l)\mid \ell\in Gr(1,q), B_i\in \operatorname{Hom}(\mathbb{C}^q,\ell)\}. \end{align*}$$

Write $\sigma $ for the map from $\widetilde {W}$ to ${W}$ . This is a G-equivariant even resolution of singularities. Therefore, in the G-equivariant derived category, $\mathcal {E}_t$ must appear as a direct summand of $\sigma _*\underline {\mathbb {Z}}_p$ (up to homological shift) as it is the unique indecomposable G-equivariant parity sheaf extending the constant sheaf and thus the same statement holds when we forget the equivariant structure.

The space $\widetilde {W}$ is the total space of a vector bundle $\mathcal {F}\cong \mathcal {O}(1)^{\oplus lq}$ over $\mathbb {P}^{q-1}$ , where the zero section is the fiber over $0\in Y$ . The Euler class $e(\mathcal {F})$ is a power of the Chern class $c_1(\mathcal {O}(1))$ . In computing the intersection form (3.1) for the resolution $\sigma $ , once irrelevant rows are deleted, one is left with the antidiagonal matrix J, which has the same rank over $\mathbb {Q}$ and $\mathbb {F}_p$ .

Since the rank does not change, we deduce that $m(i_*\underline {\mathbb {Q}} _p[l-2],\mathcal {E}_t\otimes \mathbb {Q}_p)=0$ , contradicting (6.2). Therefore, $\mathcal {E}_t$ cannot have support equal to W.

Similarly, $\mathcal {E}_t$ cannot have support equal to the closure of the other $S_l$ -equivariant intermediate stratum $Y_{\emptyset ,\{1,2,\ldots ,l\}}$ .

Therefore, $\mathcal {E}_t$ is an extension of the shifted constant sheaf on the open stratum in Y. As the stalk of $\mathcal {E}_t$ at 0 is free over $\mathbb {Z}_p$ and satisfies a parity vanishing property, it is nonzero in degree $l-2$ using (6.2). Therefore, $\mathcal {E}_t\otimes \mathbb {F}_p$ has nonzero stalk cohomology at 0 in degree $l-2$ . Thus,

$$\begin{align*}\mathcal{E}_t\otimes \mathbb{F}_p \not \cong {{}^p\tau}_{\leq l-3}(\mathcal{E}_t\otimes \mathbb{F}_p). \end{align*}$$

Since $\mathcal {E}_t\otimes \mathbb {F}_p$ is an indecomposable extension of the shifted constant sheaf on the open stratum on Y and occurs as a summand of $\pi _*\underline {\mathbb {F}_p}[n]$ , by Theorem 5.1, $\mathcal {E}_t\otimes \mathbb {F}_p\cong \mathcal {E}(Y;\mathbb {F}_p)$ . By the reduction to the slice argument made in the previous section, this completes the proof of Theorem 2.1.

Acknowledgment

I would like to thank an anonymous referee whose diligent reading of this manuscript has resulted in a much improved exposition.

Footnotes

1 $D^b_c(X;k)$ is the bounded derived category of constructible sheaves on X with coefficients in k. We always work with the classical metric topology on X.

2 The definition of fundamental class is the same as in the algebraic case [Reference Chriss and GinzburgCG, §2.6.12], using the fact that the singular locus is of real codimension at least 2.

3 The definition of an even morphism is given in [Reference Juteau, Mautner and WilliamsonJMW, Def. 2.33]. A sufficient condition that implies evenness is that each fiber is equivariantly simply connected with no odd cohomology.

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