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–H5On 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
    1. 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 \(\lambda\mapsto\lambda-\theta(\lambda)\): $$T\longrightarrow S,\quad t\longmapsto t\theta(t)^{-1},\qquad\lambda-\theta(\lambda)\in\Lambda_S.$$
    2. 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: $$\theta\alpha=\alpha\quad(\alpha\in\Phi_L),\qquad-\theta\alpha\in\Phi^+\quad(\alpha\in\Phi^+\setminus\Phi_L).$$
    3. 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: $$\boxed{\varphi:\Lambda_T^+\longrightarrow\Lambda_S^+,\quad\lambda\longmapsto\lambda-\theta(\lambda).}$$
    4. 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.

    Leading-term map · two minimal examples →

  • 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.
    1. Each orbit closure is the disjoint union of the finitely many orbits below it: $$\overline{\mathcal O_\mu}=\bigsqcup_{\nu\le\mu}\mathcal O_\nu,\qquad\#\{\nu\in\Lambda_S^+:\nu\le\mu\}\lt\infty.$$
    2. 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 $$i:D\hookrightarrow Z,\qquad r_Z:Z\hookrightarrow LX,\qquad a_{\mu,Z}:\mathcal O_\mu\hookrightarrow Z.$$
    1. 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 \(f^*\).
    2. 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: $$j_!j^*M\longrightarrow M\longrightarrow i_*i^*M\xrightarrow{+1}.$$
    3. Restriction and extension by zero respect composition: \((fg)^*\simeq g^*f^*\) and \((fg)_!\simeq f_!g_!\).
    Kuijper (2026), Definition 2.3.4 and Lemma 4.3.3 supply the abstract recollement mechanism; preservation of these constructible subcategories is part of H2.
  • 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:
    1. It lives on the closure of \(\mathcal O_\mu\): $$\operatorname{supp}(V_\lambda\ast\mathrm{IC}_0)\subseteq\overline{\mathcal O_\mu}.$$
    2. 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.

  1. 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 \(\mathrm{IC}^H_0\): $$V_{(\lambda_1,\lambda_2)}\ast\mathrm{IC}_0\longleftrightarrow\mathrm{IC}^H_{\lambda_1}\star\mathrm{IC}^H_0\star\mathrm{IC}^H_{-\lambda_2}=\mathrm{IC}^H_{\lambda_1}\star\mathrm{IC}^H_{-\lambda_2}.$$
  2. 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.
  3. 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).
  4. 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.
  5. 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.
  6. 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 \(d_1=\langle2\rho_H,\mu_H\rangle\).
  7. 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: \(\mathcal C=\operatorname{Thick}_{\mathcal C}\{p^*\mathrm{IC}^H_\eta:\eta\in\Lambda_H^+\}\).