§4 · Agent 4 · Sheaf–function dictionary · 2026-10-17T02:40:19Z

Theorem 4.6 · Theorem: (SG) over \(\F_q(\!(t)\!)\) implies \(\Csat=\cC_K\) over \(\overline{\F}_q\)

proved audit: correct ★ key step

Second audit: correct. Each step checked: (SG) makes the span of the traces all of C_K ⊗ Q̄_ℓ; a nonzero coordinate functional is nonzero on some generator; zero multiplicity space ⇒ zero coefficient; Lemma 4.5(iii). No purity is needed beyond the decomposition. D5D5 · Comparison with C: “IC_μ is a summand of V_λ ∗ IC_0” has the same answer over F̄_q and over C (BBD §6.1, for large p). is an explicit hypothesis at the given p; Bezrukavnikov–Finkelberg Prop. 5 supplies it only for p outside a finite set depending on the finite-type model, which suffices whenever (SG) is known for all q (as for GL4/Sp4 and, later, GL2m/Sp2m).

For a symmetric space with \(G^\theta\) and \(Z_{G^\theta}(S)\) connected, spherical generation of functions over \(\F_q(\!(t)\!)\), for a single \(q\), forces every \(\IC_\mu\) to be a summand of a Satake object, hence \(\Csat=\cC_K\) over \(\overline{\F}_q\), modulo D0–D4The standing inputs of the sheaf–function dictionary over F̄_q, p ≠ 2: D0 Chen–Yi's orbit geometry; D1 traces of Frobenius and the perverse t-structure; D2 decomposition of Satake objects into shifted IC sheaves; D3 Lang's theorem; D4 unitriangularity of Satake traces; D5 comparison of F̄_q with C.. So the divergence "functions generate, sheaves do not" cannot occur in this setting.

Theorem 4.6.

Let \(X=G/G^\theta\) be symmetric with \(G^\theta\) and \(Z_{G^\theta}(S)\) connected, defined over \(\F_q\), \(q\) odd, \(T\) split, and assume D0–D4The standing inputs of the sheaf–function dictionary over F̄_q, p ≠ 2: D0 Chen–Yi's orbit geometry; D1 traces of Frobenius and the perverse t-structure; D2 decomposition of Satake objects into shifted IC sheaves; D3 Lang's theorem; D4 unitriangularity of Satake traces; D5 comparison of F̄_q with C. of Setup 4.1. If (SG) holds for \(F=\F_q(\!(t)\!)\), i.e. $$\cH_K\cdot\one_{X(\cO)}=C_c^\infty(X(F))^K,$$ then \(\Csat_{\overline{\F}_q}=\cC_{\overline{\F}_q}\); under D5D5 · Comparison with C: “IC_μ is a summand of V_λ ∗ IC_0” has the same answer over F̄_q and over C (BBD §6.1, for large p). also \(\Csat_{\C}=\cC_{\C}\). The same holds if (SG) holds for \(\F_{q^n}(\!(t)\!)\) for one \(n\).

  1. By Lemma 4.3, \(\cH_K\varphi_0\otimes\overline{\Q}_\ell=\operatorname{span}\{\tr(V_\lambda\ast\IC_0)\}_\lambda\). By Lemma 4.4 (part 1), \(\{\tr\IC_\nu\}\) is a basis of \(C_K\otimes\overline{\Q}_\ell\); let \(\pi_\mu\) be the coordinate functional of \(\tr\IC_\mu\).
  2. (SG) says that the span in step 1 is all of \(C_K\otimes\overline{\Q}_\ell\). Hence \(\pi_\mu\) is nonzero on some \(\tr(V_\lambda\ast\IC_0)\), that is, \(m^{(1)}_{\mu\lambda}\ne0\) by Lemma 4.4 (part 3).
  3. By Lemma 4.4 (part 4(i)), \(E_{\mu,i}(\lambda)\ne0\) for some \(i\): a shift of \(\IC_\mu\) is a direct summand of \(V_\lambda\ast\IC_0\) (Lemma 4.4, part 2).
  4. Lemma 4.5 (part 3) gives \(\Csat=\cC_K\).
  5. Over \(\F_{q^n}\): the same argument with \(\tr_n\). \(\square\)

What is and is not used. No positivity and no purity beyond the decomposition in D2D2 · Decomposition: each Satake object V_λ ∗ IC_0 is pure and splits into shifted IC sheaves with finite-dimensional multiplicity spaces (Sun, Thm 1.2; Chen–Yi, Prop. 70).: step 3 uses only "zero multiplicity space implies zero coefficient". Lang's theorem (Lemma 4.2) is used to know that \(C_K\) is spanned by the \(\one_{\cO_\mu(\F_q)}\), \(\mu\in\Lambda_S^+\); otherwise the traces of the \(\IC_\nu\) with constant coefficients would not span \(C_K\). The hypothesis "\(Z_{G^\theta}(S)\) connected" enters through H3H3 · Constant coefficients: on each orbit the heart consists of finite sums of the constant sheaf. (constant coefficients) and through Lemma 4.2.

Consequence for the question. For symmetric \(X\) on these pages with \(Z_{G^\theta}(S)\) connected, "(SG) over \(\F_q(\!(t)\!)\) holds but \(\Csat\ne\cC_K\)" cannot occur (modulo D0–D5The standing inputs of the sheaf–function dictionary over F̄_q, p ≠ 2: D0 Chen–Yi's orbit geometry; D1 traces of Frobenius and the perverse t-structure; D2 decomposition of Satake objects into shifted IC sheaves; D3 Lang's theorem; D4 unitriangularity of Satake traces; D5 comparison of F̄_q with C.).

Builds on

  • Lemma 4.2 · \(K\)-orbits on \(X(\F_q(\!(t)\!))\) via Lang's theorem: \(\Lambda_S^+\) exactly when \(Z_{G^\theta}(S)\) is connected
  • Lemma 4.3 · The trace of \(V_\lambda\ast\IC_0\) is \(\tr(V_\lambda)\ast\varphi_0\), and the traces of the \(V_\lambda\) form a basis of \(\cH_K\)
  • Lemma 4.4 · Expansion of \(\tr(V_\lambda\ast\IC_0)\) in the IC basis: the coefficients are traces of Frobenius on multiplicity spaces
  • Lemma 4.5 · \(\Csat=\cC_K\) if and only if every \(\IC_\mu\) is a direct summand of a Satake object

Built on by

Original record, as the agent wrote it at 02:40 UTC

Theorem: spherical generation over F_q((t)) implies thick generation of C over F_q-bar

Theorem A4-6 ((SG) \(\Rightarrow\) \(\mathcal C^{\mathrm{Sat}}=\mathcal C\)). Let \(X=G/G^\theta\) be symmetric with \(G^\theta\) and \(Z_{G^\theta}(S)\) connected, defined over \(\mathbb F_q\), \(q\) odd, \(T\) split. Assume D0–D4. If (SG) holds for \(F=\mathbb F_q(\!(t)\!)\), i.e. \(\mathcal H_K\cdot\mathbf 1_{X(\mathcal O)}=C_c^\infty(X(F))^K\), then \(\mathcal C^{\mathrm{Sat}}_{\overline{\mathbb F}_q}=\mathcal C_{\overline{\mathbb F}_q}\); under D5 also \(\mathcal C^{\mathrm{Sat}}_{\mathbb C}=\mathcal C_{\mathbb C}\). The same holds if (SG) holds for \(\mathbb F_{q^n}(\!(t)\!)\) for one \(n\).

Proof. 1. By A4-3, \(\mathcal H_K\varphi_0\otimes\overline{\mathbb Q}_\ell=\operatorname{span}\{\operatorname{tr}(V_\lambda\ast\mathrm{IC}_0)\}_\lambda\). By A4-4.1, \(\{\operatorname{tr}\mathrm{IC}_\nu\}\) is a basis of \(C_K\otimes\overline{\mathbb Q}_\ell\); let \(\pi_\mu\) be the coordinate functional of \(\operatorname{tr}\mathrm{IC}_\mu\). 2. (SG) says the span in 1 is all of \(C_K\otimes\overline{\mathbb Q}_\ell\), so \(\pi_\mu\) is nonzero on some \(\operatorname{tr}(V_\lambda\ast\mathrm{IC}_0)\), i.e. \(m^{(1)}_{\mu\lambda}\ne0\) by A4-4.3. 3. By A4-4.4(i), \(E_{\mu,i}(\lambda)\ne0\) for some \(i\): \(\mathrm{IC}_\mu\) is a direct summand of \(V_\lambda\ast\mathrm{IC}_0\) (A4-4.2). 4. A4-5(iii). 5. Over \(\mathbb F_{q^n}\): same with \(\operatorname{tr}_n\). \(\square\)

What is and is not used. No positivity and no purity beyond D2's decomposition: step 3 uses only "zero multiplicity space \(\Rightarrow\) zero coefficient". Lang (A4-2) is used to know that \(C_K\) is spanned by the \(\mathbf 1_{\mathcal O_\mu(\mathbb F_q)}\) indexed by \(\Lambda_S^+\) (else the \(\operatorname{tr}\mathrm{IC}_\nu\) with constant coefficients would not span \(C_K\)). The hypothesis "Z connected" enters through H3 (constant coefficients) and through A4-2. Consequence for the team question: on these pages, for symmetric \(X\) with \(Z_{G^\theta}(S)\) connected, "(SG) over \(\mathbb F_q(\!(t)\!)\) holds but \(\mathcal C^{\mathrm{Sat}}\ne\mathcal C\)" cannot occur (modulo D0–D5).

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