arXiv:2607.08704v1

KK-spherical horospherical averages on the Nagao quotient: tree combinatorics and exact discrepancy

Sanghoon Kwon

math.DSmath.CO37A1720E0820G2511J70

Abstract

Let F=Fq( ⁣(t1) ⁣),G=SL2(F),Γ=SL2(Fq[t]),X=Γ\G, F=\mathbb{F}_q(\!(t^{-1})\!),\qquad G=\mathrm{SL}_2(F),\qquad Γ=\mathrm{SL}_2(\mathbb{F}_q[t]),\qquad X=Γ\backslash G, and let K=SL2(O)K=\mathrm{SL}_2(\mathcal{O}), where O=Fq[ ⁣[t1] ⁣]\mathcal{O}=\mathbb{F}_q[\![t^{-1}]\!]. We study right KK-spherical averages along the upper unipotent subgroup, the horospherical subgroup associated with the standard cusp, on the Nagao lattice quotient. The basic observation is that the KK-spherical projection converts two natural dynamical families - expanding translates of compact unipotent orbits and cusp-adapted truncations of dense unipotent orbits - into the same rooted descendant problem on the Bruhat--Tits tree. In the even bipartite sector the limiting height law is the explicit probability measure ρev(0)=q1q,ρev(2m)=(q21)q2m1(m1). ρ^{\mathrm{ev}}(0)=\frac{q-1}{q},\qquad ρ^{\mathrm{ev}}(2m)=(q^2-1)q^{-2m-1}\qquad (m\ge 1). We prove an exact discrepancy formula: in the backward state the error is a pure top-shell term minus a missing tail, while in the forward state the error is a first-turn weighted sum of backward errors. These formulas give quantitative KK-spherical equidistribution for expanding translates of compact UU-orbits and for dense-orbit truncations. For compactly supported KK-spherical observables in the expanding translates of compact orbits, the discrepancy is eventually exactly zero. In the dense case the rate is controlled by the continued-fraction expansion of the boundary point attached to the orbit.

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Detailed mathematical audit

Generated August 15, 2026
01Statements4 reported findingsCorrect

The central statements checked are correct. The exact rooted-shadow identities, the abstract spherical-shadow principle, the compact-orbit application, eventual exactness for compactly supported spherical tests, and the dense-truncation estimates all follow from the supplied combinatorics and standard Bruhat–Tits-tree coding with the stated normalizations.

Theorem 1.1Correct

Exact rooted-shadow discrepancy

Pages 3 and 7–12 · Theorem 1.1 and Section 3 · arXiv:2607.08704v1

The shell count at height one normalizes to the probability law ρev\rho^{\mathrm{ev}}. Re-rooting a backward shadow gives its exact top-shell correction and missing tail, while partitioning a forward shadow by its first turn gives the displayed geometric mixture. These identities imply finite-window exactness, L1(ρev)L^1(\rho^{\mathrm{ev}}) convergence for fixed roots, the three exponential regimes, and the uniform moving-root total-variation bound.

Full paper, version 1
Theorem 1.2Correct

Spherical-shadow principle

Pages 3–4 · Theorem 1.2 · arXiv:2607.08704v1

Testing a right KK-invariant observable reduces the discrepancy exactly to its height profile against the pushed-forward measure. Convexity and the componentwise total-variation estimate from Proposition 3.15 yield O(FqMT/2)O(\lVert F\rVert_\infty q^{-M_T/2}), and the backward formula yields the sharper O(FqMT)O(\lVert F\rVert_\infty q^{-M_T}) rate. Proposition 2.3 identifies the limiting height law with the spherical pushforward of μX\mu_X.

Full paper, version 1
Theorem 1.3(i) and Theorems 4.4–4.5Correct

Expanding translates of compact unipotent orbits

Pages 4 and 12–15 · Theorem 1.3(i), Lemma 4.2, and Theorems 4.4–4.5 · arXiv:2607.08704v1

Compactness restricts the initial spherical projection to finitely many sectors. In each sector, quotienting by UanKan1U\cap a_nKa_n^{-1} produces equal-mass cylinder cells forming a complete terminal descendant layer. The diagonal element translates by distance 2n2n in the type-preserving tree, while the finitely many initial roots contribute only bounded offsets, so the minimal cutoff tends to infinity. Theorem 1.2 gives equidistribution, and Proposition 3.11 makes the discrepancy exactly zero once the cutoff exceeds the finite support of the test profile.

Full paper, version 1
Theorem 1.3(ii) and Theorems 5.7–5.10Correct

Dense-orbit truncations and continued-fraction rates

Pages 4 and 15–21 · Theorem 1.3(ii) and Section 5 · arXiv:2607.08704v1

The lifted terminal layer consists of qNq^N equal-measure compact-open UU-cylinders, so its spherical average is exactly a rooted-shadow distribution with multiplicity. Function-field continued fractions code alternating cusp excursions: an excursion of degree ara_r has type-preserving length 2ar2a_r, and the turn contributes two further steps, giving Br+1=Br+2(ar+1)B_{r+1}=B_r+2(a_r+1). An irrational boundary point has infinitely many such blocks, hence MNM_N\to\infty; the bounded, admissible L1L^1, and effective estimates then follow from the corresponding rooted-shadow formulas.

Paulin–Shapira continued-fraction coding
02Proofs4 reported findingsCorrect

The proofs of the central results and their material geometric inputs are correct and complete.

Propositions 3.7–3.15Correct and complete

Rooted shell formulas and uniform discrepancy estimates

Pages 9–12 · Sections 3.3–3.6 · arXiv:2607.08704v1

The shell formula has total mass one and yields ρev\rho^{\mathrm{ev}} on every fixed finite height window. The first-turn weights sum to 1qN1-q^{-N}, with the remaining mass at the always-forward atom. Splitting turns at M/2M/2 gives the stated total-variation estimate, and the L1L^1 conclusions follow from the summable ρev\rho^{\mathrm{ev}} tail and geometric first-turn weights.

Full paper, version 1
Lemma 4.2 and Proposition 4.3Correct and complete

Finite-sector realization of compact horospheres

Pages 13–14 · Lemma 4.2 and Proposition 4.3 · arXiv:2607.08704v1

The compact set YKYK has finite image in the discrete Nagao ray. After selecting lifts in the corresponding finitely many cusp sectors, the double quotient is partitioned into cosets of the compact-open stabilizer. Along a descendant edge these stabilizers have index qq, so every family is the full terminal layer of its rooted sector with equal Haar mass. Translation by ana_n adds 2n2n to the depth and changes each root height by only a sector-dependent bounded amount. This verifies both the finite convex decomposition and the uniform divergence of its minimal cutoff.

Full paper, version 1
Lemma 5.3 and Propositions 5.5–5.6Correct and complete

Cylinder realization and exact cutoff coding

Pages 17–19 · Lemma 5.3 and Propositions 5.5–5.6 · arXiv:2607.08704v1

Conjugating the boundary point to infinity reduces the cylinder claim to compact-open additive subgroups of Fq((t1))\mathbb F_q((t^{-1})); each child stabilizer has index qq, which proves disjointness, equal mass, and the count qNq^N. The standard cross-section has first-return time twice the degree of the next partial quotient. Tracking the backward and forward halves of that return gives a constant cutoff followed by increments of two, with the additional two-step turn between blocks. Therefore the displayed block bases are exact and tend to infinity for every infinite continued fraction.

Paulin–Shapira, cross-section and return-time coding
Theorems 4.4–4.5 and 5.7–5.10Correct and complete

Applications of the rooted-shadow estimates

Pages 14–15 and 19–21 · Sections 4.2 and 5.4–5.5 · arXiv:2607.08704v1

Each application invokes a previously established shadow realization with the correct cutoff. Compact support is equivalent to finite support of the spherical height profile, so finite-window exactness applies. In the dense case, the top-shell and late-turn hypotheses in Definition 5.8 are exactly the two terms left by Proposition 3.10; the proof separately controls both and preserves the stated dependence on MNM_N.

Full paper, version 1
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Paper
arXiv:2607.08704v1
Authors listed
Sanghoon Kwon
Audit date
August 15, 2026
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