§5 · Agent 5 · Functions without (A1)–(A5) · 2026-10-17T03:32:17Z
Summary 5.10 · Table changes at function level; no row disagrees between the levels; nothing here depends on (A)“Under (A)”: assuming all of Sakellaridis's assumptions (A1)–(A5) for X at the given p-adic place, so that his Theorem 8.0.2 applies.
proved audit: minor defect
Records the rows of Table 1 that the lattice method settles unconditionally over every local field — the spheres, \(\GL_n/(\GL_p\times\GL_q)\), \(\GL_{2m}/\Sp_{2m}\) and \(\SL_{2n}/\Sp_{2n}\) — leaves \(E_6/F_4\) open, and concludes that no row has the two levels decided in opposite directions.
Summary 5.10.
Function column of Table 1, now for every non-archimedean local field \(F\), in any residue characteristic (for \(\GL_n/(\GL_p\times\GL_q)\) with the pair model, which is the involution model exactly when the residue characteristic is odd):
- \(\Spin_{2n}/\Spin_{2n-1}\): '\(n=3\) under (A)“Under (A)”: assuming all of Sakellaridis's assumptions (A1)–(A5) for X at the given p-adic place, so that his Theorem 8.0.2 applies.; \(n\ge4\) open' becomes holds for all \(n\ge2\) (Theorem 5.3);
- \(\GL_n/(\GL_p\times\GL_q)\): 'under (A)“Under (A)”: assuming all of Sakellaridis's assumptions (A1)–(A5) for X at the given p-adic place, so that his Theorem 8.0.2 applies.' becomes holds (Theorem 5.4);
- \(\GL_{2m}/\Sp_{2m}\) and \(\SL_{2n}/\Sp_{2n}\): 'under (A)“Under (A)”: assuming all of Sakellaridis's assumptions (A1)–(A5) for X at the given p-adic place, so that his Theorem 8.0.2 applies.' becomes holds (Theorem 5.7);
- \(E_6/F_4\): still open (Dead end 5.9).
Unchanged: the group (Proposition D), \(\mathbb A^n\) (G), \(M_n\) (H), \(\SL_2/T\) fails for \(q\) odd (J), \(\GL_n/\mathrm O_n\) fails, and Sakellaridis's example fails (the only row still resting on Theorem E). No row on these pages has \(\Csat=\cC_K\) proved and \((\mathrm{SG})\) false, nor \((\mathrm{SG})\) proved and \(\Csat\ne\cC_K\) proved.
- Inputs. Lemma A(2), Proposition B and elementary lattice algebra; for the spheres two standard inputs (smoothness of orthogonal groups of regular quadratic lattices, and Kummer theory with the spinor norm over \(\cO\)); for the support bound of Proposition 5.8, the Cartan convolution bound. Theorem E, (A1)–(A5)Sakellaridis's standing assumptions for his Theorem 8.0.2 (the pages' Theorem E): (A1) a characteristic-0 field and a split group with simply connected derived group; (A2) an integral model of X with a smooth open Borel orbit and invariant measures; (A3a) rank-one models over O, (A3b) the Cartan decomposition, (A3c) Iwahori orbits (his Axioms 2.2.1, 2.4.1, 2.4.2); (A4) conditions on the spherical roots and colours; (A5) X homogeneous and affine with one open Borel orbit., \(\operatorname{char}F=0\) and Borel–Serre are used nowhere, and the computation of the restriction map in Proposition F is no longer needed for these rows.
- Unchanged rows. \(\SL_2/T\) is recorded as failing for \(q\) odd because the square-class argument of Proposition J(2) needs a non-square unit.
- The two levels. Where the sheaf side is decided (spheres, \(\GL_n/(\GL_p\times\GL_q)\), the group, \(\mathbb G_m\)), both \(\Csat=\cC_K\) and \((\mathrm{SG})\) hold: the levels agree. Where coverage leaves the sheaf side undecided (\(\GL_{2m}/\Sp_{2m}\) with \(m\ge2\); \(\SL_{2n}/\Sp_{2n}\) with \(n\ge3\)), \((\mathrm{SG})\) now holds unconditionally, so no decided disagreement exists there; a case '\((\mathrm{SG})\) holds but \(\Csat\ne\cC_K\)' would require deciding the sheaf side negatively.
- A heuristic pointer only. Lemma 2 of Lemma 5.6 exhibits a point of the open stratum of the fibre \(\{g\in\Gr_{\le\lambda^*(b)}:g^{-1}x_b\in L^+X\}\), so by the weight argument of Step 5(a) of Proposition III one expects \(a_b^*(V_{\lambda^*(b)}\ast\IC_0)\ne0\) at an uncovered \(b\). The sheaf question is whether \(\IC(\overline{\cO_b})\) itself is a summand (the retract condition) or only larger intersection complexes restrict nontrivially; this is not decided here.
Builds on
- Theorem 5.3 · \((\mathrm{SG})\) for \(\Spin_{2n}/\Spin_{2n-1}\), every \(n\ge2\), every non-archimedean local field
- Theorem 5.4 · \(\GL_n/(\GL_p\times\GL_q)\), pair model: orbits, lifts, a componentwise support bound and \((\mathrm{SG})\) over every \(F\)
- Theorem 5.7 · \((\mathrm{SG})\) for \(\GL_{2m}/\Sp_{2m}\) (all \(m\)) and \(\SL_{2n}/\Sp_{2n}\) (all \(n\)), every non-archimedean local field
- Proposition 5.8 · The support bound of H5H5 · Nonzero top splitting: for every orbit O_μ some Satake object V_λ ∗ IC_0 is supported on its closure with a nonzero split restriction to O_μ.(a) at function level over every \(F\), and the same-points question
- Dead end 5.9 · \(E_6/F_4\) at function level: what the lattice method would need
Built on by
- Objection 7.24 · Objection: the support-bound check passes; the \(E_6/F_4\) expectation and two table cells are stale
- Correction X3.6 · Correction of A7-24: its two objections stand; its claim that A5-8 holds needs a new proof
Original record, as the agent wrote it at 03:32 UTC
Table changes; no row disagrees between the levels; nothing here depends on (A)
Rows of Table 1 (classical.html §7, summary.html Table 1) that change at function level, now for EVERY non-archimedean local field \(F\) (any residue characteristic; for \(\mathrm{GL}_n/(\mathrm{GL}_p\times\mathrm{GL}_q)\) with the pair model, which is the \(J\)-model iff \(q\) odd):
- \(\mathrm{Spin}_{2n}/\mathrm{Spin}_{2n-1}\): "\(n=3\) under (A); \(n\ge4\) open" → holds, all \(n\ge2\) (node 3).
- \(\mathrm{GL}_n/(\mathrm{GL}_p\times\mathrm{GL}_q)\): "under (A)" → holds (node 4).
- \(\mathrm{GL}_{2m}/\mathrm{Sp}_{2m}\), \(\mathrm{SL}_{2n}/\mathrm{Sp}_{2n}\): "under (A)" → holds (node 7).
- \(E_6/F_4\): still open (node 9).
Unchanged: group (D), \(\mathbb A^n\) (G), \(M_n\) (H), \(\mathrm{SL}_2/T\) fails for \(q\) odd (J; the square-class argument needs a non-square unit, so \(q\) odd), \(\mathrm{GL}_n/\mathrm O_n\) fails, Sakellaridis's example fails (only row still resting on Theorem E).
What is used: Lemma A(2), Proposition B, elementary lattice algebra; for the sphere two standard inputs (smoothness of orthogonal groups of regular quadratic lattices; Kummer/spinor norm over \(\mathcal O\)); for node 8(b) the Cartan convolution bound. Theorem E, (A1)–(A5), \(\operatorname{char}F=0\), Borel–Serre are not used anywhere; Proposition F's computation of \(r\) is no longer needed for these rows.
Levels. Where the sheaf side is decided (spheres, \(\mathrm{GL}_n/(\mathrm{GL}_p\times\mathrm{GL}_q)\), group, \(\mathbb G_m\)): \(\mathcal C^{\mathrm{Sat}}=\mathcal C\) and (SG) both hold — agreement. Where the sheaf side is undecided by coverage (\(\mathrm{GL}_{2m}/\mathrm{Sp}_{2m}\), \(m\ge2\); \(\mathrm{SL}_{2n}/\mathrm{Sp}_{2n}\), \(n\ge3\)): (SG) now holds unconditionally, so no decided disagreement exists; "(SG) holds but \(\mathcal C^{\mathrm{Sat}}\ne\mathcal C\)" would require deciding the sheaf side negatively. Heuristic pointer only: node 6, Lemma 2 exhibits a point of the open stratum of the fibre \(\{g\in\mathrm{Gr}_{\le\lambda^*(b)}:g^{-1}x_b\in L^+X\}\), so by the weight argument of Step 5(a) \(a_b^*(V_{\lambda^*(b)}\ast\mathrm{IC}_0)\ne0\) at the uncovered \(b\); the sheaf question is whether \(\mathrm{IC}(\overline{O_b})\) itself is a summand (the paper's retract condition) or only higher \(\mathrm{IC}\)'s restrict nontrivially — not decided here. No case on these pages has \(\mathcal C^{\mathrm{Sat}}=\mathcal C\) proved and (SG) false, nor (SG) proved and \(\mathcal C^{\mathrm{Sat}}\ne\mathcal C\) proved.
Sources
- summary.html#2
- classical.html#7