Wach models and overconvergence of \'etale $(\varphi, \Gamma)$-modules
Hui Gao

TL;DR
This paper provides a new proof that all étale $(,g)$-modules over a finite extension of $Q_p$ are overconvergent, and establishes an explicit lower bound for the overconvergence radius using Wach models.
Contribution
It offers an alternative proof of overconvergence for étale $(,g)$-modules and introduces a uniform lower bound for the overconvergence radius based on Wach models.
Findings
All étale $(,g)$-modules are overconvergent over finite extensions of $Q_p$
Explicit lower bound for the overconvergence radius established
Method uses Wach models in modulo $p^n$ Galois representations
Abstract
A classical result of Cherbonnier and Colmez says that all \'etale -modules are overconvergent. In this paper, we give another proof of this fact when the base field is a finite extension of . Furthermore, we obtain an explicit ("uniform") lower bound for the overconvergence radius, which was previously not known. The method is similar to that in a previous joint paper with Tong Liu. Namely, we study Wach models (when is unramified) in modulo Galois representations, and use them to build an overconvergence basis.
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Taxonomy
TopicsRings, Modules, and Algebras · Advanced Topics in Algebra · Homotopy and Cohomology in Algebraic Topology
Wach models and overconvergence of étale -modules
Hui Gao
Department of Mathematics and Statistics, University of Helsinki, FI-00014, Finland
Abstract.
A classical result of Cherbonnier and Colmez says that all étale -modules are overconvergent. In this paper, we give another proof of this fact when the base field is a finite extension of . Furthermore, we obtain an explicit (“uniform”) lower bound for the overconvergence radius, which was previously not known. The method is similar to that in a previous joint paper with Tong Liu. Namely, we study Wach models (when is unramified) in modulo Galois representations, and use them to build an overconvergence basis.
Key words and phrases:
Overconvergence, Wach modules
1991 Mathematics Subject Classification:
Primary 14F30,14L05
The author is partially supported by a postdoctoral position funded by Academy of Finland through Kari Vilonen.
Contents
- 1 Introduction
- 2 -modules, Wach modules, and overconvergence
- 3 Torsion Wach models
- 4 Overconvergent basis and main theorem
1. Introduction
1.1. The classical theorem of Cherbonnier-Colmez
Let us first set up some notations. Let be a prime. Let be a perfect field of characteristic , its ring of Witt vectors, , and a totally ramified finite extension with the ramification index. We fix an algebraic closure of and set . Define inductively such that is a primitive -th root of unity and , and let . Let , and .
Let be a finite free -representation of of rank . In [Fon90], for each such is associated an étale -module where
[TABLE]
See §2 for any unfamiliar terms and more details. Here is a certain “period ring”. For the -representation , we can also define its “overconvergent periods” via:
[TABLE]
where , and is the “overconvergent period ring”. We say that is overconvergent if it can be recovered by its “overconvergent periods”, i.e., if for some , we have
[TABLE]
The main theorem of [CC98] is the following:
1.1.1 Theorem** ([CC98]).**
For any finite free -representation of , its associated -module is overconvergent.
1.1.2 Remark*.*
The theorem was also reproved (and generalized to family version) by Berger and Colmez [BC08]. There is also a relatively more direct proof by Kedlaya [Ked15].
1.2. A reproof when is finite
In this paper, we give another proof of Theorem 1.1.1 when is a finite extension of . Furthermore, we obtain an explicit “uniform” lower bound (depending only on where ) on the overconvergence radius, which was previously not known.
1.2.1 Theorem**.**
Suppose is a finite extension. Let be a finite free -representation of of rank . Then is overconvergent on the interval
[TABLE]
i.e., (1.1.1) holds for (see §2.4 for our conventions).
1.2.2 Remark*.*
- (1)
We need in order to apply the loose crystalline lifting results in [GL], see [GL, Rem. 1.1.2(1)] for some remarks on this condition. 2. (2)
There are some results concerning the overconvergence radius in [BC08, §4.2] (cf. [BC08, Lem. 4.2.5, Prop. 4.2.6]). We will show that using loc. cit., together with results from [GL] and [CL11], we can also prove a certain “uniform overconvergence” (but only implicitly); see §4.3 for more details.
1.2.3 Remark*.*
It is interesting to mention that in [GP], another proof of the overconvergence property of étale -modules is given (which works without assuming ); however, the proof makes full use of Thm. 1.1.1.
The overconvergence theorem 1.1.1 plays a fundamental role in the application of -modules to study various problems, see, e.g., [GL, §1.2] for some discussion. In particular, as we mentioned in loc. cit, overconvergence helps to link the category of all Galois representations to the category of geometric (i.e., semi-stable, crystalline) representations. Similarly as in [GL], we will already use such a link to prove Theorem 1.2.1. Namely, we use crystalline representations to “approximate” general Galois representations. By writing this paper, we hope that our approach can shed some more light on the deeper meaning of overconvergence. We also hope that this paper can serve as a useful companion to the paper [GL], so that the readers can compare between the setting of -modules and -modules.
1.3. Strategy of proof
As we mentioned earlier, the strategy is similar to [GL], with one particular caveat. Namely, for a lattice in a crystalline representation of , we can always attach a -module by the main result of [Liu10], but we can not always attach a Wach module. Fortunately, when is unramified, i.e., when , we can always attach a Wach module (we have to be careful here to avoid a “circular reasoning”, see Remark 2.2.4 for more details). Now, by an argument in [CC98], overconvergence of Galois representations is insensitive to inductions (of representations); thus it suffices to prove Theorem 1.2.1 when , where we always have Wach modules (for crystalline representations). Then the strategy (indeed, the proof itself) will be parallel to [GL], except a few minor changes (in particular, the -action on period rings, cf. §2.3.5).
Let us give a quick sketch of the strategy here (very similar to [GL, §1.3]). We assume is finite and in this paragraph. By the loose crystalline lifting theorem in [GL], we can easily deduce that for each , admits a unique maximal liftable Wach model. Then we can analyse these models, and use them to build an overconvergence basis to prove the theorem.
1.4. Structure of the paper
In §2, we collect basic facts about étale -modules and Wach modules. We define what it means for an étale -module to be overconvergent, and state the theorem of Cherbonnier-Colmez. In §3, when is finite and , we show the existence of Wach models, and analyse their various properties. Finally in §4, we build an overconvergence basis to prove the main theorem; we also make some comparison with known proofs of overconvergence.
1.5. Notations
1.5.1. Some notations in -adic Hodge theory
We put , equipped with its natural coordinate-wise action of . Let be its fraction field. There is a unique surjective projection map to the -adic completion of , which lifts the projection onto the first factor in the inverse limit. Let , , be the usual period rings.
Recall that we defined inductively such that is a primitive -th root of unity and . Set . Let be the Techmüller representative, and as usual. Let with Frobenius extending the arithmetic Frobenius on and . We can embed the -algebra into by the map . This embedding extends to an embedding which is compatible with Frobenious endomorphisms.
1.5.2. Fontaine modules and Hodge-Tate weights
When is a semi-stable representation of , we let where is the dual representation of . The Hodge-Tate weights of are defined to be such that . For example, for the cyclotomic character , its Hodge-Tate weight is .
1.5.3. Some other notations
Throughout this paper, we reserve to denote Frobenius operator. We sometimes add subscripts to indicate on which object Frobenius is defined. For example, is the Frobenius defined on . We always drop these subscripts if no confusion will arise. Let be a ring endowed with Frobenius and a module over . We always denote . Note that if has a -semi-linear endomorphism then is an -linear map. We also reserve to denote valuations which is normalized so that . Finally always denotes the ring of -matrices with entries in and denotes the -identity matrix.
Acknowledgement. I thank Laurent Berger and Tong Liu for some useful discussions. I also thank the anonymous referee(s) for helping to improve the exposition.
2. -modules, Wach modules, and overconvergence
In this section, except in §2.5 (the final subsection), we will let be as in §1.1, i.e., is not necessarily finite.
In this section, we first collect some basic facts on (integral and torsion) étale -modules, étale -modules, Wach modules and their attached representations. Then, we define what it means for an étale -module to be overconvergent, and state the classical overconvergence theorem.
2.1. Étale -modules and -modules
Let be the -adic completion of . Our fixed embedding determined by uniquely extends to a -equivariant embedding , and we identify with its image in . We note that is a complete discrete valuation ring with uniformizer and residue field as a subfield of . Let denote the fractional field of , the maximal unramified extension of inside and the ring of integers. Set the -adic completion of and .
Let , and so acts on it. When (i.e., is unramified), we actually have (see e.g., first paragraph of [Ber04, §I.2]); in this case, we have for .
2.1.1 Definition**.**
Let denote the category of finite type -modules equipped with a -semi-linear endomorphism such that is an isomorphism. Morphisms in this category are just -linear maps compatible with ’s. We call objects in étale -modules.
2.1.2.
Let (resp. ) denote the category of finite type -modules with a continuous -linear (resp. )-action. For in , define
[TABLE]
For in , define
[TABLE]
2.1.3 Theorem** ([Fon90, Prop. A 1.2.6]).**
The functors and induces an exact tensor equivalence between the categories and .
2.1.4 Definition**.**
An étale -module is a triple where
- •
is an étale -module;
- •
is a continuous -semi-linear -action on which commutes with .
2.1.5 Convention**.**
Since we also use to denote an étale -module, we will now use to denote an étale -module. Clearly, this notation compares with the étale -modules that we use in [GL].
For an étale -module , define
[TABLE]
which is a -representation. For in , define
[TABLE]
which is an étale -module.
2.1.6 Theorem** ([Fon90]).**
The functors and induces an exact tensor equivalence between the categories and .
2.2. Wach -modules and Wach modules
In this subsection, we assume . As we mentioned earlier, we have in this case. We write
[TABLE]
2.2.1 Definition**.**
For a nonnegative integer , we write for the category of finite-type -modules equipped with a -semilinear endomorphism satisfying
- •
the cokernel of the linearization is killed by ;
- •
the natural map is injective.
Morphisms in are -compatible -module homomorphisms.
We call objects in Wach -module of height . The category of finite free Wach -modules of height , denoted , is the full subcategory of consisting of those objects which are finite free over . We call an object a torsion Wach -module of height if is killed by for some .
For any Wach -module , we define
[TABLE]
2.2.2 Definition**.**
A finite free (resp. torsion)Wach module of height is a triple , where
- (1)
is a finite free (resp. torsion) Wach -module of height ; 2. (2)
is a continuous -action on which commutes with ; 3. (3)
acts on trivially.
For any Wach module , we can attach a -module via
[TABLE]
2.2.3 Theorem**.**
[Ber04, KR09]** The functor induces an anti-equivalence between the category of finite free Wach modules of height and the category of -stable -lattices in crystalline representations with Hodge-Tate weights in .
2.2.4 Remark*.*
The above theorem in this form is first proved by Berger [Ber04, Thm. 2], which critically uses results by Wach and Colmez [Wac96, Col99]. However, the work in [Col99] (which proves that crystalline representations are of finite height) uses the overconvergence theorem in [CC98].
Fortunately, there is a second proof of the above theorem by Kisin and Ren ([KR09, Thm. 0.1]), which is similar to [Kis06] (and does not use results in [CC98]). Note that both [Kis06] and [KR09] use Kedlaya’s result on slope filtration over the Robba ring ([Ked04]), but that is independent of [CC98].
In summary, by citing [KR09, Thm. 0.1] for Theorem 2.2.3, there would be no circular reasoning in our paper to reprove overconvergence theorem of [CC98].
2.2.5 Convention**.**
From now on in this paper, by a crystalline representation, we always mean a crystalline representation with non-positive Hodge-Tate weights.
2.2.6.
For any integer , let denote the Wach -module corresponding to via our Theorem 2.2.3. It is easy to check that this is a rank-1 -module with a base so that . For any Wach -module , we denote . So .
2.3. Wach -models and Wach models
In this subsection, we assume . As we mentioned earlier, we have in this case.
2.3.1 Definition**.**
- (1)
Given an étale -module in . If is a Wach -module so that , then is called a Wach -model of , or simply a model of . 2. (2)
Given a torsion (resp. finite free) -module. A torsion (resp. finite free) Wach module is called a model of if is a model of and the isomorphism is compatible with -actions on both sides.
The following lemma is obvious.
2.3.2 Lemma**.**
- (1)
If is a model of , then as -modules. 2. (2)
If is a model of then as -modules.
Clearly, the most natural models of étale -modules come from lattices in crystalline representations.
2.3.3 Lemma**.**
Suppose is a -stable -lattice in a crystalline representation of with Hodge-Tate weights in . Let be the -module associated to . Let be the Wach-module associted to . Then is a model of .
Proof.
Easy. ∎
Now suppose that is a -power torsion representation of , and the étale -module associated to . A natural source of Wach -models of comes from the following. Suppose that we have a surjective map of -representations where is a crystalline finite free -representation, then it induces the surjective map (which we still denote by ) , where is the étale -module associated to . If is the Wach -module associated to , then by Lemma 2.3.3 above, is a Wach -model of . And so is clearly a Wach -model of .
2.3.4 Example**.**
Let be the trivial -representation and denote the corresponding trivial étale -module. Then is a model of which is realized by the surjection . We also have another surjection , which realizes another model . It is easy to check that .
2.3.5. Comparison between Kisin modules and Wach -modules
Let us compare the following two situations:
- (1)
(Situation 1.) Kisin modules (see, e.g., [GL, §2] for more details) for a general where (and let us fix a uniformizer of , with Eisenstein polynomial of degree ). Note that in this case. 2. (2)
(Situation 2.) Wach -modules when . Recall that of degree . Note that in this case.
The theories in these two situations have lots of similarities. In particular, when we prove something for Wach -modules, the proof could be almost verbatim as the corresponding result for Kisin modules; oftenly, we only need to change the in Situation 1 to in Situation 2 (and some other slight modifications). We already see this in §2.2.6 (compare with [GL, Ex. 2.3.4]). More notably, when we are in modulo situations, note that and ; then oftenly, we only need to change in Situation 1 to in Situation 2 to prove results about Wach modules. We already see this in Example 2.3.4 (compare with [GL, Ex. 2.4.4]). Here is another illustration of the general phenomenon (switch between and ):
- •
Given a -torsion Kisin module in (Situation 1) of -height (cf. [GL, §2]), let be the matrix for , then there exists such that .
- •
Given a -torsion Wach -module in (Situation 2) of -height , let be the matrix for , then there exists such that .
2.4. Overconvergence
In this subsection, we let be as in §1.1.
For any , we can write with . Denote the valuation on and normalized by
[TABLE]
For any , set
[TABLE]
It turns out that is a ring, stable under -action but not Frobenius, namely . See [CC98, §II.1] for more details. For any subring , denote
[TABLE]
Recall that for a finite free -representation of , we can associate the -module via:
[TABLE]
Now for any , we define
[TABLE]
2.4.1 Definition**.**
For a finite free -representation of , its associated -module is called overconvergent if there exists such that
[TABLE]
In particular, if above holds, we say that is overconvergent on the interval .
The main theorem of [CC98] is the following:
2.4.2 Theorem** ([CC98]).**
For any finite free -representation of , its associated étale -module is overconvergent.
The following lemma says that we can reduce the proof of Theorem 2.4.2 to the case when .
2.4.3 Lemma**.**
To prove Theorem 2.4.2, it suffices to prove the cases when is unramified.
Proof.
Suppose we have already proved Theorem 2.4.2 when the base field is unramified. Now let be any field with . Given a finite free -representation of of rank , then the induction is a finite free -representation of of rank . By assumption, is overconvergent as a -representation. By [CC98, Thm. II. 3.2.(i)] is overconvergent as a -representation. By Mackey decomposition, contains as a direct summand, and so has to be overconvergent as a -representation too. Note that if is overconvergent on the interval as a -representation, then is also overconvergent on the interval as a -representation ∎
2.5. A reproof when is finite extension
The main result of our paper is:
2.5.1 Theorem**.**
Suppose is a finite extension, and let . Let be a finite free -representation of of rank . Then is overconvergent on the interval
[TABLE]
By Lemma 2.4.3, it suffices to prove Thm. 2.5.1 when . Then the main input will be Theorem 4.1.1 (which is analogue of [GL, Thm. 6.1.1]), which says that there exists an “overconvergent basis” of , with respect to which all entries of matrices for and are overconvergent elements.
2.5.2 Remark*.*
- (1)
As we can see from (2.5.1), we have obtained a “uniform” lower bound of overconvergence radius for all -adic Galois representations, once we fix . It is very possible that this uniform bound can have applications to situations where we consider a “family” of Galois representations (where are naturally fixed). 2. (2)
However, let us also mention that it seems almost impossible to use methods in this paper to reprove the overconvergence property of the family of -modules attached to a family of Galois representations (as in the setting of [BC08]); indeed, it seems impossible to construct and study loose crystalline liftings of a family of residual representations. (This does not contradict with the potential usefulness mentioned in Item 1 above.) 3. (3)
Actually, we only need to prove the case to deduce the full Theorem 2.5.1. So for example, we can consider inductions of the form . This will not save much trouble for us (besides, we still use some finite unramified extensions in e.g. Lemma 3.1.8).
3. Torsion Wach models
In this section, we always assume is a finite extension and . We study liftable Wach -models in torsion étale -modules.
3.1. Maximal Wach models and devissage
For , suppose is a -torsion representation of ( is not necessarily free over ). Let be the étale -module corresponding to . Recall that in the torsion case, a Wach -module is called a Wach -model if .
3.1.1 Definition**.**
A Wach -model is called loosely liftable (in short, liftable), if there exists a -stable -lattice inside a crystalline representation and surjective map such that the corresponding map of étale -modules satisfies , where and are the étale -modules and Wach modules for (see the discussion before Example 2.3.4). In this case, we say that can be realized by the surjection .
3.1.2 Definition**.**
Let be a finite extension of , its ring of integers, a uniformizer, the maximal ideal and the residue field.
- (1)
For a torsion representation, we say that a continuous representation is a strict -lift of if . 2. (2)
For a -torsion representation of the form , we say that “ is big enough” (for ) if each direct summand of has strict crystalline -lift with non-positive Hodge-Tate weights.
3.1.3 Theorem**.**
Suppose is a -torsion representation of ( is not necessarily free over ), then it admits loose crystalline lifts, i.e., there exists a -stable -lattice inside a crystalline representation and surjective map . Furthermore, if we let and suppose is big enough for , then we can always make the loose crystalline lift to be finite free over .
Proof.
This is [GL, Thm 3.3.2]; let us sketch the proof here. We hope it can serve as a quick guide for readers not familiar with the proof of loc. cit.; also, we will use many of the (intermediate) results later in §3.2.
Step 1: case. Let be the degree unramified extension of , where ; let be the ring of integers and let be the residue field.
- •
By [GL, Lem. 3.1.3], is big enough for (cf. Def. 3.1.2).
- •
Then [GL, Thm. 3.2.1] shows that there exists a finite unramified extension of , such that the restriction of to admits a strict crystalline -lift . Then is a loose crystalline lift of .
Step 2: induction argument. Now suppose our theorem is true for , and consider the case .
- •
Denote . By induction hypothesis, let be a loose crystalline lift. Let be the cartesian product of and . We have the following diagram of short exact sequences (of -modules).
[TABLE]
Let , then one readily checks that the following is short exact:
[TABLE]
- •
Let be the “big enough” field for the -torsion representation as in Step 1. Since , is also big enough for . By Step 1, there exists finite unramified such that there exists a strict crystalline -lift . Also, is a strict crystalline -lift of . Via (Statement B) in the proof of [GL, Thm. 3.2.1] (which constructs extensions of strict crystalline lifts), we can find some finite unramified extension such that we have the following diagram of short exact sequences of -representations:
[TABLE]
where the first row are strict crystalline -lifts of the second row, and the maps from the second row to the third row are compatible projections to chosen -direct summands. Here we can easily compute that we can choose
[TABLE]
where .
- •
Define , where comes from diagram (3.1.3). The -representation sits in the following diagram of short exact sequences:
[TABLE]
One easily sees that is -finite free and crystalline. Furthermore maps surjectively onto , and so onto . Finally, is the desired loose crystalline lift of .
∎
3.1.4 Lemma**.**
- (1)
For any (coming from ), a liftable model exists. 2. (2)
The set of liftable models inside has a unique maximal object (with respect to the obvious inclusion relation). (We denote the maximal liftable model as ).
Proof.
Item (1) follows from Thm. 3.1.3. Item (2) follows from similar argument as in [GL, Lem. 4.1.2]; let us sketch the argument for the reader’s convenience. Denote the set of all liftable models inside as . It is trivial to see that admits finite supremum. Then it suffices to show that there is an upper bound for length of any chain in ; this is the content of [CL09, Lem. 3.2.4], which we need to reprove in our Wach -module setting. The proof is verbatim, if we change all (resp. ) in loc. cit. to (resp. ) (cf. §2.3.5). ∎
3.1.5.
Now let us introduce some notations. Let be a -finite free -representation, and set . Let be the finite free étale -module corresponding to , and set . Denote the natural projection for induced by modulo . Recall that we use to denote the maximal liftable Wach -model of . Set .
For , we denote the injective map where for , we choose any lift , and let . This is clearly well-defined, and we will use it to identify with (recall that the notation denotes the -torsion elements). The maps are clearly transitive; namely, . Also, the composite
[TABLE]
is precisely the map .
Let be a torsion Wach -module such that . Following the discussion above [Liu07, Lem. 4.2.4], for each , we define
[TABLE]
3.1.6 Lemma**.**
We use the above notations. In particular, for , we identify with . Then we have:
- (1)
* as Wach -models of .* 2. (2)
We have for .
Proof.
The proof is strictly verbatim as in [GL, Lem. 4.1.5, Cor. 4.1.6]; let us sketch the main ideas. Suppose realizes . Let be the composite map where the second map is the map, and let . Then the induced loose crystalline lifting realizes , and thus . For the other direction, note that is a liftable model in . So we have , and so .
For Item (2), note , which equals to (=) by Item (1). ∎
3.1.7.
Suppose is a -torsion representation of , the corresponding étale -module. Suppose is a finite unramified extension of , with residue field and ring of integers . Then it is easy to see that is the corresponding étale -module for .
3.1.8 Lemma**.**
Use notations as in 3.1.7, and use to denote the maximal liftable model of . Then we have .
Proof.
This is the -analogue of [GL, Lem. 4.2.10]. Similarly as the beginning of [GL, §4.2], we need to set . Since we have (because is unramified), we still have , where . Then all the argument in [GL, §4.2] carry over verbatim. ∎
3.2. Existence of
3.2.1 Proposition**.**
Use notations in 3.1.5. Then there exists a constant only depending on , and such that for all . Consequently for all by Lemma 3.1.6(2).
Proof.
The proof is basically the same as that for [GL, Prop. 5.2.1], except a few minor changes (mainly due to the difference of Frobenius actions, cf. §2.3.5). For the reader’s convenience, we give a sketch of the main arguments; in particular, we point out the changes in our situation.
By Lemma 3.1.8, for any , if we let (where is any finite extension), then the maximal liftable Kisin model of is . Thus, it is easy to see that for any . So to prove our proposition, it suffices to show that
[TABLE]
We divide the following argument into two steps. In Step 1, we will construct another Kisin model (denoted as ) of such that . Then in Step 2, we show that
Step 1. The loose crystalline lift realizes a liftable Kisin model of , and so . The following composite of -representations
[TABLE]
realizes a Kisin model in , and we certainly have
[TABLE]
By some elementary diagram chasing (using (3.1.1), (3.1.5) and (3.1.3); cf. [GL, Prop. 5.2.1] for the chasing), the composite (3.2.1) is the same as
[TABLE]
And so (3.2.2) also realizes .
Step 2. The last surjection of (3.2.2) is induced by the following composite of -representations:
[TABLE]
We may assume that realize ; thus the composite (3.2.3) restricted to realizes .
So in order to prove , it suffices to show
[TABLE]
And so it suffices to show that the cokernel of the following composite (which are maps of Wach modules corresponding to (3.2.2)) is killed by
[TABLE]
By the Wach module analogue of [GL, Lem. 5.2.2] (the proof in the Wach module setting is strictly verbatim), the map is in fact surjective, so we only need to consider the cokernel of the following composite of maps:
[TABLE]
Denote the image of the composite (3.2.6) as , which is contained in . So we can choose basis of , such that has a -basis formed by , where
[TABLE]
Here, the expression of “” in (3.2.7) is different from that in [GL] (below [GL, Eqn. (5.2.5)]). This is essentially because in loc. cit., [GL, Ex. 2.4.4] is (implicitly) used; whereas in our situation, we use our corresponding Ex. 2.3.4.
Finally, it suffices to bound ; the proof follows similar ideas as in [GL, Lem. 5.2.6].
Convention: In the remaining of the proof, all the representations that we consider are -representations, and all Wach modules are over . To be completely rigorous, we will need to restrict many representations from to , and use prime notation over Wach modules (i.e., notations like ). For notational simplicity, we will drop these prime notations.
- •
Firstly, given any -torsion Wach -module (over ), denote (similarly as in [GL, Def. 5.2.4])
[TABLE]
The invariant is well-defined, and is additive with respect to short exact sequences (as in [GL, Lem. 5.2.5(1)]). Furthermore, if is a -stable -lattice in a crystalline representation with non-positive Hodge-Tate weights , and the corresponding Wach module, then by the proof of [Ber04, III. 3.1], we have
[TABLE]
Note that (3.2.8) is the Wach module analogue of [GL, Lem. 5.2.5(2)].
- •
Now, recall that has a -basis formed by , where is a -basis of . We clearly have
[TABLE]
Since , so we only need to bound . By exactly the same (easy) argument as in [GL, Lem. 5.2.6] (which uses [GL, Lem. 5.2.2]), we have
[TABLE]
Note in the current paper, the -dimension of (constructed in the first row of (3.1.3)) should be , and so
[TABLE]
And so we can choose any such that . So in our current paper, we can choose
[TABLE]
∎
4. Overconvergent basis and main theorem
In this section, we prove our main theorem; then we also make some comparison with known proofs.
4.1. Overconvergent basis
We first show the existence of an “overconvergent basis”, with respect to which all entries of the matrices for and are overconvergent elements. In the following, we will use notations like to mean a row vector .
4.1.1 Theorem**.**
Suppose is finite extension and . Let be a finite free -representation of of rank . Let be as in (3.2.9). Then there exists an -basis of such that,
- •
* with where .*
- •
* with where , for any .*
Proof.
The proof follows exactly the same ideas as in [GL, Thm. 6.1.1]. Indeed, the construction of the basis is verbatim as Step 1, Step 2 and Step 3 of loc. cit. (which we sketch below for the reader’s convenience). We only need to modify Step 4 of loc. cit. in our situation.
Step 1. Generators of . First of all, by induction on , we construct a specific set of generators of such that forms a -basis of .
We choose any -basis of . Suppose we have defined the generators for . By Lem. 3.1.6(2), we can use the map to identify with when . Now define
- •
for , and
- •
choose any in , so that is a -basis of .
This finishes the inductive definition.
Step 2. Basis of . With above, now we define basis for . By [GL, Lem. 5.1.2(2)] (note that this lemma is about module theory over ; there is no involved), for any , we can write
[TABLE]
with such that and . Let
[TABLE]
We can arrange that , and (because everything is -torsion here), and we can easily check (by Nakayama Lemma) that is an -basis of .
Step 3. Compatibility of basis. We can easily check that . So now we can define , which is a basis of .
Step 4. Matrices for and . Now, to prove our theorem, similarly as in Step 4 of [GL, Thm. 6.1.1] (which used [GL, Lem. 6.1.3]), we can apply our Lemma 4.1.2(2), and so it suffices to show that (for any ),
- •
with where .
- •
with where .
Since comes from a loose crystalline lift, we can write
- •
, with ,
- •
, with .
By [GL, Lem. 5.1.2] (note that this lemma is about module theory over ; there is no involved), for all , we can write
[TABLE]
So we can write
- •
, with ,
- •
, with .
Then we have
- •
,
- •
,
and we can easily conclude. Finally, the containment is via Lemma 4.1.3(1). ∎
4.1.2 Lemma**.**
Suppose .
- (1)
. 2. (2)
Suppose that such that in . If for all , then converges to a .
Proof.
Item (1) is easy. Item (2) is similar to [GL, Lem. 6.1.3], which is a special case of the current lemma (with ). ∎
4.1.3 Lemma**.**
Suppose , then we have
- (1)
. 2. (2)
. 3. (3)
**
Proof.
Write for some . Then for where , we have
[TABLE]
Since , we can deduce (1). For (2) and (3), simply consider the expansion of . ∎
4.2. Proof of Main theorem
First, we prove our main theorem when .
4.2.1 Proposition**.**
Suppose is a finite extension and . Let be a finite free -representation of of rank . Then is overconvergent on the interval
[TABLE]
Proof.
The proof is similar to that of [GL, Thm. 6.2.1].
Let be the basis of as in Theorem 4.1.1. Let be any basis of , and let where . Then we have . In order to prove the theorem, it suffices to show that for
[TABLE]
To prove the above assertion, by Lemma 4.1.2, it suffices to show that where . We prove this by induction on . The case is verbatim as in [GL, Thm. 6.2.1]. Suppose the claim is true when , and let us consider the case . Write with where is the set of Teichmüller lifts, so that we have . It suffices to show .
From , we have
[TABLE]
Multiply both sides of (4.2.3) with . Then we have
- •
by induction hypothesis.
- •
The term
[TABLE]
where
- –
by Lemma 4.1.3(3),
- –
by induction hypothesis,
- –
and by Theorem 4.1.1.
So the term .
- •
The term by Lemma 4.1.3(2), and we have .
So in the end, we get an equation of the form
[TABLE]
where . We must have , and so we can divide (4.2.4) by and apply [GL, Lem. 6.2.2] to conclude.
∎
We can deduce the full case from above:
4.2.2 Theorem**.**
Suppose is a finite extension. Let be a finite free -representation of of rank . Then is overconvergent on the interval
[TABLE]
Proof.
This is easy corollary of Theorem 4.2.1, via Lemma 2.4.3. The expression of the overconvergence interval (4.2.5) is because the -rank of the induction is . Indeed, (4.2.5) is an overconvergence interval for (as a -representation), hence also for (as a -representation). ∎
4.3. Comparison with known proofs
It is natural to wonder how to compare our proof with the classical proof of [CC98] (and also [BC08, Ked15]). However, there does not seem to be any obvious link between the two proofs. One particular characteristic of our proof is that the key technical analysis happen over the imperfect period rings (such that and ); whereas the classical proofs [CC98, BC08] (also implicitly in [Ked15]) rely on a Tate-Sen formalism (cf. [BC08, Def. 3.1.3]) for certain perfect period rings (cf., e.g., [BC08, Prop. 4.2.1]). The link between the two worlds remain mysterious.
As we already mentioned in the introduction, the explicit uniform bound on the overconvergence radius (4.2.5) is a new result. Actually, there are some results concerning the overconvergence radius in [BC08, §4.2] (we thank an anonymous referee for pointing out this reference). In the following, we show that using loc. cit., together with results from [GL] (on loose crystalline lifting) and [CL11] (on ramification bound), we can also prove a certain (implicit) “uniform overconvergence”.
In the following, let be a finite extension. Let be a finite free -representation of of rank . Suppose is a finite Galois extension such that acts trivially on (so a priori, depends on , or at least on ).
Let be the integer defined as in [BC08, Def. 3.1.3(TS3)], and let be the number defined in [BC08, Lem. 4.2.5]. It is easy to see that both and depend only on and . Now, let . Then by [BC08, Prop. 4.2.6], is overconvergent on the interval (note that the convention of in [BC08, §4.2] is different from ours in §2.4).
4.3.1 Lemma**.**
Suppose . Then there exists a finite Galois extension over which depends only on , such that acts on trivially.
4.3.2 Remark*.*
By above lemma, when , all the numbers , and depend only on (and not on ). So the ’s are overconvergent “uniformly” (depending on only). However, in this method, we do not know how to explicitly bound the overconvergence radius, because it seems difficult to explicitly bound and (even though we can bound quite explicitly, see the proof in the following).
Proof of Lemma 4.3.1.
It suffices to show the existence of such that acts on trivially. By [GL, Thm. 3.3.2, Rem. 3.3.5], there exists a loose crystalline lift of , with Hodge-Tate weights in the range . Now we can apply [CL11, Thm. 1.1] to conclude. Namely, in loc. cit., we simply let and . Clearly, the and , and thus in loc. cit. depend on only. We then simply let our to be the Galois closure of the fixed field of . ∎
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