Exact Jacobson Filtration of the Singular Hecke Order

Using the exact presentation

O_sing = Z_3 e7 ⊕ Z_3 epair ⊕ Z_3 n,
e7^2 = e7,   epair^2 = epair,   e7*epair = 0,
e7*n = 0,    epair*n = n,       n^2 = 3n,

the Jacobson radical is

J = (3e7, 3epair, n).

For every r >= 1, one gets the exact closed formula

J^r = Z_3·3^r e7 ⊕ Z_3·3^r epair ⊕ Z_3·3^(r-1) n.

This immediately gives

O_sing / J      ≅ F_3 e7 ⊕ F_3 epair      (dimension 2),
J / 3 O_sing    ≅ F_3·n                    (dimension 1),
O_sing / 3 O_sing has dimension 3.

So the intrinsic finite residue split is exactly:

After that, the J-adic tower is infinite and every deeper graded piece has width 3.

layer generators of J^r dim J^r/J^(r+1)
1 3^1 e7, 3^1 epair, n 3
2 3^2 e7, 3^2 epair, 3^1 n 3
3 3^3 e7, 3^3 epair, 3^2 n 3
4 3^4 e7, 3^4 epair, 3^3 n 3
5 3^5 e7, 3^5 epair, 3^4 n 3
6 3^6 e7, 3^6 epair, 3^5 n 3

Associated graded multiplication

If

alpha_r = [3^r e7],
beta_r  = [3^r epair],
gamma_r = [3^(r-1) n],

in J^r/J^(r+1), then

alpha_r alpha_s = alpha_(r+s),
beta_r beta_s   = beta_(r+s),
alpha_r beta_s  = 0,
alpha_r gamma_s = 0,
beta_r gamma_s  = gamma_(r+s),
gamma_r gamma_s = gamma_(r+s).

So the nilpotent residue class n mod 3 is only first-order nilpotent after reduction modulo 3; in the full J-adic algebra it propagates indefinitely through the relation n^2 = 3n.