Homological Structure of the Pair Node

For the pair factor

R = Z_3[eta]/(eta^2 - 3 eta),

the three indecomposable torsion-free / CM modules are

B0 = R/(eta),   R,   B3 = R/(eta-3).

Hom table

Hom value
Hom(B0,B0) Z_3
Hom(B0,R) (eta-3)R ≅ Z_3
Hom(B0,B3) 0
Hom(R,B0) B0 ≅ Z_3
Hom(R,R) R
Hom(R,B3) B3 ≅ Z_3
Hom(B3,B0) 0
Hom(B3,R) eta R ≅ Z_3
Hom(B3,B3) Z_3

The cross-branch morphisms vanish:

Hom(B0,B3) = Hom(B3,B0) = 0.

So the two branches do not talk to each other directly; they only communicate through the node module R.

Fundamental exact sequences

The node sits between the two branches through the two quotient sequences

0 -> B3 -> R -> B0 -> 0,
0 -> B0 -> R -> B3 -> 0.

More concretely:

So the node module R is the unique indecomposable object that contains both branches and presents each one as a quotient by the other.

Full singular Hecke order

Since

O_sing ≅ Z_3(V7) ⊕ R,

the full indecomposable CM modules are

Z_3(V7),   B0(V1),   R(node),   B3(V5).

The V7 branch is completely orthogonal to the pair factor at the module level: all cross-Homs vanish by the central idempotent splitting.

That is the finite category we were circling: one isolated smooth branch and one three-object nodal CM category.