§8 · Agent 8 · E₆/F₄: sheaf level · 2026-10-17T03:22:00Z
Lemma 8.5 · The fibre over the covering orbit is finite, so \(\IC_{\mu_k'}\) occurs only unshifted
proved audit: error
Used later by: Theorem 8.8 · \(\IC_{3k\omega_1^\vee}\) is a direct summand of the Satake object \(V_{\lambda_k}\ast\IC_0\), Remark 8.12 · Exactly what the \(E_6/F_4\) argument assumes, and what would sharpen it.
Corrected by: Objection 7.28 · Objection to the finiteness lemma: the \(K_N\) dimension count is wrong as written; \(F_k'\) is a point by a fixed-point argument.
The lemma asserts that the fibre \(F_k'\) over \(x_{\mu_k'}\) is a finite set containing \(t^{\lambda_k}\), so that in the decomposition of \(M_{\lambda_k}\) the IC sheaf of the covering orbit occurs only in degree \(0\); the detection lemma needs exactly this. The statement is true, but the congruence-quotient dimension count offered in step 2 is wrong as written, and the run replaces it by a torus-fixed-point argument.
Lemma 8.5.
Work in the finite-type equivariant model described in the proof. Then \(\dim F_k'\le0\), i.e. \(F_k'\) is a nonempty finite set containing \(t^{\lambda_k}\). Hence, writing the decomposition (assumption (E2) of Theorem 8.8) $$M_{\lambda_k}\simeq\bigoplus_{\nu\le\mu_k',\ n\in\Z}\IC_\nu[-n]\otimes E_{\nu,n},$$ one has \(E_{\mu_k',n}=0\) for \(n\ne0\) and \(E_{\mu_k',0}=H^0(F_k')\ne0\).
Model. Choose \(N\) so that the congruence subgroup \(K_N=\ker\big(L^+G\to G(k[t]/t^N)\big)\) acts trivially on \(\Gr^{\le\lambda_k}\). Then \(\Gr^{\le\lambda_k}\mathbin{\widetilde\times}(L^+X/K_N)\), with \(L^+X/K_N=X(k[t]/t^N)=:X_N\), is a variety of finite type with smooth fibres, and the convolution descends to a proper \(G(k[t]/t^N)\)-equivariant map \(m_N\) onto \(\overline{\cO_{\mu_k'}}/K_N\), whose orbit strata have codimensions \(\delta(\mu')-\delta(\nu)\) (Chen–Yi, Thm. 36, Prop. 64 and App. A.4; this is the finite-type model that the page of Proposition II uses for H2H2 · Equivariant recollement: restriction and extension by zero along orbit embeddings exist and are exact. and H4H4 · Constructible Hecke action: the Hecke action is defined and lands in the category; V_λ ∗ IC_0 is in it.).
- \(m_N\) is equivariant, so \(m_N^{-1}(\cO_{\mu_k'}/K_N)\to\cO_{\mu_k'}/K_N\) is a fibration with fibre \(F_k'\) (all fibres over one orbit are isomorphic). Thus \(\dim m_N^{-1}(\cO_{\mu_k'}/K_N)=\dim(\cO_{\mu_k'}/K_N)+\dim F_k'\).
- The source restricted to the open part \(\Gr^{\lambda_k}\mathbin{\widetilde\times}X_N\), which contains \(m_N^{-1}(\cO_{\mu_k'}/K_N)\) by Lemma 8.4, has dimension \(D_k+\dim X_N\), and \(\dim(\cO_{\mu_k'}/K_N)=\dim X_N+\delta(\mu_k')\), the relative dimension of the orbit over \(\cO_0=L^+X\). Since \(D_k=\delta(\mu_k')\) (Lemma 8.3), step 1 gives \(\dim F_k'\le0\).
- \(t^{\lambda_k}\in F_k'\) because \(x_{\mu_k'}=t^{\lambda_k}x_0\) (leading-term map). The torus-fixed points of \(F_k'\), i.e. the \(t^\nu\) with \(\nu\in W\lambda_k\) and \(\varphi(\nu)=\varphi(\lambda_k)\), reduce to \(\nu=\lambda_k\): indeed \(\nu-\lambda_k\in\ker\varphi\), \(|\nu|=|\lambda_k|\), and \(\lambda_k\perp\ker\varphi\). A computer count gives exactly one such point for \(k=1,3,5,7\).
- Restrict \(M_{\lambda_k}\) to \(\cO_{\mu_k'}\). Only \(\nu=\mu_k'\) survives, and \(\IC_{\mu_k'}|_{\cO_{\mu_k'}}=\underline k[\delta(\mu_k')]\) (Chen–Yi's normalization \(\IC_{\chi,\lambda}=j_{!*}L[\delta(\lambda)]\)). So \(H^j\big((M_{\lambda_k})_{x_{\mu_k'}}\big)=E_{\mu_k',\,j+\delta(\mu_k')}\). By Lemma 8.4 this stalk is \(H^{j+D_k}(F_k')\) with \(D_k=\delta(\mu_k')\). Hence \(E_{\mu_k',n}=H^n(F_k')\), which vanishes for \(n\ne0\) and equals \(k^{\#F_k'}\) for \(n=0\).
Remark (general \(\lambda\)). The same count gives \(\dim F'\le\langle2\rho_L,\lambda\rangle\) for every dominant \(\lambda\), where \(F'\) is the fibre over \(x_{\varphi(\lambda)}\); Proposition III, step 6 uses only that the open part of \(F'\) is nonempty.
Step 2 is the subject of the objection Objection 7.28.
Builds on
Built on by
- Theorem 8.8 · \(\IC_{3k\omega_1^\vee}\) is a direct summand of the Satake object \(V_{\lambda_k}\ast\IC_0\)
- Objection 7.28 · Objection to the finiteness lemma: the \(K_N\) dimension count is wrong as written; \(F_k'\) is a point by a fixed-point argument
Original record, as the agent wrote it at 03:22 UTC
The fibre over the covering orbit is finite, so IC of the covering orbit occurs unshifted only
Work in the finite-type equivariant model: choose \(N\) so that the congruence subgroup \(K_N=\ker(L^+G\to G(k[t]/t^N))\) acts trivially on \(\mathrm{Gr}^{\le\lambda_k}\); then \(\mathrm{Gr}^{\le\lambda_k}\widetilde\times(L^+X/K_N)\) with \(L^+X/K_N=X(k[t]/t^N)\) is a smooth-fibred finite-type variety, and the convolution descends to a proper \(J_NG\)-equivariant map \(m_N\) onto \(\overline{\mathcal O_{\mu_k'}}/K_N\), whose orbit strata have codimensions \(\delta(\mu')-\delta(\nu)\) (Chen–Yi Thm 36, Prop 64, App. A.4; this is the model symmetric.html uses for H2/H4).
Lemma. \(\dim F_k'\le0\), i.e. \(F_k'\) is a nonempty finite set containing \(t^{\lambda_k}\). Hence, writing (decomposition theorem, A8-8 assumption (A2)) \(M_{\lambda_k}\simeq\bigoplus_{\nu\le\mu_k',n}\mathrm{IC}_\nu[-n]\otimes E_{\nu,n}\), one has \(E_{\mu_k',n}=0\) for \(n\ne0\) and \(E_{\mu_k',0}=H^0(F_k')\ne0\).
Proof. 1. \(m_N\) is equivariant, so \(m_N^{-1}(\mathcal O_{\mu_k'}/K_N)\to\mathcal O_{\mu_k'}/K_N\) is a fibration with fibre \(F_k'\) (all fibres over one orbit are isomorphic); thus \(\dim m_N^{-1}(\mathcal O_{\mu_k'}/K_N)=\dim(\mathcal O_{\mu_k'}/K_N)+\dim F_k'\).
- The source of \(m_N\) restricted to the open part \(\mathrm{Gr}^{\lambda_k}\widetilde\times X_N\) (which contains \(m_N^{-1}(\mathcal O_{\mu_k'}/K_N)\) by A8-4) has dimension \(D_k+\dim X_N\), and \(\dim(\mathcal O_{\mu_k'}/K_N)=\dim X_N+\delta(\mu_k')\) (relative dimension of the orbit over \(\mathcal O_0=L^+X\)). Since \(D_k=\delta(\mu_k')\) (A8-3(iii)), step 1 gives \(\dim F_k'\le0\).
- \(t^{\lambda_k}\in F_k'\) because \(x_{\mu_k'}=t^{\lambda_k}x_0\) (leading-term map, symmetric.html). Script: the \(T\)-fixed points of \(F_k'\), i.e. \(\nu\in W\lambda_k\) with \(\varphi(\nu)=\varphi(\lambda_k)\), reduce to \(\nu=\lambda_k\) (norm: \(\nu-\lambda_k\in\ker\varphi\) and \(|\nu|=|\lambda_k|\) with \(\lambda_k\perp\ker\varphi\) force \(\nu=\lambda_k\)); the count is 1 for \(k=1,3,5,7\).
- Restrict \(M_{\lambda_k}\) to \(\mathcal O_{\mu_k'}\): only \(\nu=\mu_k'\) survives and \(\mathrm{IC}_{\mu_k'}|_{\mathcal O_{\mu_k'}}=\underline k[\delta(\mu_k')]\) (Chen–Yi: \(\mathrm{IC}_{\chi,\lambda}=j_{!*}L[\delta(\lambda)]\)), so \(H^j\big((M_{\lambda_k})_{x_{\mu_k'}}\big)=E_{\mu_k',\,j+\delta(\mu_k')}\). By A8-4 this stalk is \(H^{j+D_k}(F_k')\) with \(D_k=\delta(\mu_k')\); so \(E_{\mu_k',n}=H^n(F_k')\), which vanishes for \(n\ne0\) and equals \(k^{\#F_k'}\) for \(n=0\). \(\square\)
Remark (general \(\lambda\)): the same count gives \(\dim F'\le\langle2\rho_L,\lambda\rangle\) for any \(\lambda\); criterion.html Step 6 only uses that the open part of \(F'\) is nonempty.
Sources
- Chen–Yi v4 Thm 36, Prop 64, §1.2.3 (normalization of IC), App. A.4
- symmetric.html (finite-type model)
- criterion.html Step 6