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.
T2 has characteristic/minimal polynomial of degree 13 (= dim S2(Γ0(163))). The discriminants are:
| Order | Discriminant |
|---|---|
| Full Hecke order T | 215 · 32 · 65657 · 82536739 |
| Monogenic order Z[T2] | 215 · 38 · 65657 · 3740832 · 82536739 |
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.
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.
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:
| Modulus | Local relation | Unit uk |
|---|---|---|
| mod 27 (33) | y2 = 9 | 1 |
| mod 81 (34) | y2 = 36 | 4 |
| mod 243 (35) | y2 = 198 | 22 |
| mod 729 (36) | y2 = 441 | 49 |
After the shift y = n − (bk/2)u0, the linear term vanishes exactly modulo each 3k, and the local factor takes the monogenic form:
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).
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.
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].