§4 · Agent 4 · Sheaf–function dictionary · 2026-10-17T02:07:17Z
Setup 4.1 · Set-up of the sheaf–function dictionary over \(\F_q(\!(t)\!)\): Weil objects, trace functions, obligations 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.
open audit: minor defect
Puts the symmetric space, its loop space and the category \(\cC_K\) over \(\F_q\), defines Frobenius trace functions of Weil objects, and lists the six inputs 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. on which every result of the dictionary track rests. Only \(\ell\)-adic sheaves over \(\overline{\F}_q\) and functions over \(\F_q(\!(t)\!)\) are compared; Betti sheaves over \(\C\) and \(p\)-adic functions are not.
Setup 4.1.
Setting. \(G,\theta,X=G/G^\theta\) are defined over \(\F_q\), \(q\) odd, with \(G^\theta\) connected and \(T\supseteq S\) split over \(\F_q\). Put \(k=\overline{\F}_q\), \(F=\F_q(\!(t)\!)\), \(\cO=\F_q[\![t]\!]\), \(K=G(\cO)\), and for \(n\ge1\) let \(F_n=\F_{q^n}(\!(t)\!)\), \(K_n=G(\F_{q^n}[\![t]\!])\). Then $$LX(\F_q)=X(F),\qquad L^+G(\F_q)=K,\qquad \Gr(\F_q)=G(F)/K,$$ and the Frobenius \(\mathrm{Fr}\) preserves every orbit \(\cO_\mu=L^+G\cdot x_\mu\), \(\mu\in\Lambda_S^+\).
Weil objects and traces. \(\cC_{K,k}=\Shv_{\mathrm{cons}}(L^+G\backslash LX)\) is Chen–Yi's \(\ell\)-adic category over \(k\) (Chen–Yi, App. A.5). A Weil object is a pair \((M,\Phi)\) with \(M\in\cC_{K,k}\) and \(\Phi:\mathrm{Fr}^*M\xrightarrow{\sim}M\). For \(x\in X(F_n)\), $$\tr_n(M,\Phi)(x)=\sum_i(-1)^i\tr\big(\Phi^n_x,\ \mathcal H^i(M)_x\big),\qquad \tr:=\tr_1 .$$ It is \(K_n\)-invariant, additive on exact triangles, \(\tr(M[1])=-\tr M\), and \(\tr(M\otimes\alpha)=\alpha\,\tr M\) for a rank-one twist by \(\alpha\in\overline{\Q}_\ell^\times\). An isomorphism \(\iota:\overline{\Q}_\ell\simeq\C\) and a square root \(q^{1/2}\) are fixed.
Objects compared. Sheaves: \(\Csat_k=\Thick_{\cC_{K,k}}\{V_\lambda\ast\IC_0\}\overset?=\cC_{K,k}\). Functions: (SG), \(\cH_K\cdot\varphi_0=C_K\), for \(F=\F_q(\!(t)\!)\). Not compared directly: \(\cC_K\) over \(\C\), and (SG) over a \(p\)-adic field.
Obligations. The results of this track are proved modulo:
- D0D0 · Orbit geometry over F̄_q, p ≠ 2 (Chen–Yi, Prop. 17, Thm 18): orbits indexed by Λ_S^+, closures, the support bound and the stabilizers. Chen–Yi's orbit geometry over \(k\), \(\operatorname{char}k\ne2\): orbits \(\leftrightarrow\Lambda_S^+\) with representatives \(x_\mu\) (Prop. 17), closures (Thm. 18), the support bound \(\supp(V_\lambda\ast\IC_0)\subseteq\overline{\cO_{\varphi(\lambda)}}\) (Proposition III, step 2), and the stabilizer lemma \(\pi_0\Stab_{L^+G}(x_\mu)\cong\pi_0Z_{G^\theta}(\mu)\), \(Z_{G^\theta}(\mu)=Z_{G^\theta}(\mu)^\circ Z_{G^\theta}(S)\) (Proposition III, step 4).
- D1D1 · Traces and t-structure: proper base change and the Grothendieck–Lefschetz trace formula on convolution fibres, with a Frobenius-compatible perverse t-structure whose simple objects are the IC sheaves. Proper base change and the Grothendieck–Lefschetz trace formula on the fibres of \(m:\Gr_{\le\lambda}\widetilde\times\overline{\cO_\nu}\to LX\) over rational points (closed subschemes of the finite-type \(\Gr_{\le\lambda}\)); a Frobenius-compatible perverse t-structure on \(\cC_{K,k}\) (Chen–Yi A.7) with finite-length heart whose simple objects are the \(\IC_{\chi,\mu}\), \(\chi\in\operatorname{Irr}\pi_0\Stab(x_\mu)\), with \(\End(\IC_{\chi,\mu})=\overline{\Q}_\ell\).
- 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). \(V_\lambda\ast\IC_0\) is pure and \(\simeq\bigoplus_b\IC(\overline{\cO_{\nu_b}},\mathcal L_b)[s_b]\) over \(k\) (decomposition theorem, BBD 5.4.5–5.4.6, as in the proof of Chen–Yi Thm. 93; Deligne's purity of proper pushforward), and \({}^pH^i\) of a pure Weil complex of weight \(w\) is pure of weight \(w+i\) (BBD 5.4.1) in Chen–Yi's sense (Def. 109, via finite-type smooth covers).
- D3D3 · Lang's theorem for the arc group L⁺G and its stabilizers over F_q. Lang's theorem for the pro-algebraic groups \(L^+G=\varprojlim G(\cO/t^n)\) and \(\Stab_{L^+G}(x_\mu)\).
- D4D4 · Unitriangularity of the Satake traces tr V_λ in the basis T_λ = 1_{Kt^λK} (Zhu (5.6.2), Lemma 5.6.3; Lusztig, Kato). Unitriangularity of \(\tr V_\lambda\) in the basis \(T_\lambda=\one_{Kt^\lambda K}\) (Zhu (5.6.2) and Lemma 5.6.3; Lusztig, Kato).
- 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). The comparison \(\overline{\F}_q\leftrightarrow\C\) of the statement "\(\IC_\mu\) is a summand of \(V_\lambda\ast\IC_0\)", a statement on a finite-type equivariant model (BBD 6.1.9; Bezrukavnikov–Finkelberg, Prop. 5); the workspace already assumes it (open item 1 of the criterion page).
- Rationality of the orbits. The Cartan map \(\tau(gG^\theta)=g\theta(g)^{-1}\) is injective on points over an algebraically closed field, hence on \(k(\!(t)\!)\)-points. Since \(S\) is split, \(t^\mu\in S(F)\) for \(\mu\in\Lambda_S\), so \(\tau(\mathrm{Fr}(x_\mu))=\mathrm{Fr}(t^\mu)=t^\mu=\tau(x_\mu)\): the point \(x_\mu\) is the unique point with \(\tau(x_\mu)=t^\mu\), and it is rational. Therefore \(\mathrm{Fr}(\cO_\mu)=\mathrm{Fr}(L^+G)\cdot x_\mu=\cO_\mu\).
- Weil objects. The pairs \((M,\Phi)\) are the Weil objects of Chen–Yi §8.2.1–8.2.2 (defined there for the Iwahori subgroup \(I_0\)) and §8.5.3 (for \(L^+G\)); the splitting of \(T\) over \(\F_q\) is the standing assumption of Chen–Yi §8.2. The listed properties of \(\tr_n\) are the usual ones: equivariance gives \(K_n\)-invariance, and the trace is additive along exact triangles.
- What is compared. The two statements are compared only in one pair of settings: \(\ell\)-adic sheaves over \(\overline{\F}_q\) and functions over \(\F_q(\!(t)\!)\). Passing to \(\cC_K\) over \(\C\) needs 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).; passing to a \(p\)-adic field needs a separate transfer that is not available (see Objection 4.12).
- Why D0D0 · Orbit geometry over F̄_q, p ≠ 2 (Chen–Yi, Prop. 17, Thm 18): orbits indexed by Λ_S^+, closures, the support bound and the stabilizers. is listed. Chen–Yi state Theorem 18 over any algebraically closed field of characteristic \(\ne2\) (Remark 19) and work over \(\F_q\) in §8.2, but their Proposition 17 is proved by citing Gaitsgory–Nadler and Nadler, over \(\C\). 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 the transfer the criterion page lists as its open item 1.
Builds on
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Built on by
- 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
- Objection 4.12 · Obstacles: \(\C\) versus \(\overline{\F}_q\), characteristic \(0\) in (A1)(A1) Field and group: F is a local field of characteristic 0 (p-adic), and G is split over the integers, with connected fibres and simply connected derived group. Its characteristic-p counterpart is (A1ₚ). versus \(\F_q(\!(t)\!)\), Weil versus geometric, eigenvalue cancellation
- Audit 7.3 · Audit of the orbit count, the trace dictionary and the IC expansion: they hold under D0–D3The 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., and D4D4 · Unitriangularity of the Satake traces tr V_λ in the basis T_λ = 1_{Kt^λK} (Zhu (5.6.2), Lemma 5.6.3; Lusztig, Kato). is elementary
- Lemma X2.2 · Weil inertia lemma: \(\operatorname{tr}_n\mathrm{IC}_{\chi,\nu}\circ\sigma_n=\chi(-1)\,\operatorname{tr}_n\mathrm{IC}_{\chi,\nu}\)
Original record, as the agent wrote it at 02:07 UTC
Dictionary set-up: Weil category over F_q, trace functions, and the obligations D0-D5
Setting for the dictionary. Take \(G,\theta,X=G/G^\theta\) over \(\mathbb F_q\) (\(q\) odd), \(T\) split over \(\mathbb F_q\) (the standing assumption of Chen–Yi §8.2), \(k=\overline{\mathbb F}_q\), \(F=\mathbb F_q(\!(t)\!)\), \(\mathcal O=\mathbb F_q[[t]]\). Then \(LX(\mathbb F_q)=X(F)\), \(L^+G(\mathbb F_q)=K=G(\mathcal O)\), \(\mathrm{Gr}(\mathbb F_q)=G(F)/K\), and Frobenius \(\mathrm{Fr}\) acts on \(LX\), \(LG\), on the orbits \(\mathcal O_\mu\) (each \(\mathrm{Fr}\)-stable: \(x_\mu\) is the unique point with \(\tau(x_\mu)=t^\mu\in S(F)\), so it is rational), and on \(\mathcal C_k:=\mathrm{Shv}_{\mathrm{cons}}(L^+G\backslash LX)\) in Chen–Yi's \(\ell\)-adic theory (App. A.5).
Weil objects and trace functions. \(\mathcal C^{\mathrm W}\): pairs \((M,\Phi)\), \(M\in\mathcal C_k\), \(\Phi:\mathrm{Fr}^*M\xrightarrow{\sim}M\) (Chen–Yi §8.2.1–8.2.2 define exactly this for \(I_0\) and, in §8.5.3, for \(L^+G\)). For \(x\in X(F)\) and \(n\ge1\) with \(x\in LX(\mathbb F_{q^n})\): $$\operatorname{tr}_n(M,\Phi)(x):=\sum_i(-1)^i\operatorname{tr}\big(\Phi^n_x,\ \mathcal H^i(M)_x\big),\qquad \operatorname{tr}:=\operatorname{tr}_1 .$$ It is \(G(\mathcal O_n)\)-invariant (equivariance), additive on exact triangles, and \(\operatorname{tr}(M[1])=-\operatorname{tr}M\), \(\operatorname{tr}(M\otimes\alpha)=\alpha\operatorname{tr}M\) for a rank-one twist by \(\alpha\in\overline{\mathbb Q}_\ell^\times\). Fix \(\iota:\overline{\mathbb Q}_\ell\simeq\mathbb C\) and \(q^{1/2}\).
Objects compared. Sheaf side: \(\mathcal C^{\mathrm{Sat}}_k=\mathrm{Thick}_{\mathcal C_k}\{V_\lambda\ast\mathrm{IC}_0\}\) over \(k=\overline{\mathbb F}_q\). Function side: (SG) for \(F=\mathbb F_q(\!(t)\!)\): \(\mathcal H_K\cdot\varphi_0=C_K\). Not compared directly: \(\mathcal C\) over \(\mathbb C\) and (SG) over \(p\)-adic \(F\); these need D5 and a separate (unavailable) transfer, see A4-12.
Obligations (the gap). Everything below is proved modulo:
- D0 Chen–Yi's geometry over \(k=\overline{\mathbb F}_q\), \(\operatorname{char}\neq2\): Prop. 17 (orbits \(\leftrightarrow\Lambda_S^+\), \(x_\mu\)), Thm 18 (closures), Lemma Step 2 of criterion.html (support bound \(\operatorname{supp}(V_\lambda\ast\mathrm{IC}_0)\subseteq\overline{\mathcal O_{\varphi(\lambda)}}\), geometric), Lemma Step 4 (\(\pi_0\mathrm{Stab}_{L^+G}(x_\mu)\cong\pi_0Z_K(\mu)\), \(Z_K(\mu)=Z_K(\mu)^\circ Z_K(S)\)). Chen–Yi state Thm 18 for any algebraically closed field of characteristic \(\ne2\) (Remark 19) and use the \(\mathbb F_q\)-setting in §8.2, but Prop. 17 cites [GN10],[Nad04] (over \(\mathbb C\)).
- D1 Proper base change and the Grothendieck–Lefschetz trace formula for \(m:\mathrm{Gr}_{\le\lambda}\tilde\times\overline{\mathcal O_\nu}\to LX\) restricted to the fibre over a rational point (a closed subscheme of the finite-type \(\mathrm{Gr}_{\le\lambda}\)); and the perverse t-structure \(\mathrm{Perv}_\delta\) of Chen–Yi A.7 on \(\mathcal C_k\), compatible with \(\mathrm{Fr}^*\), with heart of finite length whose simple objects are the \(\mathrm{IC}_{\chi,\mu}\) (\(\chi\in\mathrm{Irr}\,\pi_0\mathrm{Stab}(x_\mu)\)), \(\operatorname{End}(\mathrm{IC}_{\chi,\mu})=\overline{\mathbb Q}_\ell\).
- D2 Purity/decomposition: \(V_\lambda\ast\mathrm{IC}_0\) is pure and \(\simeq\bigoplus_b\mathrm{IC}(\overline{\mathcal O_{\nu_b}},\mathcal L_b)[s_b]\) over \(k\) (criterion.html Step 5 Lemma (b), Chen–Yi Thm 93 proof, BBD 5.4.5–5.4.6, Deligne's purity of proper pushforward), and \(\mathcal{}^p\mathcal H^i\) of a pure weight-\(w\) Weil complex is pure of weight \(w+i\) (BBD 5.4.1) in Chen–Yi's sense (Def. 109, via finite-type smooth covers).
- D3 Lang's theorem for the pro-algebraic groups \(L^+G=\varprojlim G(\mathcal O/t^n)\) and \(\mathrm{Stab}_{L^+G}(x_\mu)\) (A4-2).
- D4 The Lusztig–Kato unitriangularity for \(\operatorname{tr}V_\lambda\) (Zhu's notes (5.6.2), Lemma 5.6.3; Lusztig 1983, Kato 1982).
- D5 Comparison \(\overline{\mathbb F}_q\leftrightarrow\mathbb C\) of the statement "\(\mathrm{IC}_\mu\) is a summand of \(V_\lambda\ast\mathrm{IC}_0\)" (a statement on a finite-type equivariant model: BBD 6.1.9, Bezrukavnikov–Finkelberg Prop. 5; already assumed by criterion.html, "open item 1").
Sources
- /Users/miltonlin/Projects/Trees/subpages/case-study-1-ramifiedrelative/proof_graphs/spherical-generation/criterion.html (Steps 2,4,5)
- sources/chen-yi-v4.pdf §8.2, §8.5.3, App. A.5, A.7, A.8, Thm 93
- sources/zhu-satake-v2.pdf §5.6
- sources/bbd-perverse.pdf 5.4.1, 5.4.5, 5.4.6, 6.1.9