Let
R = Z_3[eta]/(eta^2 - 3 eta)
≅ Z_3 ×_{F_3} Z_3.
Its normalization is
S = Z_3 × Z_3,
and the two branch modules are
B0 = R/(eta) ≅ Z_3 (eta = 0),
B3 = R/(eta - 3) ≅ Z_3 (eta = 3).
The node itself is the third basic module:
R.
Let M be a finitely generated torsion-free R-module. Suppose its ranks on the two branches are (a,b). After scaling inside the total quotient ring one may arrange
3(Z_3^a ⊕ Z_3^b) ⊆ M ⊆ Z_3^a ⊕ Z_3^b.
Set
W = M / 3(Z_3^a ⊕ Z_3^b) ⊂ F_3^a ⊕ F_3^b.
Define
K0 = W ∩ (F_3^a ⊕ 0),
K3 = W ∩ (0 ⊕ F_3^b).
Choose complements
F_3^a = K0 ⊕ U,
F_3^b = K3 ⊕ V.
Then the image of W in U ⊕ V has trivial intersections with the coordinate axes, so it is the graph of an isomorphism U -> V. After independent basis changes on U and V, that graph becomes a diagonal copy Δ^c of F_3^c.
Hence
W ≅ K0 ⊕ Δ^c ⊕ K3,
and therefore
M ≅ B0^u ⊕ R^c ⊕ B3^v
for unique integers
u = dim K0, v = dim K3, c = dim U = dim V.
So the indecomposable torsion-free / CM modules are exactly
B0, R, B3.
For Z_3-rank 2, the gluing space lives in F_3 ⊕ F_3. Up to the unit action (F_3^×)^2, the subspaces are:
orbit in F_3^2 |
representative(s) | resulting module | indecomposable? |
|---|---|---|---|
| zero | 0 |
B0 ⊕ B3 |
no |
| left axis | <(1,0)> |
B0 ⊕ B3 |
no |
| right axis | <(0,1)> |
B0 ⊕ B3 |
no |
| diagonal | <(1,1)>, <(1,-1)> |
R |
yes |
| full plane | F_3^2 |
B0 ⊕ B3 |
no |
Therefore there is no rank-2 indecomposable outside R.
Equivalently, the normalization module
S = Z_3 × Z_3
is not indecomposable; it splits as
S ≅ B0 ⊕ B3.
So the CM-category of the 3-adic Hecke node is finite and completely understood: three indecomposable objects, namely the two branches and the glued node.