Proposition II and proof
Click a dotted symbol or a label such as H5 to recall its definition. This page checks H1–H5 by hand in the group case \(G=H\times H\); Proposition III decides them for every symmetric space.
Definitions
Symmetric space
Work over \(k=\mathbb C\) with complex coefficients. Fix a connected reductive group \(G\) and an involution \(\theta\) of \(G\) whose fixed subgroup \(G^\theta\) is connected.
$$X=G/G^\theta,\qquad x_0=eG^\theta.$$Two tori, two jobs. \(T\) belongs to the group: its dominant cocharacters label the Satake sheaves. \(S\subseteq T\) belongs to the space: its dominant cocharacters label the orbits on \(LX\) (see the index sets).
The θ-split torus \(S\). A torus is θ-split when \(\theta\) inverts it, and \(S\) is a maximal one. All such are \(G^\theta\)-conjugate, and their dimension is the rank of \(X\). \(S\) is the torus that \(X\) sees: the Cartan embedding \(\tau\) lands in the elements that \(\theta\) inverts, and each orbit has a representative with \(\tau(x_\mu)=t^\mu\in S(F)\).
$$\theta(s)=s^{-1}\quad(s\in S),\qquad\dim S=\operatorname{rank}X.$$The maximal torus \(T\). \(T\) is a maximal torus of \(G\) that contains \(S\) and is θ-stable. \(\theta\) splits it into a fixed part and the split part, which is \(S\):
$$S=\{t\in T:\theta(t)=t^{-1}\}^\circ,\qquad T=(T^\theta)^\circ\cdot S.$$Positive roots. A Borel \(B\supseteq T\) inside a minimal θ-split parabolic \(P\) fixes the positive roots \(\Phi^+\). The Levi \(L\) centralizes \(S\).
$$P\cap\theta(P)=L=Z_G(S).$$Loops and arcs. Loop spaces use Laurent series \(F=k(\!(t)\!)\) and arc spaces power series. The arc group \(L^+G\) acts on the loop space \(LX\).
$$LX(k)=X(F),\qquad L^+X(k)=X(k[\![t]\!]).$$Examples. In the group case \(G=H\times H\), \(\theta(g_1,g_2)=(g_2,g_1)\), and \(T_H\) is a maximal torus of \(H\). In \(\mathrm{GL}_2/\mathrm{Sp}_2\), \(\theta(g)=g/\det g\) (worked out here).
Table 1. \(X\) and \(T\) and \(S\) \(X\) \(T\) \(S\) \(\operatorname{rank}X\) \((H\times H)/H\) \(T_H\times T_H\) \(\{(s,s^{-1}):s\in T_H\}\) \(\operatorname{rank}H\) \(\mathrm{GL}_2/\mathrm{Sp}_2\) \(\{\operatorname{diag}(t_1,t_2)\}\) \(\{\operatorname{diag}(a,a)\}\) \(1\) The group case and its dictionary
The factor \(H\). \(H\) is a connected reductive group over \(k\) with maximal torus \(T_H\), Borel subgroup \(B_H\supseteq T_H\), opposite Borel subgroup \(B_H^-\), positive roots \(\Phi_H^+\), simple coroots \(\alpha_1^\vee,\dots,\alpha_r^\vee\), half-sum of positive roots \(\rho_H\) and longest Weyl element \(w_0\). Its cocharacters carry the dominance order:
$$\Lambda_H=X_*(T_H),\qquad\Lambda_H^+=\{\eta\in\Lambda_H:\langle\alpha,\eta\rangle\ge0\ \text{for all }\alpha\in\Phi_H^+\},\qquad\eta'\le_H\eta\iff\eta-\eta'\in\textstyle\sum_i\mathbb Z_{\ge0}\,\alpha_i^\vee.$$The affine Grassmannian of \(H\). \(p\) is the quotient map. For \(\eta\in\Lambda_H^+\), the Schubert cell \(\operatorname{Gr}_H^\eta\) is the \(L^+H\)-orbit of \(t^\eta\), the Schubert variety \(\operatorname{Gr}_H^{\le\eta}\) is its closure, and \(\mathrm{IC}^H_\eta\) is the intersection complex of \(\operatorname{Gr}_H^{\le\eta}\), normalized to be perverse:
$$p:LH\longrightarrow\operatorname{Gr}_H=LH/L^+H,\qquad\operatorname{Gr}_H^\eta=L^+H\,t^\eta L^+H/L^+H,\qquad\mathrm{IC}^H_\eta\big|_{\operatorname{Gr}_H^\eta}\simeq\underline k[\langle2\rho_H,\eta\rangle].$$\(\star\) is convolution of \(L^+H\)-equivariant complexes on \(\operatorname{Gr}_H\). Its unit is \(\mathrm{IC}^H_0\), the constant sheaf on the point \(\operatorname{Gr}_H^0\).
Jet groups. The arc group is the limit of the jet groups, and the kernels \(K_n\) are pro-unipotent:
$$J_nH=H\big(k[t]/(t^n)\big),\qquad L^+H=\varprojlim_nJ_nH,\qquad K_n=\ker\big(L^+H\to J_nH\big).$$Dictionary. Unadorned symbols are those of H1–H5 for \(G=H\times H\); an orbit label is written \(\mu=(\mu_H,-\mu_H)\). Step 1 proves each row.
Table 2. For \(G=H\times H\), as in H1–H5 and On the affine Grassmannian of \(H\) For \(G=H\times H\), as in H1–H5 On the affine Grassmannian of \(H\) \(X=G/G^\theta\), base point \(x_0\) \(H\) with \((g_1,g_2)\cdot x=g_1xg_2^{-1}\), base point \(e\) \(L^+G\) acting on \(LX\) \(L^+H\times L^+H\) acting on \(LH\) \(\lambda=(\lambda_1,\lambda_2)\in\Lambda_T^+\) \(\lambda_1\in\Lambda_H^+\), \(-\lambda_2\in\Lambda_H^+\) \(\mu=(\mu_H,-\mu_H)\in\Lambda_S^+\) \(\mu_H\in\Lambda_H^+\) \(\nu\le\mu\) \(\nu_H\le_H\mu_H\) \(\mathcal O_\mu\) and \(\overline{\mathcal O_\mu}\) \(p^{-1}(\operatorname{Gr}_H^{\mu_H})\) and \(p^{-1}(\operatorname{Gr}_H^{\le\mu_H})\) \(\mathcal C\) \(\operatorname{Shv}_{\mathrm{cons}}(L^+H\backslash\operatorname{Gr}_H)\), via \(p^*\) \(V_\lambda\ast\mathrm{IC}_0\) \(\mathrm{IC}^H_{\lambda_1}\star\mathrm{IC}^H_{-\lambda_2}\) Example. Nothing here fixes \(H\). For \(H=\mathrm{GL}_2\), \(\Lambda_H^+=\{(a_1,a_2)\in\mathbb Z^2:a_1\ge a_2\}\); the orbit with \(\mu_H=(a_1,a_2)\) is the double coset of \(\operatorname{diag}(t^{a_1},t^{a_2})\), its Schubert cell has dimension \(a_1-a_2\), and step 6 uses the label \(\lambda=\big((a_1,a_2),(0,0)\big)\).
Two index sets, two roles
Hecke labels. Cocharacters of \(T\) label the Satake sheaves \(V_\lambda\). A dominant \(\lambda\) is a highest weight of the dual group.
$$\Lambda_T=X_*(T),\qquad\Lambda_T^+=\{\lambda\in\Lambda_T:\langle\alpha,\lambda\rangle\ge0\text{ for all }\alpha\in\Phi^+\}.$$Orbit labels. Dominant cocharacters of \(S\) label the arc-group orbits on \(LX\). The Cartan embedding \(\tau\) picks a representative \(x_\mu\) of each orbit (Chen–Yi, Proposition 17).
$$\Lambda_S=X_*(S)\subseteq\Lambda_T,\qquad\Lambda_S^+=\Lambda_S\cap\Lambda_T^+,$$ $$\tau:X\hookrightarrow G,\quad gG^\theta\longmapsto g\theta(g)^{-1},\qquad\tau(x_\mu)=t^\mu,$$ $$LX=\bigsqcup_{\mu\in\Lambda_S^+}\mathcal O_\mu,\qquad\mathcal O_\mu=L^+G\cdot x_\mu.$$The leading-term map. Translating the base point by a Hecke label lands in one orbit, and \(\varphi\) names it.
$$\varphi:\Lambda_T^+\longrightarrow\Lambda_S^+,\qquad\lambda\longmapsto\lambda-\theta(\lambda),$$ $$\tau(t^\lambda x_0)=t^\lambda\theta(t^\lambda)^{-1}=t^{\varphi(\lambda)},\qquad t^\lambda x_0\in\mathcal O_{\varphi(\lambda)}.$$Why the leading-term map is well defined
- For \(t\in T\), \(\theta\) inverts \(t\theta(t)^{-1}\), and the image of \(T\) is connected; so the image lies in \((T^{-\theta})^\circ\), which is \(S\) by maximality of \(S\). On cocharacters the map is \(\lambda\mapsto\lambda-\theta(\lambda)\): $$T\longrightarrow S,\quad t\longmapsto t\theta(t)^{-1},\qquad\lambda-\theta(\lambda)\in\Lambda_S.$$
- Roots of \(L\) vanish on \(S\), and \(T=(T^\theta)^\circ\cdot S\), so \(\theta\) fixes them. Since \(B\subseteq P\) and \(P\cap\theta(P)=L\), the parabolic \(\theta(P)\) is opposite to \(P\), so \(\theta\) sends the roots \(\Phi^+\setminus\Phi_L\) of the unipotent radical of \(P\) to negative roots: $$\theta\alpha=\alpha\quad(\alpha\in\Phi_L),\qquad-\theta\alpha\in\Phi^+\quad(\alpha\in\Phi^+\setminus\Phi_L).$$
- Since \(\langle\alpha,\theta\lambda\rangle=\langle\theta\alpha,\lambda\rangle\), a dominant input gives an output that pairs nonnegatively with every positive root: $$\langle\alpha,\lambda-\theta\lambda\rangle=\begin{cases}0,&\alpha\in\Phi_L^+,\\\langle\alpha,\lambda\rangle+\langle-\theta\alpha,\lambda\rangle\ge0,&\alpha\in\Phi^+\setminus\Phi_L.\end{cases}$$ Therefore the map has the stated domain and codomain: $$\boxed{\varphi:\Lambda_T^+\longrightarrow\Lambda_S^+,\quad\lambda\longmapsto\lambda-\theta(\lambda).}$$
- The Cartan embedding is injective, and \(\tau(t^\lambda x_0)=t^{\varphi(\lambda)}=\tau(x_{\varphi(\lambda)})\). So the translate is the orbit representative: $$t^\lambda x_0=x_{\varphi(\lambda)}\in\mathcal O_{\varphi(\lambda)}.$$
For a symmetric space, H5 forces \(\varphi\) to be onto, and under H3 Proposition III proves the converse. The example page computes \(\varphi\) for the group case of \(\mathrm{SL}_2\), where it is onto, and for \(\mathrm{SL}_2/\mathrm{SO}_2\), where it doubles.
Categories
For an \(L^+G\)-stable locally closed \(W\subseteq LX\), let \(\mathcal C_W\) be the small, idempotent-complete, stable \(\infty\)-category of bounded \(L^+G\)-equivariant constructible complexes on \(W\) with coefficients in \(k\). Proposition I concerns the one on all of \(LX\):
$$\mathcal C=\mathcal C_{LX}=\operatorname{Shv}_{\mathrm{cons}}(L^+G\backslash LX),\qquad\mathcal C_Z=\operatorname{Shv}_{\mathrm{cons}}(L^+G\backslash Z),$$ $$\mathcal C_\mu=\operatorname{Shv}_{\mathrm{cons}}(L^+G\backslash\mathcal O_\mu),\qquad\widehat{\mathcal C}=\operatorname{Ind}(\mathcal C).$$Orbit order and supports
Order \(\Lambda_S^+\) by the dominance order of \(\Lambda_T\):
$$\nu\le\mu\iff\mu-\nu\in\textstyle\sum_{\check\alpha\in\check\Phi^+}\mathbb Z_{\ge0}\,\check\alpha.$$A closed finite union of orbits is a closed \(L^+G\)-stable \(Z\subseteq LX\) that is the union of finitely many orbits. \(I(Z)\) lists its orbits, and \(r_Z\) is its inclusion:
$$I(Z)=\{\mu:\mathcal O_\mu\subseteq Z\},\qquad r_Z:Z\hookrightarrow LX.$$An object \(M\in\mathcal C\) is supported on \(Z\) when the unit of \(r_Z^*\dashv r_{Z*}\) is an isomorphism on \(M\):
$$\operatorname{supp}(M)\subseteq Z\quad:\Longleftrightarrow\quad M\xrightarrow{\ \sim\ }r_{Z*}r_Z^*M.$$Boundary, orbit inclusions and standards
Boundary. The boundary of the orbit \(\mathcal O_\mu\) is its closure minus the orbit. By H1(a) it is the union of the orbits below \(\mu\), a closed finite union of orbits:
$$\overline{\mathcal O_\mu}\setminus\mathcal O_\mu=\bigsqcup_{\nu\lt\mu}\mathcal O_\nu.$$Inclusions. The orbit inclusion \(a_\mu\) is locally closed and the boundary inclusion \(i_\mu\) is closed. Inside a closed finite union \(Z\), the orbit includes by \(a_{\mu,Z}\).
$$a_\mu:\mathcal O_\mu\hookrightarrow LX,\qquad i_\mu:\overline{\mathcal O_\mu}\setminus\mathcal O_\mu\hookrightarrow LX,\qquad a_{\mu,Z}:\mathcal O_\mu\hookrightarrow Z.$$Top and boundary parts. The top part of \(M\in\mathcal C\) restricts it to the orbit and extends by zero. The boundary part restricts it to the boundary and pushes forward:
$$a_{\mu!}a_\mu^*M\ \ \text{(top part)},\qquad i_{\mu*}i_\mu^*M\ \ \text{(boundary part)}.$$Standards. A standard object extends the constant sheaf of an orbit by zero. \(\mathrm{IC}_0\) is the standard of \(\mathcal O_0=L^+X\), the orbit of the base point, which is closed.
$$\Delta_\mu=a_{\mu!}\underline k_{\mathcal O_\mu}\in\mathcal C,\qquad\Delta_{\mu,Z}=a_{\mu,Z!}\underline k_{\mathcal O_\mu}\in\mathcal C_Z,\qquad\mathrm{IC}_0=\Delta_0.$$The constant objects are unshifted; a fixed normalization shift does not affect thick generation.
Thick span
For a set \(\mathcal S\) of objects of a stable \(\infty\)-category \(\mathcal D\), \(\operatorname{Thick}_{\mathcal D}(\mathcal S)\) is the smallest full subcategory that contains \(0\) and \(\mathcal S\) and is closed under isomorphisms, shifts, cofibers and retracts. Two of its properties are used:
$$\text{(T1)}\quad A\to B\to C\xrightarrow{+1}\ \text{exact},\ \ A,C\in\operatorname{Thick}_{\mathcal D}(\mathcal S)\ \Longrightarrow\ B\in\operatorname{Thick}_{\mathcal D}(\mathcal S),$$ $$\text{(T2)}\quad F:\mathcal D\to\mathcal D'\ \text{exact}\ \Longrightarrow\ F\big(\operatorname{Thick}_{\mathcal D}(\mathcal S)\big)\subseteq\operatorname{Thick}_{\mathcal D'}\big(F(\mathcal S)\big).$$Proofs of (T1) and (T2) → · Thick versus the draft's two spans →
Spherical Hecke action
The action uses the contracted product, where the arc group acts on the right on the first factor and on the left on the second.
$$\operatorname{Gr}_G=LG/L^+G,\qquad\mathcal H=\operatorname{Shv}_{\mathrm{cons}}(L^+G\backslash LG/L^+G),$$ $$m:LG\mathbin{\times^{L^+G}}LX\longrightarrow LX,\qquad[g,x]\longmapsto gx,$$ $$\boxed{\ast:\mathcal H\times\mathcal C\longrightarrow\mathcal C,\qquad\mathcal A\ast\mathcal F=m_!(\mathcal A\mathbin{\widetilde\boxtimes}\mathcal F).}$$The twisted external product descends the equivariant external product to the contracted product. Hypothesis H4 requires the result to stay in the constructible category.
Satake objects
Geometric Satake identifies representations of the dual group with spherical perverse sheaves. \(V_\lambda\) is the sheaf of the irreducible representation with highest weight \(\lambda\).
$$\operatorname{Sat}:\operatorname{Rep}_k(\check G)\xrightarrow{\sim}\operatorname{Perv}(L^+G\backslash\operatorname{Gr}_G)\subseteq\mathcal H,\qquad V_\lambda=\operatorname{Sat}(V_\lambda^{\mathrm{rep}}).$$The Satake objects are the convolutions \(V_\lambda\ast\mathrm{IC}_0\), \(\lambda\in\Lambda_T^+\). Chen–Yi (2025), §10.2 defines the spherical action in its sheaf theory; we assume its realization in the category specified here.
Mapping convention
Every Map denotes the full derived mapping complex, with its category as a subscript.
$$\Map_{\mathcal D}:\mathcal D^{\mathrm{op}}\times\mathcal D\longrightarrow D(k),$$ $$\Map_{\mathcal D}(A,B)=0\quad\Longleftrightarrow\quad\operatorname{Hom}_{h\mathcal D}(A,B[n])=0\ \text{ for every }n\in\mathbb Z.$$
Hypotheses H1–H5 of Proposition I
On this page every hypothesis is read for \(G=H\times H\).
H1 · Finite orbit filtration.
- Each orbit closure is the disjoint union of the finitely many orbits below it: $$\overline{\mathcal O_\mu}=\bigsqcup_{\nu\le\mu}\mathcal O_\nu,\qquad\#\{\nu\in\Lambda_S^+:\nu\le\mu\}\lt\infty.$$
- Every object of \(\mathcal C\) is supported on a finite union of orbit closures: $$\forall M\in\mathcal C\ \ \exists J\subseteq\Lambda_S^+\ \text{finite}:\qquad\operatorname{supp}(M)\subseteq\bigcup_{\mu\in J}\overline{\mathcal O_\mu}.$$
H2 · Equivariant recollement.
Let \(D\subseteq Z\) be closed finite unions of orbits and \(\mathcal O_\mu\subseteq Z\) an orbit, with embeddings $$i:D\hookrightarrow Z,\qquad r_Z:Z\hookrightarrow LX,\qquad a_{\mu,Z}:\mathcal O_\mu\hookrightarrow Z.$$- Restriction \(f^*\) and extension by zero \(f_!\) along these embeddings and their composites are defined and exact. For a closed embedding \(f\), the extension \(f_!=f_*\) is right adjoint to \(f^*\).
- If \(\mathcal O_\mu\) is open in \(Z\) with complement \(D\), then \(j=a_{\mu,Z}\) and \(i\) give every \(M\in\mathcal C_Z\) a localization triangle: $$j_!j^*M\longrightarrow M\longrightarrow i_*i^*M\xrightarrow{+1}.$$
- Restriction and extension by zero respect composition: \((fg)^*\simeq g^*f^*\) and \((fg)_!\simeq f_!g_!\).
H3 · Constant coefficients.
Each orbit category has a bounded t-structure whose heart consists of the finite direct sums of the constant sheaf: $$\mathcal C_\mu^\heartsuit\simeq\operatorname{Vect}_k^{\mathrm{fd}},\qquad V\longmapsto\underline k_{\mathcal O_\mu}\otimes_kV.$$ For the ordinary t-structure the heart is \(\operatorname{Rep}^{\mathrm{fd}}_k\big(\pi_0(\operatorname{Stab}_{L^+G}(x_\mu))\big)\) (draft Construction 3.34), so connected stabilizers give H3.H4 · Constructible Hecke action.
The action is defined and takes values in \(\mathcal C\): $$\ast:\mathcal H\times\mathcal C\longrightarrow\mathcal C,\qquad V_\lambda\ast\mathrm{IC}_0\in\mathcal C\quad(\lambda\in\Lambda_T^+).$$H5 · Nonzero top splitting.
Let \(a_\mu:\mathcal O_\mu\hookrightarrow LX\) be the orbit inclusion. For every \(\mu\in\Lambda_S^+\) there is \(\lambda\in\Lambda_T^+\) whose Satake object \(V_\lambda\ast\mathrm{IC}_0\) has two properties:- It lives on the closure of \(\mathcal O_\mu\): $$\operatorname{supp}(V_\lambda\ast\mathrm{IC}_0)\subseteq\overline{\mathcal O_\mu}.$$
- Its restriction to \(\mathcal O_\mu\) is a finite, nonzero sum of shifted constant sheaves: $$a_\mu^*(V_\lambda\ast\mathrm{IC}_0)\simeq\bigoplus_{s=1}^{N_\mu}\underline k_{\mathcal O_\mu}[d_s]\ \text{ in }\mathcal C_\mu,$$ $$0\lt N_\mu\lt\infty,\qquad d_s\in\mathbb Z.$$
Proposition II
Setting. \(H\) is any connected reductive group over \(k=\mathbb C\). The group case is the symmetric space
$$G=H\times H,\qquad\theta(g_1,g_2)=(g_2,g_1),\qquad G^\theta=\{(h,h):h\in H\},\qquad X=G/G^\theta.$$Notation. H1–H5 are statements about \(G=H\times H\): the tori \(T,S\), the labels \(\Lambda_T^+,\Lambda_S^+\), the orbits \(\mathcal O_\mu\), the Satake sheaves \(V_\lambda\) and the Hecke category \(\mathcal H\) all belong to \(G\). An index \(H\) marks an object of the factor \(H\), and the group-case dictionary translates between the two.
Category. \(\mathcal C\) is the category of Proposition I, made explicit: the bounded \(L^+G\)-equivariant constructible complexes on \(LX\) with complex coefficients, each supported on a finite union of orbit closures.
Claim. H1–H5 hold, so Proposition I applies:
$$\boxed{\mathrm{H1}\wedge\cdots\wedge\mathrm{H5}},\qquad\mathcal C^{\mathrm{Sat}}=\mathcal C.$$Sources
References
- Zhu, An introduction to affine Grassmannians and the geometric Satake equivalence, v2: the Cartan decomposition (2.1.2), Proposition 2.1.5 for Schubert cells, their dimension and closures, and (2.1.17) for bounded convolution (steps 1, 2, 5); §5.1 for connected stabilizers and the IC normalization (steps 4, 6); Lemma A.1.4, Remark A.1.7, §A.1.2 and §A.1.4 for equivariant categories, twisted products and the reduction to jet groups (steps 1, 3, 5); the opening of §5 for complex coefficients.
- J. Bernstein and V. Lunts, Equivariant sheaves and functors, Lecture Notes in Math. 1578 (1994), Part I: the equivariant derived category of a variety with an action of an algebraic group, and its functors (step 3).
- A. Beilinson, J. Bernstein and P. Deligne, Faisceaux pervers, Astérisque 100 (1982), §1.4.1: the functors and triangle of an open–closed pair (step 3). Kuijper, v4 (2026), Definition 2.3.4 and Lemma 4.3.3, give the same mechanism for stable \(\infty\)-categories.
- Chen–Yi, v4: Proposition 17 and Theorem 18, of which steps 1–2 are the group case.
References checked 8 October 2026. The reader in D holds located extracts.
Proof
Step 1 proves the dictionary by passing from \(LX\) to the affine Grassmannian of \(H\). Steps 2–6 check H1–H5 one at a time on Schubert varieties, and step 7 applies Proposition I.
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Dividing by the second factor of \(L^+G=L^+H\times L^+H\) turns each object of H1–H5 into an object on \(\operatorname{Gr}_H\):
$$\mathcal C\simeq\operatorname{Shv}_{\mathrm{cons}}(L^+H\backslash\operatorname{Gr}_H),\qquad\mathcal O_\mu=p^{-1}(\operatorname{Gr}_H^{\mu_H}),\qquad V_{(\lambda_1,\lambda_2)}\ast\mathrm{IC}_0\longleftrightarrow\mathrm{IC}^H_{\lambda_1}\star\mathrm{IC}^H_{-\lambda_2}.$$Proof
- Model of \(X\). \((g_1,g_2)G^\theta\mapsto g_1g_2^{-1}\) is a \(G\)-equivariant isomorphism \(X\simeq H\). It turns the action into two-sided multiplication and the Cartan embedding into \(x\mapsto(x,x^{-1})\): $$(g_1,g_2)\cdot x=g_1xg_2^{-1},\qquad\tau(x)=(x,x^{-1}),\qquad LX\simeq LH.$$
- Quotient. The second factor of \(L^+G\) acts freely on \(LH\) by right multiplication, and \(p\) is the quotient, an \(L^+H\)-torsor. So the quotient stacks agree, and pullback along \(p\) is an equivalence (Zhu, Lemma A.1.4(1) and Remark A.1.7): $$L^+G\backslash LX\simeq L^+H\backslash\operatorname{Gr}_H,\qquad p^*:\operatorname{Shv}_{\mathrm{cons}}(L^+H\backslash\operatorname{Gr}_H)\xrightarrow{\ \sim\ }\mathcal C.$$
- Labels. The centralizer of \(S\) is \(T\), so a minimal θ-split parabolic is a Borel subgroup. \(B\) is one, since \(\theta(B)=B_H^-\times B_H\) is opposite to it: $$T=T_H\times T_H,\qquad S=\{(s,s^{-1}):s\in T_H\},\qquad B=B_H\times B_H^-,\qquad\Phi^+=\{(\alpha,0),\,(0,-\alpha):\alpha\in\Phi_H^+\}.$$ Pairing with \(\Phi^+\) gives the two dominant cones: $$\Lambda_T^+=\Lambda_H^+\times(-\Lambda_H^+),\qquad\Lambda_S^+=\{(\mu_H,-\mu_H):\mu_H\in\Lambda_H^+\}.$$
- Order. The positive coroots of \(G\) are \((\alpha^\vee,0)\) and \((0,-\alpha^\vee)\) for \(\alpha\in\Phi_H^+\). So \(\mu-\nu=(\delta,-\delta)\) is a nonnegative sum of them exactly when \(\delta=\mu_H-\nu_H\) is a nonnegative sum of positive coroots of \(H\): $$\nu\le\mu\iff\nu_H\le_H\mu_H.$$
- Orbits. \(\tau(x_\mu)=t^\mu=(t^{\mu_H},t^{-\mu_H})\) and \(\tau(x)=(x,x^{-1})\) give \(x_\mu=t^{\mu_H}\). Its orbit is a double coset, and the Cartan decomposition of \(LH\) (Zhu, (2.1.2)) is the orbit decomposition: $$\mathcal O_\mu=L^+H\,t^{\mu_H}L^+H=p^{-1}(\operatorname{Gr}_H^{\mu_H}),\qquad LH=\bigsqcup_{\mu_H\in\Lambda_H^+}L^+H\,t^{\mu_H}L^+H.$$
- Hecke action. \(\operatorname{Gr}_G=\operatorname{Gr}_H\times\operatorname{Gr}_H\), and \(V_\lambda\) is the intersection complex of the closure of the \(L^+G\)-orbit of \(t^\lambda\). The coordinate \(\lambda_2\) is antidominant, with dominant conjugate \(w_0\lambda_2\): $$V_{(\lambda_1,\lambda_2)}=\mathrm{IC}^H_{\lambda_1}\boxtimes\mathrm{IC}^H_{w_0\lambda_2}.$$ In \(m([(g_1,g_2),x])=g_1xg_2^{-1}\), the first factor convolves on the left and the second on the right after inversion \(g\mapsto g^{-1}\). Inversion carries \(L^+H\,t^\eta L^+H\) to \(L^+H\,t^{-\eta}L^+H\), whose dominant label is \(-w_0\eta\); so \(\mathrm{IC}^H_{w_0\lambda_2}\) becomes \(\mathrm{IC}^H_{-\lambda_2}\). Finally \(\mathrm{IC}_0\), the constant sheaf on \(L^+X=L^+H\), descends to the unit \(\mathrm{IC}^H_0\): $$V_{(\lambda_1,\lambda_2)}\ast\mathrm{IC}_0\longleftrightarrow\mathrm{IC}^H_{\lambda_1}\star\mathrm{IC}^H_0\star\mathrm{IC}^H_{-\lambda_2}=\mathrm{IC}^H_{\lambda_1}\star\mathrm{IC}^H_{-\lambda_2}.$$
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Orbit closures are preimages of Schubert varieties, with finitely many orbits below each:
$$\overline{\mathcal O_\mu}=p^{-1}(\operatorname{Gr}_H^{\le\mu_H})=\bigsqcup_{\nu\le\mu}\mathcal O_\nu,\qquad\#\{\nu\in\Lambda_S^+:\nu\le\mu\}\lt\infty.$$Proof
- Closures. A Schubert variety is the union of the Schubert cells below it (Zhu, Proposition 2.1.5(2)). A torsor is open and surjective, so preimage under \(p\) commutes with closure, and step 1 turns cells into orbits and \(\le_H\) into \(\le\): $$\overline{p^{-1}(\operatorname{Gr}_H^{\mu_H})}=p^{-1}(\operatorname{Gr}_H^{\le\mu_H})=\bigsqcup_{\nu_H\le_H\mu_H}p^{-1}(\operatorname{Gr}_H^{\nu_H})=\bigsqcup_{\nu\le\mu}\mathcal O_\nu.$$
- Finiteness. Write \(\mu_H-\nu_H=\sum_in_i\alpha_i^\vee\) with \(n_i\ge0\). Since \(\langle2\rho_H,\alpha_i^\vee\rangle=2\) and \(\langle2\rho_H,\nu_H\rangle\ge0\), the coefficients are bounded, and the tuple \((n_i)\) determines \(\nu_H\): $$2\textstyle\sum_in_i=\langle2\rho_H,\mu_H-\nu_H\rangle\le\langle2\rho_H,\mu_H\rangle.$$ With the first bullet this is H1(a).
- Supports. Every object of \(\mathcal C\) is supported on a finite union of orbit closures by the definition of \(\mathcal C\), which is H1(b). A retract keeps the bound, and each \(\mathcal C_Z\) is idempotent complete (step 3), so \(\mathcal C\) is idempotent complete, as Proposition I requires.
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A closed finite union of orbits \(Z\) is the preimage of a projective variety \(Z_H\subseteq\operatorname{Gr}_H\), on which the arc group acts through a jet group. There the functors of H2 are the operations of an equivariant derived category, and an open orbit \(j\) with closed complement \(i\) gives the triangle of H2(b):
$$\mathcal C_Z\simeq D^b_{J_nH,c}(Z_H)\quad(n\gg0),\qquad j_!j^*M\longrightarrow M\longrightarrow i_*i^*M\xrightarrow{+1}.$$Proof
Bullets 1–2 replace \(Z\) by a variety of finite type with an action of an algebraic group, bullet 3 uses the operations that exist there, and bullet 4 assembles them over all \(Z\).
- 1 · Model. By step 2, \(Z=p^{-1}(Z_H)\) for a finite union \(Z_H\) of Schubert varieties, a projective variety. For \(n\) large the pro-unipotent kernel \(K_n\) acts trivially on \(Z_H\), so the arc group acts through the jet group (Zhu, §A.1.4): $$L^+H\twoheadrightarrow J_nH=L^+H/K_n,\qquad K_n\ \text{acts trivially on }Z_H.$$
- 2 · The category of \(Z\). Step 1 identifies \(\mathcal C_Z\) with the \(L^+H\)-equivariant complexes on \(Z_H\), which are by definition the \(J_nH\)-equivariant ones of Bernstein–Lunts. Enlarging \(n\) changes nothing, because \(\ker(J_{n'}H\to J_nH)\) is unipotent and acts trivially (Bernstein–Lunts, Part I; Zhu, §A.1.4 for the perverse version): $$\mathcal C_Z\simeq\operatorname{Shv}_{\mathrm{cons}}(L^+H\backslash Z_H)\simeq D^b_{J_nH,c}(Z_H)\simeq D^b_{J_{n'}H,c}(Z_H)\qquad(n'\ge n).$$
- 3 · Operations. In an equivariant derived category, a \(J_nH\)-stable locally closed embedding \(f\) of varieties has exact functors \(f^*,f_!,f_*\) that preserve bounded constructible complexes. They satisfy \(f^*\dashv f_*\), \(f_!=f_*\) for closed \(f\), \((fg)^*\simeq g^*f^*\) and \((fg)_!\simeq f_!g_!\), and an open \(j\) with closed complement \(i\) gives the localization triangle (Bernstein–Lunts, Part I; BBD, §1.4.1). The embeddings of H2 inside \(Z\) are of this kind, since \(p\) carries them to $$p(D)\hookrightarrow Z_H,\qquad\operatorname{Gr}_H^{\mu_H}\hookrightarrow Z_H.$$ This gives H2(a) for \(i\) and \(a_{\mu,Z}\), the triangle of H2(b), and H2(c).
- 4 · Inside \(LX\). \(\mathcal C\) is the union of the \(\mathcal C_Z\) along closed pushforwards, so \(r_{Z*}\) is the inclusion of \(\mathcal C_Z\). For \(M\) supported on a closed finite union \(Z'\supseteq Z\), set \(r_Z^*M=i_{Z\subseteq Z'}^*M\). This does not depend on \(Z'\): for \(Z\subseteq Z'\subseteq Z''\), H2(c) and \(i^*i_*\simeq\mathrm{id}\) for closed \(i\) give $$i_{Z\subseteq Z''}^*\,i_{Z'\subseteq Z''*}\simeq i_{Z\subseteq Z'}^*\,i_{Z'\subseteq Z''}^*\,i_{Z'\subseteq Z''*}\simeq i_{Z\subseteq Z'}^*.$$ The adjunction \(r_Z^*\dashv r_{Z*}\) holds on each \(\mathcal C_{Z'}\), hence on \(\mathcal C\), and \(a_\mu=r_Z\circ a_{\mu,Z}\) is a composite. This completes H2(a).
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The stabilizer of \(x_\mu\) in \(L^+G\) is the stabilizer \(\Gamma_\mu\) of \(t^{\mu_H}\) in \(\operatorname{Gr}_H\). It is connected, so each orbit category has heart \(\operatorname{Vect}^{\mathrm{fd}}_k\):
$$\operatorname{Stab}_{L^+G}(x_\mu)\simeq\Gamma_\mu=L^+H\cap t^{\mu_H}L^+H\,t^{-\mu_H},\qquad\pi_0(\Gamma_\mu)=1,\qquad\mathcal C_\mu^\heartsuit\simeq\operatorname{Vect}^{\mathrm{fd}}_k.$$Proof
- Stabilizer. \((g,h)\in L^+H\times L^+H\) fixes \(x_\mu=t^{\mu_H}\) exactly when \(gt^{\mu_H}h^{-1}=t^{\mu_H}\), that is, when \(g=t^{\mu_H}ht^{-\mu_H}\). So \((g,h)\mapsto g\) is an isomorphism onto \(\Gamma_\mu\).
- Image at \(t=0\). In each root space \(\mathfrak h_\alpha\) of \(\mathfrak h=\operatorname{Lie}H\), \(\operatorname{Lie}\Gamma_\mu\) consists of the series divisible by \(t^{\max(0,\langle\alpha,\mu_H\rangle)}\). So evaluation at \(t=0\) maps it onto the Lie algebra of the parabolic subgroup \(P^-_{\mu_H}\): $$\operatorname{Lie}\Gamma_\mu=\mathfrak t_H[\![t]\!]\oplus\bigoplus_{\alpha\in\Phi_H}t^{\max(0,\langle\alpha,\mu_H\rangle)}\mathfrak h_\alpha[\![t]\!]\ \xrightarrow{\ t\mapsto0\ }\ \mathfrak t_H\oplus\bigoplus_{\langle\alpha,\mu_H\rangle\le0}\mathfrak h_\alpha=\operatorname{Lie}P^-_{\mu_H}.$$ So the image of \(\Gamma_\mu\) has identity component \(P^-_{\mu_H}\) and normalizes it. A parabolic subgroup is its own normalizer, so the image is \(P^-_{\mu_H}\), which is connected.
- Kernel. The kernel \(\Gamma_\mu\cap K_1\) is a closed subgroup of the pro-unipotent group \(K_1\), hence pro-unipotent and connected over \(\mathbb C\). An extension of a connected group by a connected group is connected (Zhu, §5.1): $$1\longrightarrow\Gamma_\mu\cap K_1\longrightarrow\Gamma_\mu\xrightarrow{\ t\mapsto0\ }P^-_{\mu_H}\longrightarrow1.$$
- Heart. \(\mathcal O_\mu\) is one orbit with stabilizer \(\Gamma_\mu\). So the ordinary heart of \(\mathcal C_\mu\) consists of the equivariant local systems of finite rank on \(\mathcal O_\mu\), that is, \(\operatorname{Rep}^{\mathrm{fd}}_k(\pi_0\Gamma_\mu)\) (draft Construction 3.34). With \(\pi_0\Gamma_\mu=1\) this is \(\operatorname{Vect}^{\mathrm{fd}}_k\), via \(V\mapsto\underline k_{\mathcal O_\mu}\otimes_kV\). Objects of \(\mathcal C_\mu\) are bounded, so the t-structure is bounded. This is H3.
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On bounded supports the action map is proper, with image a closed finite union of orbits. So convolution lands in \(\mathcal C\) and is exact in each variable:
$$\ast:\mathcal H\times\mathcal C\longrightarrow\mathcal C,\qquad V_\lambda\ast\mathrm{IC}_0\in\mathcal C.$$Proof
- Bounds. Each \(\mathcal A\in\mathcal H\) is supported on a Schubert variety of \(G\), a projective variety, and each \(\mathcal F\in\mathcal C\) on a closed finite union of orbits \(Z\) (H1(b)): $$\operatorname{Gr}_G^{\le\lambda}=\operatorname{Gr}_H^{\le\lambda_1}\times\operatorname{Gr}_H^{\le w_0\lambda_2}\qquad(\lambda\in\Lambda_T^+).$$
- Proper. \([g,x]\mapsto(gL^+G,gx)\) identifies the contracted product with a closed subspace of a product, and \(m\) becomes the second projection. Projecting away a projective factor is proper: $$\operatorname{Gr}_G^{\le\lambda}\mathbin{\widetilde\times}Z\ \xrightarrow{\ \sim\ }\ \{(gL^+G,y):g^{-1}y\in Z\}\subseteq\operatorname{Gr}_G^{\le\lambda}\times LX\xrightarrow{\ \mathrm{pr}_2\ }LX.$$
- Finite image. After the quotient of step 1, the image of \(m\) is the image of the convolution map \(\operatorname{Gr}_H^{\le\lambda_1}\mathbin{\widetilde\times}Z_H\mathbin{\widetilde\times}\operatorname{Gr}_H^{\le-\lambda_2}\to\operatorname{Gr}_H\) (Zhu, (2.1.17)). It is closed, \(L^+H\)-stable and of finite type, so it is a finite union of Schubert varieties, and its preimage \(Z'\) is a closed finite union of orbits.
- Sheaves. The twisted product \(\mathcal A\mathbin{\widetilde\boxtimes}\mathcal F\) is a bounded constructible equivariant complex, built by descent on the finite-type models of step 3 (Zhu, §A.1.2 and §A.1.4), and it is exact in each variable. Proper pushforward \(m_!=m_*\) is exact and preserves bounded constructible complexes. So \(\mathcal A\ast\mathcal F\in\mathcal C_{Z'}\subseteq\mathcal C\); for \(\mathcal A=V_\lambda\) and \(\mathcal F=\mathrm{IC}_0\) this is H4.
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Fix \(\mu=(\mu_H,-\mu_H)\in\Lambda_S^+\) and take the Hecke label \(\lambda=(\mu_H,0)\). Its Satake object is the intersection complex of \(\overline{\mathcal O_\mu}\), which restricts to one shifted constant sheaf on \(\mathcal O_\mu\):
$$\operatorname{supp}(V_{(\mu_H,0)}\ast\mathrm{IC}_0)\subseteq\overline{\mathcal O_\mu},\qquad a_\mu^*(V_{(\mu_H,0)}\ast\mathrm{IC}_0)\simeq\underline k_{\mathcal O_\mu}[\langle2\rho_H,\mu_H\rangle]\ \text{ in }\mathcal C_\mu.$$Proof
- Label. \(\mu_H\in\Lambda_H^+\) and \(-0\in\Lambda_H^+\), so \(\lambda\in\Lambda_T^+\), and it is a dominant lift of \(\mu\): $$\varphi(\lambda)=\lambda-\theta(\lambda)=(\mu_H,0)-(0,\mu_H)=\mu.$$
- Unit. In step 1 with \(\lambda_2=0\), the right factor is the unit: $$V_{(\mu_H,0)}\ast\mathrm{IC}_0\longleftrightarrow\mathrm{IC}^H_{\mu_H}\star\mathrm{IC}^H_0\simeq\mathrm{IC}^H_{\mu_H},\qquad\text{that is,}\qquad V_{(\mu_H,0)}\ast\mathrm{IC}_0\simeq p^*\mathrm{IC}^H_{\mu_H}.$$
- H5(a). \(\mathrm{IC}^H_{\mu_H}\) is supported on \(\operatorname{Gr}_H^{\le\mu_H}\), whose preimage is \(\overline{\mathcal O_\mu}\) by step 2.
- H5(b). The cell \(\operatorname{Gr}_H^{\mu_H}\) is smooth of dimension \(\langle2\rho_H,\mu_H\rangle\) (Zhu, Proposition 2.1.5(1)), and the intersection complex restricts to the shifted constant sheaf there (Zhu, §5.1). Pulling back along \(p\): $$a_\mu^*(V_{(\mu_H,0)}\ast\mathrm{IC}_0)\simeq p^*\big(\mathrm{IC}^H_{\mu_H}\big|_{\operatorname{Gr}_H^{\mu_H}}\big)\simeq\underline k_{\mathcal O_\mu}[\langle2\rho_H,\mu_H\rangle].$$ The object has a single nonzero cohomology object, of rank one, and by step 4 the only rank-one object of \(\mathcal C_\mu^\heartsuit\) is \(\underline k_{\mathcal O_\mu}\). So the isomorphism holds in \(\mathcal C_\mu\), with \(N_\mu=1\) and \(d_1=\langle2\rho_H,\mu_H\rangle\).
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Steps 2–6 verify H1–H5 for \(G=H\times H\) in \(\mathcal C\), so Proposition I gives generation and detection:
$$\mathcal C^{\mathrm{Sat}}=\mathcal C,\qquad\Map_{\widehat{\mathcal C}}(V_\lambda\ast\mathrm{IC}_0,F)=0\ \ \forall\lambda\in\Lambda_T^+\ \Longrightarrow\ F=0.$$The induction of Proposition I uses only the label chosen in H5 for each orbit. So the objects \(p^*\mathrm{IC}^H_{\mu_H}\) of step 6 already generate: \(\mathcal C=\operatorname{Thick}_{\mathcal C}\{p^*\mathrm{IC}^H_\eta:\eta\in\Lambda_H^+\}\).