Lemma 15.101.1. Let I be an ideal of a Noetherian ring A. Let K \xrightarrow {\alpha } L \xrightarrow {\beta } M be a complex of finite A-modules. Set H = \mathop{\mathrm{Ker}}(\beta )/\mathop{\mathrm{Im}}(\alpha ). For n \geq 0 let
I^ nK \xrightarrow {\alpha _ n} I^ nL \xrightarrow {\beta _ n} I^ nM
be the induced complex. Set H_ n = \mathop{\mathrm{Ker}}(\beta _ n)/\mathop{\mathrm{Im}}(\alpha _ n). Then there are canonical A-module maps
\ldots \to H_3 \to H_2 \to H_1 \to H
There exists a c > 0 such that for n \geq c the image of H_ n \to H is contained in I^{n - c}H and there is a canonical A-module map I^ nH \to H_{n - c} such that the compositions
I^ n H \to H_{n - c} \to I^{n - 2c}H \quad \text{and}\quad H_ n \to I^{n - c}H \to H_{n - 2c}
are the canonical ones. In particular, the inverse systems (H_ n) and (I^ nH) are isomorphic as pro-objects of \text{Mod}_ A.
Proof.
We have H_ n = \mathop{\mathrm{Ker}}(\beta ) \cap I^ nL/\alpha (I^ nK). Since \mathop{\mathrm{Ker}}(\beta ) \cap I^ nL \subset \mathop{\mathrm{Ker}}(\beta ) \cap I^{n - 1}L and \alpha (I^ nK) \subset \alpha (I^{n - 1}K) we get the maps H_ n \to H_{n - 1}. Similarly for the map H_1 \to H.
By Artin-Rees we may choose c_1, c_2 \geq 0 such that \mathop{\mathrm{Im}}(\alpha ) \cap I^ nL \subset \alpha (I^{n - c_1}K) for n \geq c_1 and \mathop{\mathrm{Ker}}(\beta ) \cap I^ nL \subset I^{n - c_2}\mathop{\mathrm{Ker}}(\beta ) for n \geq c_2, see Algebra, Lemmas 10.51.3 and 10.51.2. Set c = c_1 + c_2.
It follows immediately from our choice of c \geq c_2 that for n \geq c the image of H_ n \to H is contained in I^{n - c}H.
Let n \geq c. We define \psi _ n : I^ nH \to H_{n - c} as follows. Say x \in I^ nH. Choose y \in I^ n\mathop{\mathrm{Ker}}(\beta ) representing x. We set \psi _ n(x) equal to the class of y in H_{n - c}. To see this is well defined, suppose we have a second choice y' as above for x. Then y' - y \in \mathop{\mathrm{Im}}(\alpha ). By our choice of c \geq c_1 we conclude that y' - y \in \alpha (I^{n - c}K) which implies that y and y' represent the same element of H_{n - c}. Thus \psi _ n is well defined.
The statements on the compositions I^ n H \to H_{n - c} \to I^{n - 2c}H and H_ n \to I^{n - c}H \to H_{n - 2c} follow immediately from our definitions.
\square
Comments (0)
There are also: