Fontaine-Laffaille Theory over Power Series Rings
Abstract.
Let be a perfect field of characteristic . We extend the equivalence of categories between Fontaine-Laffaille modules and lattices inside crystalline representations with Hodge-Tate weights at most of [FL82] to the situation where the base ring is the power series ring over the Witt vectors and a -adically complete ring that is étale over the Tate Algebra .
1. Introduction
Let be a perfect field of characteristic , the ring of Witt-vectors over with its Frobenius automorphism, its fraction field, and the ring of power series over in variables. Let be a “small base ring,” a ring that is -adically completed étale over the Tate algebra, (i.e. the ring of restricted Laurent series over ), for some . Let be an integer such that When the base ring is , Fontaine and Laffaille introduced in [FL82] strongly divisible -lattices, which we now call Fontaine-Laffaille modules, to study -lattices in crystalline representations of with Hodge-Tate weights in Denote this category by . We first recall the definition of a Fontaine-Laffaille module in the classical setting:
Definition 1.
A finite free Fontaine-Laffaille module over is a triple where:
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is a finite free module over
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is a decreasing filtration of such that is a direct summand of for all , ,
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are -semilinear maps whose restriction to is
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Let denote the category of finite free Fontaine-Laffaille modules over . These modules classify lattices within crystalline representations as in the following theorem:
Theorem 2 ([FL82]).
When the functor given by
is an equivalence of categories
The work of Faltings in [Fal89] extended this theory to more general base rings. Our goal is to extend the above theorem to the setting where the base ring is and to the setting of a small base ring .
Let us first recall the representation category in the relative case. Let denote where is a fixed geometric point and is the union of finite -subalgebras of a fixed algebraic closure of such that is étale over Let denote the category of crystalline representations of with Hodge-Tate weights in and we make the analogous definitions over the base ring .
Using recent results of Du, Liu, Moon, and Shimizu in [Du+24] and the category of finite, free Fontaine-Laffaille modules in the relative case first introduced by Faltings in [Fal89] and more recently studied by [LMP23], which we will denote , we obtain the following result (see Definition 9 for the definition of Fontaine-Laffaille modules in the relative case, and see Section 2.3 for a brief review of the period rings and crystalline representations in the relative case):
Theorem 3.
Let be an integer satisfying and let denote either the base ring or . The functor
given by
is an equivalence of categories.
Showing this functor is fully faithful is routine, and the difficulty lies in showing essential surjectivity and specifically associating a Fontaine-Laffaille module to a given lattice inside a crystalline representation.
The key input of [Du+24] is the existence of a Kisin module over the ring associated to an object of . The ring comes equipped with a Frobenius map extending the Frobenius on . We can then define the associated Fontaine-Laffaille module as , but the Kisin module alone is not enough to obtain the full data of a Fontaine-Laffaille module over .
In the classical case, Breuil in [Bre02] studied lattices in crystalline representations of using strongly divisible -modules. To obtain the full data of our Fontaine-Laffaille module, we define in the relative setting to be the -adic completion of the divided power envelope of taken with respect to with or . The ring comes with a canonical divided power filtration and additional structure which will descend to our proposed Fontaine-Laffaille module.
To show the main theorem holds over , we will verify that the data properly descends through the use of two base change maps relating our -module back to the classical theory. Let be the perfection of and , which gives rise to a flat embedding . Let denote reduction moduo . A result of [LMP23] allows us to verify that is an object of by checking that and are Fontaine-Laffaille modules over and in the classical sense.
To show the main theorem holds over , we obtain a result analogous to that of [LMP23] where we can check that is Fontaine-Laffaille at the -adic completion of localizations at maximal ideals. This enables us to use a base change as described in Section 2.2.3 and reduce to the setting where the base ring is .
Recently Würthen in [Wür23] proved this result in the setting of a smooth -adic formal scheme over a mixed characteristic complete discrete valuation ring with perfect residue field. Our work uses different methods to focus on the case where the base ring is more limited, and it is routine to extend the results from a small base ring to accommodate the setting of a smooth, -adic formal scheme.
The work of Imai, Kato, and Youcis in [IKY24],developed simultaneously, uses different methods to obtain a different fully faithful functor between lattices inside crystalline representations and Fontaine-Laffaille modules in a relative setting. Their functor has the advantage of being extendable beyond the Fontaine-Laffaille range, and it yields objects in a nicer category. Our functor has the advantage of being essentially surjective. They also place additional assumptions on the prismatic -crystal, and their technique has not yet been applied to the case where the base ring is a power series ring.
Acknowledgements: The author would like to thank his Ph.D advisor Tong Liu for suggesting the work in this paper, and for his extensive and invaluable guidance, comments, and conversation throughout the production of this paper and its earlier drafts. This paper includes and generalizes the content of the author’s Ph.D. thesis at Purdue University when he was partially supported by the Ross Fellowship of Purdue University and a Summer Research Grant during the summer of 2021.
2. Preliminary Results on some Categories and Functors in the Relative Setting
2.1. Base Ring Conventions
Much of integral -adic Hodge Theory has been established in the relative case in far more generality than Fontaine-Laffaille theory. We present the most general setting we will consider here.
Recall is a perfect field of characteristic Let be a totally ramified extension of with ring of integers . Fix a uniformizer of and let denote the monic minimal polynomial of Write for the -adic completion of the Laurent polynomial ring .
Convention 4.
In order to reference results with maximal generality, we will say is a general base ring if is a -adically complete -algebra which is of the form where is an integral domain obtained from by a finite number of iterations of the operations:
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-adic completion of an étale extension
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-adic completion of a localization;
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completion with respect to an ideal containing .
Our new results will hold for a subset of these general base rings which we describe next:
Convention 5.
We will say a general base ring is small if it is -adically completed étale over for some .
The key strategy for showing our results over small base rings will be to reduce to the case of the power series ring due to the local structure of small base rings described in the following lemma:
Lemma 6.
Let be a small base ring that is -adically compaeted étale over and let be a maximal ideal (note that ). Then , the -adic completion of the localization of at , is isomorphic to .
Proof.
Let be a maximal ideal of , and let denote the -adic completion of the localization of at The ring is a regular Noetherian ring, and thus by Cohen’s Structure Theorem. ∎
We will try to reserve the letter in usual font for referring to such a power series ring, the letter in usual font for a small base ring, and the stylized for a general base ring. We will use the stylized to concisely state results that hold for a small base ring or the power series ring .
When we refer to the “classical” theory we will be referring to the setting where the base ring is : the historically typical setting of -adic Hodge Theory.
We will now describe the Frobenius structure and the category of Galois representations for a general base ring. We will let denote the lift of Frobenius on uniquely determined by . Let denote the union of finite -subalgebras of a fixed algebraic closure of such that is étale over . Set . Let denote the category of finite dimensional vector spaces with continuous action, and let denote the full category of finite free modules equipped with a continuous action of .
Remark 7.
This describes the Frobenius structure for a general base ring, but we will actually take for our base ring in order to use the results of [LMP23] as stated. This is not significant, as we will show the relevant category of Fontaine-Laffaille modules defined below is independent of the choice of Frobenius.
2.2. Important Base Change Maps
Our main technique for developing the Fontaine-Laffaille Theory for new base rings will be to base change to rings where the Fontaine-Laffaille Theory is already known. We describe the important base change maps here.
2.2.1. Shilov Point Base Changes
Let be the perfection of and let . We have a -compatiable, flat embedding . Set , and let be the -adically completed divided power envelope of with respect to which comes equipped with a structure and PD-filtration.
As the Shilov point above forgets the data of the connection , we will also need to consider a second Shilov point with imperfect residue field. Let denote the -adic completion of the localization . Then is a complete discrete valuation ring with imperfect residue field. We define and to be the -adically completed divided power envelope of with respect to
2.2.2. Closed Fiber Base Change of a Power Series Ring
In the case of our base ring , we also have a natural projection given by for every . Showing that the Fontaine-Laffaille Theory holds for will amount to checking it is compatible with the Shilov point base change and the closed fiber base change.
2.2.3. Small Base Ring Base Changes
We will now discuss a base change map from a small base ring to suggested by Lemma 6. Let be a maximal ideal of (recall is regular), and let denote the -adic completion of the localization of at which is isomorphic to by Lemma 6.
This gives us a flat base change ring homomorphism . In order to make this map Frobenius equivariant, though, we must consider to be the lift of the Frobenius on which acts on the as . For example, if , then we must take
By Lemma 12 below, there is a canonical equivalence between the categories of finite, free Fontaine-Laffaille modules over with different Frobenii, so this choice will not impact our results.
2.3. Review of relative period rings and crystalline representations
In this section we briefly review the crystalline period rings and the functor in the relative case. For full details of their constructions, see [Bri08, Chapter 6] for a treatment of the period rings and [Bri08, Chapter 8] for a treatment of relevant functors. Let be a general base ring as in Convention 4. Let be the -adic completion of . Set . Then we define and write for the Teichmüler lift of where is a compatible sequence of -power roots of . Let be the unique surjective -algebra homomorphism lifting the first projection.
Let be the -adic completion of the divided power envelope of with respect to the kernel of . Let denote a (non-trivial) sequence of compatible -power roots of unity (i.e. such that . Let and Let
Let be the extension of to and set to be the -adic completion of the divided power envelope of with respect to the kernel of . Let .
For , we have a functor
which is a finite projetive module of rank at most equipped with a and an integrable connection induced by that on We say that is crystalline if the natural map
is an isomorphism. An object is said to be crystalline if is crystalline. There is also a contravariant version of defined to be
dual to the above covariant version.
2.4. Finite free Fontaine-Laffaille modules
Here we introduce the various categories of Fontaine-Laffaille modules in the relative case, following the work of [Fal89] and [LMP23]. Here we will need to distinguish between the case of the base ring and a small base ring for the statement of some theorems.
Definition 8.
Let be the category whose objects consist of a an -module , a sequence of -modules , and sequences of -linear maps and -semi-linear maps , satisfying the following conditions:
(1) The composition is the map
(2) The map is an isomorphism for
(3) The composition of with is
Morphism between these objects are compatible collections of -linear maps between ’s and ’s.
We write when we consider the category of such modules equipped with an integrable connection for which the are parallel and that satisfies Griffiths transversality. Specifically, when the following conditions hold:
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Griffiths-transversality holds. i.e. the following diagram commutes:
Note that this simplifies to when the are injective.
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The are parallel: as a map from to where is .
We write when and
We will replace “f” with “tor” when working in the setting of -power torsion modules as in [LMP23]. We define these categories analgously when working over small base rings.
Definition 9.
Let denote the full subcategory of such that and are finitely generated and free, each is a direct summand of , for , and generate We call an object in this category a “finite free Fontaine-Laffaille module (over )” or sometimes just a “Fontaine-Laffaille module (over )” for convenience. The tags , , and “tor” are used in the same way as for the big category, and we define the categories analagously for small base rings.
We next recall a main theorem of [LMP23] which we will refine to our finite free setting over the base ring , and we will develop an analogue for small base rings. Recall the Shilov point from Section 2.2.1 and that here is a -compatible, flat embedding . Recall from Section 2.2.2 that there is a natural projection determined by for each . A main theorem of [LMP23] is as follows:
Theorem 10.
[LMP23, Proposition 2.2.5]
Suppose such that each is finite as an -module. Then is in if and only if:
(1) Both and are objects in and respectively.
(2) as -modules.
Lt denote the full subcategory of where and each are finite, free -modules. Then we have:
Proposition 11.
Theorem 10, holds if each “” is replaced with “”
Proof.
If , by tensoring with and and noting that and are finite free -modules, it is clear that (1) and (2) hold.
We can show the reverse direction by reducing to the torsion case. Let be a positive integer. It is clear that and are elements of and , respectively.
By tensoring with , we also see that and are of the same type. Then by Theorem 10, we conclude that is an element of Since and and each is free, we deduce that each is finite free and we have the direct summand condition. Similarly, as generates , the same condition lifts to . ∎
We will now build to a theorem analogous to Theorem 11 but which holds for small base rings. First we will show that the category is independent of the lift of Frobenius.
Lemma 12 ([Fal89]).
Let be such that . Let be two lifts of the natural Frobenius on to which coincide modulo . We write (resp. ) when we are considering with the Frobenius lift (resp. ). Then there is an equivalence between the corresponding categories and , and up to canonical isomorphism, is independent of the lift of Frobenius.
Proof.
We show the result for the torsion categories, and the result for the finite free categories follows via projective limits.
The proof of [Fal89] applies almost identically in the torsion case, but we do not have an étale map from , but we still have that gives the dual basis of -derivations. From there we proceed identically to Faltings. By shifting if necessary, we can assume that , The act on via Given a multi-index , we get an endomorphism of . Let denote , and , and . Comparing divisibility by , we can see this gives a well defined element.
Note that an object is in if and only if the Frobenius on induces an isomorphism where is the right exact functor defined explicitly as the cokernel of the map
where is given by
Equivalently, can be defined as the colimit of the following diagram:
where the right arrows denote the maps and the left arrows denote multiplication by .
Now we define a map . Let , which defines an element of , and it suffices to show is an isomorphism. We define:
Noting that divides , we can confirm that gives a well-defined element of and that this sum converges to in the -adic topology. If , the fraction is obviously well-defined as it forces and If this can be done by writing each in its base representation as and using the well-known identity
Then the -adic valuation of the fraction becomes at least
We can then see that for , . Since , the -adic valuation is nonnegative and thus the original fraction is well-defined, and we can see that grows without bound as does.
As in Faltings, Taylor’s formula shows us that gives a well-defined map. The ’s satisfy transitivity for three different Frobenius lifts by the binomial formula. Applying this to gives us that the are isomorphisms. It is easy to verify that is parallel for the connections. ∎
We are now ready to state the analogue of Theorem 11 for a small base ring :
Theorem 13.
Suppose is in such that each is finite as a -module. Then is in if and only if for all maximal ideals of .
Proof.
Again we show the result in the torsion case and the result in the finite free case follows from taking projective limits.
For the forward direction, it is clear that are finitely generated -power torsion -modules with for since and have these properties over . The axioms of are verified directly by properties of the tensor product and the fact that is -equivariant with our choice of Frobenius. Recalling that is a cokernel and again using that is -equivariant, we obtain an isomorphism Thus induces an isomorphism, and is an object in
For the reverse direction, we are assuming that each is a finite module, so we need only check that is an isomorphism. It suffices to check that this is an isomorphism locally at maximal ideals. Since is a Noetherian local ring and is an ideal contained in , the ring map is faithfully flat. Thus it suffices to check that is an isomorphism for every maximal ideal , which is true by assumption since, as in the previous paragraph, ∎
2.5. Étale -modules
In this section and the next we will work over a general base ring as in Convetion 4. Here we review the theory of étale -modules in the relative case.
Let with Frobenius obtained by setting Let be the -adic completion of with Frobenius extending that on
Definition 14.
An étale (, )-module is a pair where is a finitely generated -module and is a -semilinear endomorphism such that the linearization (i.e. the map for ) is an isomorphism.
Let denote the category of projective étale (, )-modules whose morphisms are -compatible -linear maps and the category with the projective condition replaced by finite free. We now recall how étale (, )-modules relate to Galois representations.
Recall that is chosen compatibly so that and . Set to be the -adic completion of and its tilt. Let and denote the -adic completion of . Write for .
Remark 15.
While we have described in full generality for completeness, for our base ring we will only need to use which has a much more explicit description as
for a fixed choice of compatibly chosen th roots of .
Then we have the following relationship:
Proposition 16.
[Kim15, Prop. 7.7], [Du+24, Prop 2.16] There is a functor from the category of finite free -modules with continuous action to the category which is an exact equivalence of categories. The inverse of is given by
This functor behaves well with respect to base change in the following sense: Let be another base ring equipped with Frobenius satisfying the same conditions as with a -equivariant map . If , then can be considered as a -representation via the map and we have the isomorphism
as étale (, )-modules.
2.6. Kisin Modules
We next review Kisin modules in the relative case and the main result of [Du+24] which provides the key input to the proof of our main theorem.
First we recall the the ring considered in [Du+24]. Let denote the absolute prismatic site of . In full generality, is the ring and is an choice of minimal Eisenstein polynomial of (in our setting, or ). We write for the Breuil-Kisin prism. Then is defined to be the self-product of in and that it satisfies a universal property as follows:
If and if we are given maps such that the maps induced by agree, then there is a map uniquely determined by We will write for the maps . We will also utilize the triple-self product of denoted .
The details of the construction of and a justification that this self-product exists can be found in [Du+24, Example 3.4]. We now introduce the category of free Kisin modules with descent data.
Definition 17 ([Du+24] Definition 3.24).
Let denote the category consisting of triples where
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is a finite -module that is projective away from and saturated.
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is a -semi-linear endomorphism such that has finite -height.
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is an isomorphism of -modules that is compatible with Frobenii and satisfies the cocycle condition over
An object of this category is called an integral Kisin descent datum. If we replace the third piece of data with a map that is an isomorphism of -modules that is compatible with Frobenii and satisfies the cocycle condition over , we call such an object a rational Kisin descent datum. Let denote the full subcateogry consisting of objects with -height and which are finite free over .
Remark 18.
The category is equivalent to the category of completed prismatic -crystals on introduced in [Du+24].
The main theorem of [Du+24] is the following:
Theorem 19 ([Du+24] Prop. 3.25, Theorem 3.28).
There is an equivalence of categories between and .
A main result of [Du+24] is the association of a Kisin module to a crystalline representation:
Theorem 20.
[Du+24, Theorem 4.19] Let be a crystalline representation of with Hodge-Tate weights in , and let be a finite free lattice of stable under the action. Let be the étale (, )-module associated to as in Proposition 16. Then there exists a submodule of stable under Frobenius such that:
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with the induced Frobenius is a Kisin module over of -height .
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If and are as above, we call a Kisin module associated to . On ocassion we will want to forget the structure on the Kisin module.
Remark 21.
In the setting of our base ring , [Du+24, Remark 4.23] shows that the Kisin module associated to a lattice in a crystalline representation is projective. As is a local ring, the Kisin module is thus a free -module. Furthermore, in the setting of a small base ring , the Kisin module associated to a lattice in a crystalline representation is projective (but not necessarily free).
2.7. Base Change of the Kisin Module
Here we will again work over a general base ring to state the base change theorems in full generality.
We recall the following standard fact from commutative algebra:
Lemma 22.
[Du+24, Lemma 3.1] Let be a ring, a flat -module, and submodules of an -module . Then as submodules of , we have
2.7.1. Shilov point base change of the Kisin module
We will now recall the base change properties of the Kisin module. Let be another another general base ring for which there exists a map compatible with Frobenius which makes into an -module.
Theorem 23.
Let be the module and data of the Kisin module associated to the lattice inside the crystalline representation as in Theorem 20 with structure forgotten. Let be the module and data of the Kisin module associated to with structure forgotten, and assume and are finite free. Then gives the module and data of the Kisin module associated to , i.e. .
Proof.
Let denote the étale -module associated to as in Theorem 20. Let denote the Kisin module associated to and its associated étale -module. We have injections and By Proposition 16, we know that and so we also have an injection
Then and are both the module data of Kisin modules lying inside of . We claim there is unique such module data. By [Du+24, Lemma 4.18] and Proposition 16 there is a unique Kisin module associated to the étale -module and thus
as submodules of We also know that
Thus we have contained in the intersection of and . By Lemma 22 and the fact that , this intersection is , concluding the proof as and have the same rank and our maps are all compatible with the structures.
∎
Working in the setting of , set and let be the -adically completed divided power envelope of with respect to . We have induced maps and which confirm that if is an étale -module corresponding to a -stable lattice inside a crystalline representation of then is an étale -module corresponding to a -stable lattice inside a crystalline representation of Then by [Kis06, Lemma 2.1.15] or as a corollary of Theorem 23, we have
Corollary 23.1.
If is a Kisin module associated to a -stable lattice in a crystalline representation of , then is, in the classical setting of [Kis06], a Kisin module associated to a stable lattice in a crystalline representation of .
Remark 24.
Here we are using that is free by Remark 21 and that , which is why the corollary has only been stated for the base ring .
2.8. Breuil Modules
In this section we will work over which is either a small base ring or the power series ring . We define to be the -adically completed divided power envelope of with respect to a choice of minimal polynomial of . The ring comes equipped with a Frobenius map that extends It also comes with its divided power filtration that we will denote Note that for , (just consider the action of on ), so we can set The ring also comes equipped with an integrable connection
Definition 25.
For a positive integer, let be the category whose objects are quadruples where:
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is a finite, projective -module.
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is a decreasing filtration of with , , and
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are -semilinear maps so that the composite is Also, generates
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is a topologically quasi-nilpotent integrable connection which satisfies -Griffiths transversality (see Definition 29 below) and commutes with each as before.
We refer to objects of this category as Breuil modules.
Given a Kisin module , we define the associated Breuil module to be
If such a Kisin module exists for a given Breuil module , we will say that “ arises from a Kisin module.” In the next few sections, we show how the full data of a Breuil module can be constructed on
2.8.1. The filtration from the Kisin module
Definition 26.
Let be a Breuil module that arises from a Kisin module which arises from a crystalline representation. We define a decreasing filtration on via:
and a filtration on via
We have the following lemma which shows that the filtration structure descends integrally:
Lemma 27.
Let be a Breuil module that arises from a Kisin module and let . We can express the filtration on as in Definition 26 as
Proof.
Observe that so we can realize an element of as an element such that is contained in
where we are relying on Lemma 22 (note is projective and hence flat). By comparing elements term-by-term we can show , as needed. Specifically, an element in can be written as
with For this element to be in we must have whenever . But with each whenever , so , as well. ∎
2.8.2. The structure
Definition 28.
Let be a Breuil module that arises from a Kisin module . We can also define a structure by setting to be the composition:
Note the first arrow is well-defined by the definition of It is then clear that the composite is because
2.8.3. The integrable connection
Here we discuss where the connection
arises from, and then we will show it descends to the integral setting.
Let be a Breuil module that arises from a Kisin module with descent datum By Theorem 19 there exists , a lattice inside a crystalline representation corresponding to under the equivalence of categories. Then we consider which is a finite projective -module equipped with an integrable connection , a , and filtration structure which we will denote . Set . Then by [Du+24, Theorem 4.28] there is a -compatible isomorphism . By [Du+24, Theorem 4.2] we can identify with as modules. Also see Lemma 43.
The connection can be further extended to an integrable connection on defined as , and comes equipped with a filtration defined inductively by setting and:
where is the -linear derivation and is the projection as in [Du+24, Theorem 4.2]. By [Du+24, Lemma 4.31], the filtration defined in Definition 26 using the -structure on and the filtration defined above agree and, consequently, satisfies rational -Griffiths transversality as we define below:
Definition 29.
We say the connection satisfies rational -Griffiths transversality if for every
and
where is the derivation given by
If restricts to a connection where the same condition on the filtration holds with replaced by , we say that satisfies integral -Griffiths transversality.
We now show this connection descends to the integral setting.
Proposition 30.
Let be a Breuil module that arises from a Kisin module . Then is stable under and satisfies integral -Griffiths transversality.
Proof.
We consider the base change to the Shilov point with imperfect residue field (defined in Section 2.2.1. Let be the crystalline representation corresponding to the étale -module . By [Moo24, Theorem 4.20] there is a Breuil module associated to .
By [Moo24, p. 10] there exists a Kisin module such that By its uniqueness and Theorem 23 we must have and thus
Thus is stable under its integrable connection Thus the image of under is contained in By Lemma 22:
where can be checked term-by-term as in the proof of Lemma 43 below.
For integral -Griffiths Transversality, we know as it satisfies rational -Griffiths transversality and that because is stable under . We conclude that satisfies integral -Griffiths Transversality from Definition 26. ∎
2.8.4. The functor from Fontaine-Laffaille modules to Breuil modules
In the classical setting, it has already been established as the main result of [Gao19, Theorem 1.1] that there is a “direct” equivalence of categories between Fontaine-Laffaille modules and Breuil modules. We rely on this equivalence when reducing the relative setting to the classical setting. It is also well-known that the same story holds in the classical case as in the above section. There is an equivalence of categories between Kisin modules and lattices inside of crystalline representations. If is a lattice associated to Kisin module , there is a functor such that where is a Fontaine-Laffaille module in the classical sense of [FL82].
In the relative setting there is an analogous “obvious” functor from Fontaine-Laffaille modules to Breuil modules.
Definition 31.
Let . Then we can define the functor , the -adic completion of The additional structure is defined in the natural way as follows:
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where we’ve added an “” tag to a structure if it arises from that appropriate structure on and an “” tag if it arises from the appropriate structure on . Much of our focus will be on trying to reverse this functor: obtaining Fontaine-Laffaille module data from Breuil module data.
In the classical setting, this functor is well-known to be an equivalence of categories and Hui Gao established a direct quasi-inverse in [Gao19, Theorem 1.1]
Remark 32.
Our results will imply that this functor is an equivalence of categories in the setting with base ring , as well.
2.9. Functors to Galois Representations
2.9.1. Definition of
Let Now we recall how the Galois action on and hence
is defined. This is discussed in [LMP23, Section 2.3]. Set on to extend the natural on with Choose to be a fixed sequence of compatible th roots of and denote by its Teichmüller lift. For any we define , and we have for :
where is defined as and is a multi-index with for all and . It follows from [LMP23, Lemma 2.20] that this formula gives a well-defined -semilinear action of which is compatible with the filtration structure (i.e. ) and commutes with the Frobenius structure. This ensures is well-defined and that .
can be defined analogously for but is set to be and we use instead of .
2.9.2. The definition of
Write for . Let be a Kisin module with descent data associated to a crystalline representation. Here we will work over our base ring and explain how the map as in Definition 17 is used to construct a Galois action on as in [DL22, 4.3]. First recall that we have an embedding via .
Let be the map determined by which extends the above embedding of into . Let and let be the map determined by and Then the universal property described in Section 2.6 gives a unique map and since satisfies the cocycle condition there exists a map making the following diagram commute:
and from this we have a action on Alsom the action commutes with the -structure.
We will make use of this action on two separate functors. We define
and
where we write and we set and defined by
These functors are related via
as in [LL23, Lemma 6.11], where denotes the th Tate twist. Their proof only establishes the isomorphism in the classical case, but the proof works mutatis mutandis in the relative case.
Remark 33.
We are using the covariant versions of these functors rather than the contravariant versions used in [Du+24] (defined below) which are dual to the covariant versions. With this in mind, if we take a lattice , we should first consider , the dual with the th Tate twist applied. Then using Theorem 20 as stated for the contravariant versions of the functors, there exists a Kisin module with descent data such that Then taking duals and applying the th Tate twist, we obtain , so we do have a Kisin module with descent data with for our covariant version, too.
Remark 34.
We can define and analogously when working over a small base ring using the analogous embedding of via . Note that the embedding induces an embedding which gives an isomorphism when is a Kisin module over
2.9.3. Equivalence between and
Again let be a Kisin module associated to a crystalline representation. By [Du+24, Lemma 4.27], the natural -equivariant map
is an isomorphism, though we need to make slight adjustments because we are using the covariant versions of these functors as defined above rather than the contravariant versions sometimes used in [Du+24].
Lemma 35.
The natural map
is an isomorphism of representations.
Proof.
Recall
The embedding above extends to an embedding which gives us a natural embedding
The last embedding is known to be an isomorphism of representations as a consequence of [Du+24, Lemma 2.15], completing the proof. ∎
2.9.4. The definition of
Write For Let be a Breuil module. We can define a Galois action on is defined using in the same way as the Galois action on a Fontaine-Laffaille module was defined above. First embed into where maps to , the Teichmuller lift of a compatible sequence of -power roots of . If we let and we set
with notation as above in the previous section and the sum over multi-indices of nonnegative integers. Similarly to Section 2.9.1, this gives us an -semilinear action of which preserves the filtration structure ()) and commutes with Frobenius. It is also clear that if , then
We can also view this Galois action on determined by as one arising from the descent data. We first recall that there are rings and analogous to and . The details of the construction can be found in [Du+24, Example 3.9]. We will write and for the maps from to analogous to the and defined in Section 2.9.2
Given a
Kisin module associated to a lattice in a crystalline representation as in Theorem 20 , [Du+24, Construction 4.3] constructs a descent datum on as follows:
Let be the derivation given by and let be the derivation given by . Then we can define as
where the sum is over multi-indices of nonnegative integers.
This descent datum determines a Galois action on in the same way as the descent datum determined a Galois action on just with and replaced by and . Specifically, let The maps and from Section 2.9.2 extend to embeddings and by the analogous universal property as discussed at the beginning of Section 2.6, there exists a unique map and since satisfues the cocycle condition, there exists a map , depending on , making the diagram commute:
which establishes the desired Galois action on .
So determines a Galois action of on and hence on
We have seen two ways of defining a Galois action on : the first via the descent datum and the second via the connection . Via the explicit formulas and above, we see that the two ways of defining the Galois action are the same.
Remark 36.
We define analogously when working over a small base ring instead of . Writing for and letting be a Breuil module over , we have
2.9.5. Equivalence between and
We will now explore the relationship between and defined in the preceding sections. Continue to assume that is a Kisin module arising from a -crystalline representation of . Let be a Breuil module arising from as in Section 2.8 (recall this means ).
Now consider the natural map
By [Du+24, Prop. 4.6], the map as defined in the previous section (originally constructed in [Du+24, Construction 4.3]) satisfies
Thus we see that and define the same Galois action on , as we discussed how defines a Galois action on using the following diagram:
and defines a Galois action on via the same diagram mutatis mutandi:
Thus we see that the Galois action established on is compatible with the Galois action on via the natural map .
As , it is standard to see from the definitions of the filtration structure on and that the map respects the filtration and structures. This gives us a natural injective map
compatible with the -action, filtration, and , structure.
We will later prove the following theorem:
Theorem 37.
The natural injection
induced by the embedding is an isomorphism of representations.
but we will need information about the Fontaine-Laffaille module associated to which won’t be established until the next section. Nevertheless, we state the result here in our section on Galois representations for completeness.
2.10. A summary of categories
Here we include a brief diagram summarizing the relationship between the many categories introduced above in the setting of our base ring :
2.11. is fully faithful
To conclude Section 2, we will show that is fully faithful. First we work over the base ring .
Let and be Fontaine-Laffaille modules over so that there exists a morphism
of representations. By Proposition 16 there is an equivalence of categories between stable lattices in finite free representations and étale -modules and thus exists a unique morphism where is the étale -module associated to the representation
Moreover, there is a unique morphism between the associated Kisin modules with descent data by [Du+24, Proposition 3.25, Theorem 3.28]. Proposition 3.25 establishes an equivalence of categories between and a category of prismatic -crystals, and Theorem 3.28 establishes that this category of prismatic -crystals is equivalent to . So it suffices to show that induces a map such that agrees with on , which are isomorphic as established above.
Set which is a morphism of the associated Breuil modules. We can then obtain a morphism on the associated Fontaine-Laffaille modules using the unique sections guaranteed by Theorem 43. Let be the section and the section as in the following diagram:
where the bottom map is defined to be the natural projection composed with . Tensoring the above diagram with we see that agrees with If we let denote the map , we obtain a similar diagram
which shows that will agree with
To complete the proof of fully-faithfulness, we need to justify the uniqueness of . This follows from the established rational theory. Such a morphism induces a morphism which is known to be unique as [Du+24, Proposition 4.28] establishes an isomorphism and the induced morphism on is known to be unique by the original theory of Brinon in [Bri08].
Thus we have established:
Theorem 38.
The functor
given by
is fully faithful.
We can also establish fully-faithfulness for small base rings via base change.
We also have the analogous result for the Tate Algebra:
Theorem 39.
The functor
given by
is fully faithful.
Proof.
Let and be Fontaine-Laffaille modules over so that there exists a morphism
of representations. Write for We get an induced map , for which there exists a unique morhphism as is fully faithful with the base ring . We also have a unique induced map , setting up the following diagram: where the vertical maps are injective. But the image of under is contained in , completing the proof of fully faithfulness. ∎
3. Essential Surjectivity of over Power Series Rings
In this section we aim to prove the following two theorems, working over the base ring . Let denote the kernel of the projection given by
Theorem 40.
Let be a Breuil module which arises from a Kisin module which arises from a an object in Set
Then carries the data of a Fontaine-Laffaille module and satisfies as in Definition 31 We call it the “Fontaine-Laffaille module associated to .”
Theorem 41.
Let be the Fontaine-Laffaille module associated to Then
Combined, these theorems complete the proof of essential surjectivity of For the remainder of Section 3, we will assume satisfies the hypotheses of the above theorem.
3.1. Fontaile-Laffaille data on
We will now define the Fontaine-Laffaille data on and show that is indeed a Fontaine-Laffaille module with our key tool being Theorem 11. As modules, we have from Theorem 23 and Proposition 23.1 that and are isomorphic, as modules, to Fontaile-Laffaille modules arising from stable lattices in crystalline representations, so they come equipped with the data of a classical Fontaine-Laffaille module as in Definition 1. We do not yet know, though, whether this data, particularly the filtration data, is compatible with the base change maps. Showing this will be a major focus of this section.
3.1.1. The Filtration and structure on
We first develop the filtration and structure on . The key is to show that the following Lemma from [Du+24] descends to the integral situation:
Lemma 42 ([Du+24] Lemma 4.2).
Consider the projection induced by the -compatible projection , Then admits a unique -compatible section Furthermore, is an isomorphism.
We first prove the following:
Lemma 43.
The projection as in Lemma 42 admits a unique -compatible section
Proof.
To attain this section we base change to the Shilov point obtaining the following commutative diagram:
Note that determines a section . By [Gao19, Prop 3.2.3] this section is unique and it takes , and thus , into . Tracing through the top of the diagram, we see that the image of in is contained in
From Lemma 22, we obtain:
We can verify term by term. If we take in the intersection, we can write it as
with We can also write it as
with Comparing term-by-term we can see that ∎
Lemma 44.
The map is an isomorphism.
Proof.
Since and are finite, free -modules of the same rank, it suffices to show that is surjective. Moreover, is a local ring, so by Nakayama’s Lemma it suffices to show that is surjective after reducing modulo the maximal ideal of which is the ideal generated by , , and the divided powers . After reducing modulo the maximal ideal, becomes the identity map which is obviously surjective. ∎
We now define the filtration and structure on .
Definition 45.
Realizing as a submodule of via the section , we can define
Definition 46.
We set .
Note that the filtration on induces a filtration on for which the composite is . By the corresponding properties on (see Definition 25), it is easy to see that and
Thus has the structure of an object in . We rely on Proposition 11 to show that we have an object of in the following section.
3.2. as Fontaine-Laffaille modules
We need to show that the filtration data on the tensor product is compatible with the filtration on . The difficulty in doing this is establishing a base change theorem for the Breuil module . The ring is very large, so treating as an -module and tensoring with over will not get us back : we would need to -adically complete The fact is non-Noetherian makes -adic completion difficult to work with.
Instead, we can work over the ring which is Noetherian when . This will allow us to decompose and show that is contained in the nicer piece.
Lemma 47.
Let be a nonnegative integer less than . Then we can decompose as follows:
Proof.
Another way to express the definition of is as a kernel in the exact sequence
It follows quickly from the definition of that is contained in the kernel, so we get an exact sequence
We can now tensor with which maintains the exactness since is a flat -module. As a further conesequence of the flatness of , the tensor product commutes with quotients and we obtain the exact sequence:
We also have on the Shilov point the exact sequence
where the rightmost map restricts to the rightmost map of exact sequence via the embedding . We can also see that is in the kernel, so this gives an exact sequence
Now note that
since is a finite, free -module. Also,
Since is a finite, free -module and is a finite, free- module of the same rank, the rightmost maps of and are the same with the same domain. Thus the kernels must be the same.
Since , we obtain that an element in is determined by an element of up to an element in , completing the proof of the lemma. ∎
We now want to use this decomposition to show that elements of cannot arise containing any components. Formally, we have the following lemma:
Lemma 48.
Proof.
Let , which we know to be a subset of This means by Lemma 47 we can write with and . Since , we have that We claim
Let be an -basis of Since , we can write
with Since , we can write
with and Thus,
Then since , we must have
for and then it is clear that and the lemma is proven. ∎
Theorem 49.
Now that we have shown the compatibility of the filtrations, has the full Fontaine-Laffaille module structure of . We thus conclude:
Theorem 50.
is a Fontaine-Laffaille module over , and as Fontaine-Laffaille modules.
3.3. as Fontaine-Laffaille Modules
The strategy in this section is similar to the strategy in the above section where we analyze the Breuil module filtration to understand the Fontaine-Laffaille module filtration, but we have to deal with the additional concern that is not a flat -module, which means analyzing various terms of the form . These Tor terms aren’t too concerning because the barrier to being a flat -module is, effectively, -torsion, which does not show up in most of our modules.
Lemma 51.
We have (for ):
(a)
(b)
(c)
(d)
Proof.
For (a), we compute by recognizing that
is a free resolution of since is a free -module. When tensoring with , it is clear that the first map remains injective, so indeed .
For (b), by Lemma 44, we have that is a direct sum of finitely many copies of , so by part (a).
For part (c), we observe that is (for ) a free -module and hence a free -module. We also know is a free -module, giving us our conclusion.
For Part (d), we have an exact sequence
Below in Lemma 52, we justify that the cokernel of this map
is a finite free -module, hence a free -module.
The following lemma completes the proof of (c):
Lemma 52.
Let be the map induced by Then is a finite, free -module.
Proof.
Write for . We have an exact sequence
Tensoring with , we obtain
where the first map is Then we obtain the following diagram projecting to the level:
from which we conclude that is surjective and that By Lemma 23.1 and the proof of Lemma 51(c) which justifies that and allows us to commute the base change with the quotient,
By tensoring with , we find that is the cokernel of induced by . If , by [GLS14, Theorem 4.20] we know that and where are the Hodge-Tate weights from which it is clear that is a finite free -module of rank, say, .
Let be a basis of as a -module. By Nakayama’s Lemma, we can lift it to which generate as an -module. Analogously, we can see that which, by the same reasoning replacing with , is a free -module of rank . The rank is the same since arises from a crystalline representation. A crystalline representation in the relative case is Hodge-Tate and will have the same Hodge-Tate weights on all of its fibers, so the decomposition of will use the same Hodge-Tate weights as the analogous decomposition of Then the images of in must generate . Therefore they are linearly independent over and, hence, over , as well. Thus is a finite, free -module. ∎
On the Shilov point we had to be concerned that is very large: it is not true that , we would need an additional -adic completion which does not behave nicely over non-Noetherian rings. On the closed fiber we have a little more freedom since is smaller than and this concern is not present on the closed fiber. We can thus obtain a stronger version of Lemma 47 more easily:
Lemma 53.
We have
Proof.
We have the exact sequence
from the definition of , and let be the labelled map. Factoring through the kernel, we obtain the short exact sequence
We now base change to , noting that is a finite, free -module by Lemma 52 and the tensor produdct commutes with the quotients by Lemma 51. We thus obtain the exact sequence
As is exactly the kernel of inside of and is contained in this kernel, the proof of the lemma is complete. ∎
Now that we can reduce the Breuil module filtration to the classical case, we will introduce a second filtration on which behaves a little more nicely under base change. In the classical case, the two filtrations agree, which is what we will show in our power series ring setting.
Definition 54.
Let
be the map determined by . Note this map sends to . Define to be the image of under .
Lemma 55.
Proof.
We first show that . Recall that we set and upon which we can utilize the rational theory. Set We have the exact sequence
The kernel of is by [Du+24, Lemma 4.31], and removing the part ensures that will give the entire kernel. Recalling from the rational theory that
we obtain the exact sequence
(1) |
Since , we have an injective map
On the other hand, this agrees with the map
giving us that
Tensoring with and applying Lemma 53 we obtain the exact
But we also know from the classical theory that is the image of under , so we obtain that and hence is a finite, free -module. Let be a basis and by Nakayama’s Lemma we can lift it to a generating set of . Since is an image after , it is clear that we can safely mod out by to obtain the exact
Now we can safely base change to the Shilov point to obtain
the base change in the first two terms is as written due to Theorem 50 and the classical functor from Fontaine-Laffaille modules to Breuil modules described in Definition 31. Applying the classical theory to the Shilov point, we know and hence is a finite, free module and is of the same rank as . Note that the rank is the same again because of the Hodge-Tate property of crystalline representations. The places where the filtrations of and increase in rank and the amount they increase in rank by are determined completely by the Hodge-Tate weights of the crystalline representation associated to . These are the same on each fiber and, consequently, the ranks of and are the same.
Thus with our embedding , we see that is a basis of and hence is a finite, free -module.
Now we know that is a finite, free -module contained in both and We conclude that
∎
Theorem 56.
Proof.
In the proof of the previous lemma we established that . The result of the previous lemma is that , completing the proof. ∎
This completes the proof of the following theorem:
Theorem 57.
is a Fontaine-Laffaille module over , and as Fontaine-Laffaille modules.
3.4. is an object of
We now complete the proof of Theorem 40:
Proof.
Theorem 58.
is an object of the category .
Proof.
By Theorem 57 and Theorem 20, we only need to show that is stable under and that it satisfies integral Griffiths Transversality.
Using Lemma 42 and Lemma 22 we see that as submodules of We know is stable under (which restricts to on ) and, by Proposition 30, so is , showing that is stable under
Because , is stable under , and satisfies integral -Griffiths transversality by lemma 30 we conclude satisfies Griffiths transversality, as needed. ∎
3.5. Proof of Essential Surjectivity
We now complete the proof that is essentially surjective. Let be an object of . Let be the Kisin module with descent data associated to guaranteed by Theorem 20 (note Remark 33). Note also this theorem associates a Kisin module with descent data to an étale -module with , and then by Lemma 35.
Let be the Breuil module associated with We first prove the following stepping stone to Theorem 37.
Lemma 59.
The natural injection
induced by the embedding is an isomorphism of representations.
Proof.
We prove the lemma by reducing to the Shilov point where we argue as in [Moo24, Lemma 4.7]. First note that using Lemma 35,
is an isomorphism of representations.
Then we obtain the diagram:
where the bottom map is an isomorphism by [LL23, Prop 6.12] and represents the usual from the classical theory. We do not know whether the right vertical map is an injection since the natural map requires a -adic completion. We can, however, extend the diagram to the right because if is the Fontaine-Laffaille module associated to , then the unique section of Lemma 42 and the discussion of Section 2.9.4 induces an isomorphism , and we get a similar isomorphism on the Shilov point. This gives us the diagram:
where the rightmost vertical arrow is an isomorphism by [LMP23, Cor 2.3.5]. Since is an injection, it must then be an isomorphism, completing the proof of the lemma. ∎
The last diagram in the proof of this lemma then establishes that as representations. We now are able to prove Theorem 37 by showing this is actually an isomorphism of representations which comes from the fact that the above maps are compatible with the relevant Galois actions.
The isomorphism is determined by the unique -compatible section , and it is clear that the Galois action on determined by on is compatible with the Galois action on determined by on , confirming that this map is actually an isomorphism of representations.
To see that the map is compatible with the action, [Du+24, Proposition 4.6] confirms that there is a unique descent datum on such that . As the descent data is used to construct the full action in the same way as described in Section 2.9.4 and Section 2.9.2 and this is the same as the Galois action defined via the structure, the Galois action established on is compatible with the Galois action on and thus the map which was previously shown to be an isomorphism of representations is actually an isomorphism of representations, completing the proof of Theorem 37.
From the diagram in the above proof, we have also shown that as representations, which completes the proof of essential surjectivity over .
4. Essential Surjectivity of over small base rings
We will now prove theorems analaogous to those in the last section but in more generality over small base rings. While the results are analogous, the proof is easier because we are able to leverage the theory from the previous section to define a structure via the rational theory, which would be difficult to do for the power series ring. Throughout this section, fix a small base ring. Write and . Let denote the kernel of the projection given by .
4.1. Statement of Main Theorems
Theorem 60.
Let be a Breuil module which arises from a Kisin module which arises from a an object in Set
Then carries the data of a Fontaine-Laffaille module and satisfies as in Definition 31 We call it the “Fontaine-Laffaille module associated to .”
Theorem 61.
Let be the Fontaine-Laffaille module associated to Then
4.2. Preliminaries
Similar to the previous section, our strategy will be to show the Fontaine-Laffaille data is compatible with the base change to discussed in Section 2.2.3 and then to apply Theorem 13. This time we will be able to rely on the rational theory combined with the theory we have established for a power series ring.
Recall that associated to is (which we will denote with in this section), a finite, projective module equipped with a filtration structure , a Frobenius structure , and a structure. We will transfer the data on to in a similar way as how in the last section we transferred the data on to .
By Theorem 23, we can see that and , the Fontaine-Laffaille over associated to are isomorphic as modules (note that is a local ring, and a projective module over a local ring is free). Write for through the remainder of this section.
Lemma 62.
Consider the projection induced by the -compatible projection , . Then admits a unique -compatible section .
Proof.
The proof of Lemma 43 works identically when the base ring is . ∎
This section gives us an injective map and the projection takes to , and thus we have an injective map
4.3. The Filtration Structure
We first define the filtration structure on via the filtration on from the rational theory.
Definition 63.
Set
It remains to show this filtration behaves well under base change.
4.4. The structure
We now define the structure on . Fix a maximal ideal of and again write For As is a Fontaine-Laffaille module, there is a structure on which we will denote . Via our -compatible embedding , we can define a structure on as
Let Note that , and the compatibility of with base change in [Du+24, Lemma 2.13] gives us that acts the same on elements of and sends them into . Thus sends into
by Lemma 22. Since the satisfies , the same holds true for our new structure.
4.5. The Structure
As comes equipped with a structure, set
The proof that is stable under is similar to the proof that is stable under the structure.
We can embed into which is stable under its structure, and we can also embed into which is stable under its structure. As as above, we see that is stable under .
4.6. is essentially surjective over .
Combining the last few subsections, we have equipped with the data of an object in which is compatible with each base change to , completing the proof of Theorem 60 by utilizing Theorem 13. It only remains to show that
Theorem 65.
Proof.
We define a map via the functors to Galois representations from Kisin modules. As , we obtain an injective map
and analogously for . We obtain the diagram
as we also have a map since and and
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