In this section we prove our most general results on algebraization of coherent formal modules. We first prove it in case the ideal has cohomological dimension 1. Then we apply this to a blowup to prove a more general result.
Proof.
We will check hypotheses (a), (b), and (c) of Lemma 52.16.10. Before we start, let us point out that the modules H^0(U, \mathcal{F}''_ n) and H^1(U, \mathcal{F}''_ n) are finite A-modules for all n by Local Cohomology, Lemma 51.12.1.
Observe that for each p \geq 0 the limit topology on \mathop{\mathrm{lim}}\nolimits H^ p(U, \mathcal{F}_ n) is the I-adic topology by Lemma 52.4.5. In particular, hypothesis (b) holds.
We know that M = \mathop{\mathrm{lim}}\nolimits H^0(U, \mathcal{F}_ n) is an A-module whose limit topology is the I-adic topology. Thus, given n, the module M/I^ nM is a subquotient of H^0(U, \mathcal{F}_ N) for some N \gg n. Since the inverse system \{ H^0(U, \mathcal{F}_ N)\} is pro-isomorphic to an inverse system of finite A-modules, namely \{ H^0(U, \mathcal{F}''_ N)\} , we conclude that M/I^ nM is finite. It follows that M is finite, see Algebra, Lemma 10.96.12. In particular hypothesis (c) holds.
For each n \geq 0 let us write Ob_ n = \mathop{\mathrm{lim}}\nolimits _ N H^1(U, I^ n\mathcal{F}_ N). A special case is Ob = Ob_0 = \mathop{\mathrm{lim}}\nolimits _ N H^1(U, \mathcal{F}_ N). Arguing exactly as in the previous paragraph we find that Ob is a finite A-module. (In fact, we also know that Ob/I Ob is annihilated by a power of \mathfrak a, but it seems somewhat difficult to use this.)
We set \mathcal{F} = \mathop{\mathrm{lim}}\nolimits \mathcal{F}_ n, we pick generators f_1, \ldots , f_ r of I, we pick c \geq 1, and we choose \Phi _\mathcal {F} as in Lemma 52.4.4. We will use the results of Lemma 52.2.1 without further mention. In particular, for each n \geq 1 there are maps
\delta _ n : H^0(U, \mathcal{F}_ n) \longrightarrow H^1(U, I^ n\mathcal{F}) \longrightarrow Ob_ n
The first comes from the short exact sequence 0 \to I^ n\mathcal{F} \to \mathcal{F} \to \mathcal{F}_ n \to 0 and the second from I^ n\mathcal{F} = \mathop{\mathrm{lim}}\nolimits I^ n\mathcal{F}_ N. We will later use that if \delta _ n(s) = 0 for s \in H^0(U, \mathcal{F}_ n) then we can for each n' \geq n find s' \in H^0(U, \mathcal{F}_{n'}) mapping to s. Observe that there are commutative diagrams
\xymatrix{ H^0(U, \mathcal{F}_{nc}) \ar[r] \ar[dd] & H^1(U, I^{nc}\mathcal{F}) \ar[dd] \ar[rd]^{\Phi _\mathcal {F}} \\ & & \bigoplus _{e_1 + \ldots + e_ r = n} H^1(U, \mathcal{F}) \cdot T_1^{e_1} \ldots T_ r^{e_ r} \ar[ld] \\ H^0(U, \mathcal{F}_ n) \ar[r] & H^1(U, I^ n\mathcal{F}) }
We conclude that the obstruction map H^0(U, \mathcal{F}_ n) \to Ob_ n sends the image of H^0(U, \mathcal{F}_{nc}) \to H^0(U, \mathcal{F}_ n) into the submodule
Ob'_ n = \mathop{\mathrm{Im}}\left( \bigoplus \nolimits _{e_1 + \ldots + e_ r = n} Ob \cdot T_1^{e_1} \ldots T_ r^{e_ r} \to Ob_ n \right)
where on the summand Ob \cdot T_1^{e_1} \ldots T_ r^{e_ r} we use the map on cohomology coming from the reductions modulo powers of I of the multiplication map f_1^{e_1} \ldots f_ r^{e_ r} : \mathcal{F} \to I^ n\mathcal{F}. By construction
\bigoplus \nolimits _{n \geq 0} Ob'_ n
is a finite graded module over the Rees algebra \bigoplus _{n \geq 0} I^ n. For each n we set
M_ n = \{ s \in H^0(U, \mathcal{F}_ n) \mid \delta _ n(s) \in Ob'_ n\}
Observe that \{ M_ n\} is an inverse system and that f_ j : \mathcal{F}_ n \to \mathcal{F}_{n + 1} on global sections maps M_ n into M_{n + 1}. By exactly the same argument as in the proof of Cohomology, Lemma 20.35.1 we find that \{ M_ n\} is ML. Namely, because the Rees algebra is Noetherian we can choose a finite number of homogeneous generators of the form \delta _{n_ j}(z_ j) with z_ j \in M_{n_ j} for the graded submodule \bigoplus _{n \geq 0} \mathop{\mathrm{Im}}(M_ n \to Ob'_ n). Then if k = \max (n_ j) we find that for n \geq k and any z \in M_ n we can find a_ j \in I^{n - n_ j} such that z - \sum a_ j z_ j is in the kernel of \delta _ n and hence in the image of M_{n'} for all n' \geq n (because the vanishing of \delta _ n means that we can lift z - \sum a_ j z_ j to an element z' \in H^0(U, \mathcal{F}_{n'c}) for all n' \ge n and then the image of z' in H^0(U, \mathcal{F}_{n'}) is in M_{n'} by what we proved above). Thus \mathop{\mathrm{Im}}(M_ n \to M_{n - k}) = \mathop{\mathrm{Im}}(M_{n'} \to M_{n - k}) for all n' \geq n.
Choose n. By the Mittag-Leffler property of \{ M_ n\} we just established we can find an n' \geq n such that the image of M_{n'} \to M_ n is the same as the image of M' \to M_ n. By the above we see that the image of M' \to M_ n contains the image of H^0(U, \mathcal{F}_{n'c}) \to H^0(U, \mathcal{F}_ n). Thus we see that \{ M_ n\} and \{ H^0(U, \mathcal{F}_ n)\} are pro-isomorphic. Therefore \{ H^0(U, \mathcal{F}_ n)\} has ML and we finally conclude that hypothesis (a) holds. This concludes the proof.
\square
Proof.
Let Y' \subset X' be the exceptional divisor. Let Z' \subset Y' be the inverse image of Z \subset Y. Then U' = X' \setminus Z' is the inverse image of U. With \delta ^{Y'}_{Z'} as in (52.18.0.1) we set
T' = \{ y' \in Y' \mid \delta ^{Y'}_{Z'}(y') = 1\text{ or }2\} \subset T = \{ y' \in Y' \mid \delta ^{Y'}_{Z'}(y') = 1\}
These are specialization stable subsets of U' \cap Y' = Y' \setminus Z'. Consider the object (b|_{U'}^*\mathcal{F}_ n) of \textit{Coh}(U', I\mathcal{O}_{U'}), see Cohomology of Schemes, Lemma 30.23.9. For y' \in U' \cap Y' let us denote
\mathcal{F}_{y'}^\wedge = \mathop{\mathrm{lim}}\nolimits (b|_{U'}^*\mathcal{F}_ n)_{y'}
the “stalk” of this pullback at y'. We claim that conditions (a), (b), (c), (d), and (e) of Lemma 52.21.2 hold for the object (b|_{U'}^*\mathcal{F}_ n) on U' with d replaced by 1 and the subsets T' \subset T \subset U' \cap Y'. Condition (a) holds because Y' is an effective Cartier divisor and hence locally cut out by 1 equation. Condition (e) holds by Lemma 52.18.1 parts (1) and (2). To prove (b), (c), and (d) we need some preparation.
Let y' \in U' \cap Y' and let \mathfrak p' \subset \mathcal{O}_{X', y'}^\wedge be a prime ideal not contained in V(I\mathcal{O}_{X', y'}^\wedge ). Denote y = b(y') \in U \cap Y. Choose f \in I such that y' is contained in the spectrum of the affine blowup algebra A[\frac{I}{f}], see Divisors, Lemma 31.32.2. For any A-algebra B denote B' = B[\frac{IB}{f}] the corresponding affine blowup algebra. Denote I-adic completion by {\ }^\wedge . By our choice of f we get a ring map (\mathcal{O}_{X, y}^\wedge )' \to \mathcal{O}_{X', y'}^\wedge . If we let \mathfrak q' \subset (\mathcal{O}_{X, y}^\wedge )' be the inverse image of \mathfrak m_{y'}^\wedge , then we see that ((\mathcal{O}_{X, y}^\wedge )'_{\mathfrak q'})^\wedge = \mathcal{O}_{X', y'}^\wedge . Let \mathfrak p \subset \mathcal{O}_{X, y}^\wedge be the corresponding prime. At this point we have a commutative diagram
\xymatrix{ \mathcal{O}_{X, y}^\wedge \ar[d] \ar[r] & (\mathcal{O}_{X, y}^\wedge )' \ar[d]_\alpha \ar[r] & (\mathcal{O}_{X, y}^\wedge )'_{\mathfrak q'} \ar[d] \ar[r]_\beta & \mathcal{O}_{X', y'}^\wedge \ar[d] \\ \mathcal{O}_{X, y}^\wedge /\mathfrak p \ar[r] & (\mathcal{O}_{X, y}^\wedge /\mathfrak p)' \ar[r] & (\mathcal{O}_{X, y}^\wedge /\mathfrak p)'_{\mathfrak q'} \ar[r]^\gamma & ((\mathcal{O}_{X, y}^\wedge /\mathfrak p)'_{\mathfrak q'})^\wedge \ar[d] \\ & & & \mathcal{O}_{X', y'}^\wedge /\mathfrak p' }
whose vertical arrows are surjective. By More on Algebra, Lemma 15.43.1 and the dimension formula (Algebra, Lemma 10.113.1) we have
\dim (((\mathcal{O}_{X, y}^\wedge /\mathfrak p)'_{\mathfrak q'})^\wedge ) = \dim ((\mathcal{O}_{X, y}^\wedge /\mathfrak p)'_{\mathfrak q'}) = \dim (\mathcal{O}_{X, y}^\wedge /\mathfrak p) - \text{trdeg}(\kappa (y')/\kappa (y))
Tracing through the definitions of pullbacks, stalks, localizations, and completions we find
(\mathcal{F}_ y^\wedge )_{\mathfrak p} \otimes _{(\mathcal{O}_{X, y}^\wedge )_\mathfrak p} (\mathcal{O}_{X', y'}^\wedge )_{\mathfrak p'} = (\mathcal{F}_{y'}^\wedge )_{\mathfrak p'}
Details omitted. The ring maps \beta and \gamma in the diagram are flat with Gorenstein (hence Cohen-Macaulay) fibres, as these are completions of rings having a dualizing complex. See Dualizing Complexes, Lemmas 47.23.1 and 47.23.2 and the discussion in More on Algebra, Section 15.51. Observe that (\mathcal{O}_{X, y}^\wedge )_\mathfrak p = (\mathcal{O}_{X, y}^\wedge )'_{\tilde{\mathfrak p}} where \tilde{\mathfrak p} is the kernel of \alpha in the diagram. On the other hand, (\mathcal{O}_{X, y}^\wedge )'_{\tilde{\mathfrak p}} \to (\mathcal{O}_{X', y'}^\wedge )_{\mathfrak p'} is flat with CM fibres by the above. Whence (\mathcal{O}_{X, y}^\wedge )_\mathfrak p \to (\mathcal{O}_{X', y'}^\wedge )_{\mathfrak p'} is flat with CM fibres. Using Algebra, Lemma 10.163.1 we see that
\text{depth}((\mathcal{F}_{y'}^\wedge )_{\mathfrak p'}) = \text{depth}((\mathcal{F}_ y^\wedge )_{\mathfrak p}) + \dim (F_\mathfrak r)
where F is the generic formal fibre of (\mathcal{O}_{X, y}^\wedge /\mathfrak p)'_{\mathfrak q'} and \mathfrak r is the prime corresponding to \mathfrak p'. Since (\mathcal{O}_{X, y}^\wedge /\mathfrak p)'_{\mathfrak q'} is a universally catenary local domain, its I-adic completion is equidimensional and (universally) catenary by Ratliff's theorem (More on Algebra, Proposition 15.109.5). It then follows that
\dim (((\mathcal{O}_{X, y}^\wedge /\mathfrak p)'_{\mathfrak q'})^\wedge ) = \dim (F_\mathfrak r) + \dim (\mathcal{O}_{X', y'}^\wedge /\mathfrak p')
Combined with Lemma 52.18.2 we get
52.22.3.1
\begin{equation} \label{algebraization-equation-one} \begin{aligned} & \text{depth}((\mathcal{F}_{y'}^\wedge )_{\mathfrak p'}) + \delta ^{Y'}_{Z'}(y') \\ & = \text{depth}((\mathcal{F}_ y^\wedge )_{\mathfrak p}) + \dim (F_\mathfrak r) + \delta ^{Y'}_{Z'}(y') \\ & \geq \text{depth}((\mathcal{F}_ y^\wedge )_{\mathfrak p}) + \delta ^ Y_ Z(y) + \dim (F_\mathfrak r) + \text{trdeg}(\kappa (y')/\kappa (y)) - (d - 1) \\ & = \text{depth}((\mathcal{F}_ y^\wedge )_{\mathfrak p}) + \delta ^ Y_ Z(y) - (d - 1) + \dim (\mathcal{O}_{X, y}^\wedge /\mathfrak p) - \dim (\mathcal{O}_{X', y'}^\wedge /\mathfrak p') \end{aligned} \end{equation}
Please keep in mind that \dim (\mathcal{O}_{X, y}^\wedge /\mathfrak p) \geq \dim (\mathcal{O}_{X', y'}^\wedge /\mathfrak p'). Rewriting this we get
52.22.3.6
\begin{equation} \label{algebraization-equation-two} \begin{aligned} & \text{depth}((\mathcal{F}_{y'}^\wedge )_{\mathfrak p'}) + \dim (\mathcal{O}_{X', y'}^\wedge /\mathfrak p') + \delta ^{Y'}_{Z'}(y') \\ & \geq \text{depth}((\mathcal{F}_ y^\wedge )_{\mathfrak p}) + \dim (\mathcal{O}_{X, y}^\wedge /\mathfrak p) + \delta ^ Y_ Z(y) - (d - 1) \end{aligned} \end{equation}
This inequality will allow us to check the remaining conditions.
Conditions (b) and (d) of Lemma 52.21.2. Assume V(\mathfrak p') \cap V(I\mathcal{O}_{X', y'}^\wedge ) = \{ \mathfrak m_{y'}^\wedge \} . This implies that \dim (\mathcal{O}_{X', y'}^\wedge /\mathfrak p') = 1 because Z' is an effective Cartier divisor. The combination of (b) and (d) is equivalent with
\text{depth}((\mathcal{F}_{y'}^\wedge )_{\mathfrak p'}) + \delta ^{Y'}_{Z'}(y') > 2
If (\mathcal{F}_ n) satisfies the inequalities in (3)(b) then we immediately conclude this is true by applying (52.22.3.6). If (\mathcal{F}_ n) satisfies (3)(a), i.e., the (d + 1, d + 2)-inequalities, then we see that in any case
\text{depth}((\mathcal{F}_ y^\wedge )_{\mathfrak p}) + \delta ^ Y_ Z(y) \geq d + 1 \quad \text{or}\quad \text{depth}((\mathcal{F}_ y^\wedge )_{\mathfrak p}) + \dim (\mathcal{O}_{X, y}^\wedge /\mathfrak p) + \delta ^ Y_ Z(y) > d + 2
Looking at (52.22.3.1) and (52.22.3.6) above this gives what we want except possibly if \dim (\mathcal{O}_{X, y}^\wedge /\mathfrak p) = 1. However, if \dim (\mathcal{O}_{X, y}^\wedge /\mathfrak p) = 1, then we have V(\mathfrak p) \cap V(I\mathcal{O}_{X, y}^\wedge ) = \{ \mathfrak m_ y^\wedge \} and we see that actually
\text{depth}((\mathcal{F}_ y^\wedge )_{\mathfrak p}) + \delta ^ Y_ Z(y) > d + 1
as (\mathcal{F}_ n) satisfies the (d + 1, d + 2)-inequalities and we conclude again.
Condition (c) of Lemma 52.21.2. Assume V(\mathfrak p') \cap V(I\mathcal{O}_{X', y'}^\wedge ) \not= \{ \mathfrak m_{y'}^\wedge \} . Then condition (c) is equivalent to
\text{depth}((\mathcal{F}_{y'}^\wedge )_{\mathfrak p'}) + \delta ^{Y'}_{Z'}(y') \geq 2 \quad \text{or}\quad \text{depth}((\mathcal{F}_{y'}^\wedge )_{\mathfrak p'}) + \dim (\mathcal{O}_{X', y'}^\wedge /\mathfrak p') + \delta ^{Y'}_{Z'}(y') > 3
If (\mathcal{F}_ n) satisfies the inequalities in (3)(b) then we see the second of the two displayed inequalities holds true by applying (52.22.3.6). If (\mathcal{F}_ n) satisfies (3)(a), i.e., the (d + 1, d + 2)-inequalities, then this follows immediately from (52.22.3.1) and (52.22.3.6). This finishes the proof of our claim.
Choose (b|_{U'}^*\mathcal{F}_ n) \to (\mathcal{F}_ n'') and (\mathcal{H}_ n) in \textit{Coh}(U', I\mathcal{O}_{U'}) as in Lemma 52.21.2. For any affine open W \subset X' observe that \delta ^{W \cap Y'}_{W \cap Z'}(y') \geq \delta ^{Y'}_{Z'}(y') by Lemma 52.18.1 part (7). Hence we see that (\mathcal{H}_ n|_ W) satisfies the assumptions of Lemma 52.22.1. Thus (\mathcal{H}_ n|_ W) extends canonically to W. Let (\mathcal{G}_{W, n}) in \textit{Coh}(W, I\mathcal{O}_ W) be the canonical extension as in Lemma 52.16.8. By Lemma 52.16.9 we see that for W' \subset W there is a unique isomorphism
(\mathcal{G}_{W, n}|_{W'}) \longrightarrow (\mathcal{G}_{W', n})
compatible with the given isomorphisms (\mathcal{G}_{W, n}|_{W \cap U}) \cong (\mathcal{H}_ n|_{W \cap U}). We conclude that there exists an object (\mathcal{G}_ n) of \textit{Coh}(X', I\mathcal{O}_{X'}) whose restriction to U is isomorphic to (\mathcal{H}_ n).
If A is I-adically complete we can finish the proof as follows. By Grothedieck's existence theorem (Cohomology of Schemes, Lemma 30.24.3) we see that (\mathcal{G}_ n) is the completion of a coherent \mathcal{O}_{X'}-module. Then by Cohomology of Schemes, Lemma 30.23.6 we see that (b|_{U'}^*\mathcal{F}_ n) is the completion of a coherent \mathcal{O}_{U'}-module \mathcal{F}'. By Cohomology of Schemes, Lemma 30.25.3 we see that there is a map
(\mathcal{F}_ n) \longrightarrow ((b|_{U'})_*\mathcal{F}')^\wedge
whose kernel and cokernel is annihilated by a power of I. Then finally, we win by applying Lemma 52.17.1.
If A is not complete, then, before starting the proof, we may replace A by its completion, see Lemma 52.16.6. After completion the assumptions still hold: this is immediate for condition (3), follows from Dualizing Complexes, Lemma 47.22.4 for condition (1), and from Divisors, Lemma 31.32.3 for condition (2). Thus the complete case implies the general case.
\square
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