Local ring refinement beyond mod 3

Paper XIV in the singular Hecke node series
Richard Hoekstra · 2026

Beyond the mod-3 picture

Paper III describes the singular Hecke order modulo 3. This paper lifts the analysis to the full 3-adic integers, revealing structure invisible at the residue field level.

Discriminant computation

T2 has characteristic/minimal polynomial of degree 13 (= dim S20(163))). The discriminants are:

OrderDiscriminant
Full Hecke order T215 · 32 · 65657 · 82536739
Monogenic order Z[T2]215 · 38 · 65657 · 3740832 · 82536739
T2 is primitive over Q — it generates the Hecke algebra rationally. But the index [T : Z[T2]] = 10100241 = 33 · 374083, so in particular v3([T : Z[T2]]) = 3. The full integral 3-local fiber is not the naive monogenic order Z3[T2].

Rational 3-adic splitting

The T2 polynomial factors over Q3 with factor degrees [1, 1, 1, 4, 6]. The rational 3-adic Hecke algebra therefore splits as:

T ⊗ Q3 = Q33 × K4 × K6

where K4 and K6 are unramified extensions of Q3 of degrees 4 and 6 respectively. The singular part is the rank-3 factor coming from the three linear Q3 roots that all reduce to 0 mod 3.

The rank-3 singular order

Projecting onto the three singular Q3 factors, the full 3-local order is spanned over Z3 by {1, T3, T11}. Every Tn for 1 ≤ n ≤ 13 has integral coordinates in this basis. The determinant valuation of this basis in the ambient Q33 is v3 = 1.

Lifted idempotent and local factor

The mod-3 idempotent E = T3|Q lifts uniquely modulo each 3k. Splitting by ek gives a rank-1 etale factor and a rank-2 local factor Rloc.

In the local factor, with identity u0 = 1 − ek and generator y = (1 − ek)T11, the local factor relations modulo successive powers of 3 are:

ModulusLocal relationUnit uk
mod 27 (33)y2 = 91
mod 81 (34)y2 = 364
mod 243 (35)y2 = 19822
mod 729 (36)y2 = 44149

After the shift y = n − (bk/2)u0, the linear term vanishes exactly modulo each 3k, and the local factor takes the monogenic form:

Local factor structure The local factor modulo 3k is (Z/3kZ)[y]/(y2 − 9uk) where uk is a 3-adic unit. The Loewy length of this quotient is exactly k+1, with dimF3(mj/mj+1) = 2 for 1 ≤ j < k and 1 for j = k.

Over Z3, the maximal ideal of Rloc is generated by 3 and y. It is not nilpotent (the Loewy filtration is infinite), but in the finite quotients modulo 3k the ideal powers terminate with mj = (3j, 3j−1y).

Key observations

T11 as local generator. The generator of the local factor is T11 (nilpotent escape operator), not T3 (idempotent exclusion). This is consistent with the automaton picture: T11 carries the depth information.

T163 as negative identity. In the local factor, T163 = −u0 to full working precision. The Atkin-Lehner involution at the prime level acts as −1 on the singular part.

Canonical collision splits. T43 ≡ T67 (mod 3) — the canonical collision from Paper II — but they split modulo 9. The collision is a residue-field phenomenon, not a 3-adic one.

Summary

The singular 3-local Hecke factor is not just the mod-3 syndrome algebra. It is a semilocal rank-3 order that splits canonically into Z3 × Rloc, where Rloc is a rank-2 local Z3-order whose finite quotients are quadratic orders (Z/3kZ)[y]/(y2 − 9uk) with unit uk. The non-semisimple mod-3 defect comes from this quadratic 3-adic local ring, not from the naive monogenic order Z3[T2].

This goes well beyond Paper III. The full 3-adic structure — Loewy filtration, lifted idempotent, monogenic presentation, explicit local relations — is invisible at the mod-3 level but governs the automaton's shell dynamics.