On Mochizuki’s Idea of Anabelomorphy and its applications
Jean-Marc Fontaine
In Memoriam
1 Introduction
§ 1.1 What is Anabelomorphy?
The term anabelomorphy (pronounciation guide anabel-o-morphy; the root of this term is in Alexander Grothendieck’s Anabelian Program) is coined and introduced here as a concise way of expressing Shinichi Mochizuki’s notion of an anabelian way of changing base fields or base rings. Roughly speaking, one may understand anabelomorphy as the branch of arithmetic in which one studies arithmetic by fixing the absolute Galois group of a field rather than the field itself, and is firmly grounded in the well-known theorem of Mochizuki which asserts that a -adic field is determined by its absolute Galois group equipped with the upper numbering ramification filtration [Mochizuki, 1997].
The case of -adic fields is already quite non-trivial and hence this Introduction will focus on this case. Two -adic fields are anabelomorphic if and only if their absolute Galois groups are topologically isomorphic (see Definition 2.1.1). Anabelomorphy is a new equivalence relation on -adic fields. Isomorphic -adic fields are anabelomorphic, but there exist many non-isomorphic but anabelomorphic -adic fields (Lemma 4.4).
A quantity (resp. a property, an algebraic structure) associated with a -adic field is said to be amphoric if it depends only on the anabelomorphism class of i.e. if two -adic fields in the same anabelomorphism class have the same quantity (resp. same property, isomorphic algebraic structures). The amphora of is the collection of all quantities, properties, algebraic structures associated with which depend only on the anabelomorphism class of . For example if is a -adic local field, then the following are examples of an amphoric quantity, property, algebraic structures respectively: the residue characteristic of , the property of unramifiedness of , and the topological group (Theorem 2.4.3).
The existence of anabelomorphic -adic fields which are not isomorphic means that within the anabelomorphism class of , the additive structure of a -adic field deforms or wiggles around while the multiplicative structure of (i.e. the topological group ) remains fixed. This provides us with a new degree of freedom which can be exploited in number theory. For a picturesque way of thinking about anabelomorphy see § 1.8.
The theory of perfectoid fields and perfectoid varieties [Scholze, 2012] also provides highly non-trivial examples of anabelomorphy (see § 18). While this paper deals mostly with the group theoretic aspects of anabelomorphy, in [Joshi, 2019], I demonstrate that Mochizuki’s idea of keeping multiplicative structures of fields (and rings) fixed while allowing the ring structure to vary, can in fact be algebraized.
§ 1.2 Anbelomorphy, Galois representations and the local Langlands Correspondence
If two -adic fields are anabelomorphic, one can view representations of as representations of . Thus Anabelomorphy of -adic fields has immediate applications to the theory of representations of the absolute Galois group of a -adic field. Thanks to the main theorem of [Mochizuki, 1997], an important realization on which this paper is founded is that the upper numbering ramification inertia filtration of the absolute Galois group of a -adic field is a Galois theoretic stand-in for the additive structure of a -adic field and through this stand-in the additive structure (of the field) makes its presence felt in the theory of Galois representations.
This theme is explored here in many different ways in this paper starting with establishing the amphoricity of ordinary representations (Theorem 6.1). One knows, by [Mochizuki, 1997], that the property of a representation being Hodge-Tate is unamphoric, so amphoricity of ordinary representations (Theorem 6.1, Theorem 6.2) assumes arithmetic/geometric significance. Theorem 7.1 and Theorem 7.2 deal with properties of under anabelomorphy. In Theorem 8.1, I show that the -invariant (which given, for a Tate elliptic curve with Tate parameter , by ) is unamphoric. Another important observation is that the Fontaine subspace of ordinary crystalline two dimensional representations of is also amphoric (Theorem 14.1.4).
[Theorem 20.6, should be thought of as the Ordinary Synchronization Theorem at archimedean primes, I provide the archimedean analog of Mochizuki’s theory of étale theta functions [Mochizuki, 2009] (which deals with non-archimdean primes of semi-stable reduction). This approach is quite different from Mochizuki’s treatment of archimedean primes and I believe that my approach provides a certain aesthetic symmetry by bringing the theory at archimedean primes on par with the theory at semi-stable primes. ]
Now let me say a few words about the relationship between Anabelomorphy and the local Langlands Correspondence. The local Langlands Correspondence deals with representations of the absolute Galois group of a -adic field (or a local field of characteristic ). So the natural question which arises is this: If two -adic fields are anabelomorphic, then how are the corresponding automorphic representations related? The amphoricity of ordinary Galois representations (Theorems 6.1 and 6.2) suggested to me that there might be a portion of the Local Langlands Correspondence which is amphoric. This leads me to the following results. In Theorem 15.2.2, I show that for anabelomorphic -adic fields , one can also synchronize or match local automorphic principle series representations of and i.e. the principal series representations are amphoric (here are only assumed to be anabelomorphic and there may be not exist any (abstract) field isomorphism between them at all). If and , then one can also synchronize supercuspidal representations of and in a manner compatible with the Local Langlands Correspondence (§ 15, Theorem 15.2.2, Theorem 15.3.2). The situation for () needs substantial clarification.
Another important observation of this paper is that several arithmetic invariants of Galois representations such as the different and the discriminant Theorem 4.1, the Swan conductor Theorem 9.1, are unamphoric. This has not appeared in the existing literature on anabelian geometry.
§ 1.3 Anabelomorphy of varieties
The idea of anabelomorphy can be extended to higher dimensions from the zero dimensional case of fields, by means of fundamental groups of various types. The two principal ones discussed here and [Joshi, 2021, 2022, 2023b, 2023a, 2024b] are the tempered fundamental group of a rigid analytic space arising from a reasonable quasi-projective variety over a -adic field and the case of étale fundamental groups of varieties over number fields or -adic fields. Because of this, anabelomorphy also enjoys a close relationship with the absolute Grothendieck Conjecture and one obtains non-trivial geometric examples of anabelomorphy when the said conjecture fails. A non-trivial example of this is [Joshi, 2020]–which is important from the point of view of [Mochizuki, 2021a, b, c, d] and [Joshi, 2021, 2022, 2023b, 2023a, 2024b].
§ 1.4 Local anabelomorphy and Galois Theoretic Surgery on Number Fields
The validity of Grothendieck’s Anabelian Conjecture for number fields (Theorem 2.4.1) means that a number field is anabelomorphically rigid. So the question of globalizing local changes of arithmetic into global arithmetic a geometry is quite a subtle one. Local Anabelomorphy, may be thought of as Galois-theoretic surgery on number fields. This leads to the notion of anabelomorphically connected number fields (see 13.1.1, basic example is in Example 13.1.2). The notion of anabelomorphically connected number fields is an important stepping stone in incorporating local anabelomorphic changes into global geometry (Theorem 13.2.2, Theorem 13.2.4).
To begin the discuss, recall that in many results related to automorphic forms and Galois representations (for example [Taylor, 2002]), a theorem of [Moret-Bailly, 1989] plays a central role in incorporating local changes into global arithmetic. An important insight of this paper is that Moret-Bailly’s Theorem can be viewed as arising from a trivial case of Anabelomorphy.
This observation, together with Grothendieck’s Section Conjecture, suggests an anabelomorphic version of Moret-Bailly’s Theorem about density of global points in -adic topologies for anabelomorphically connected number fields. Simplest version of this anabelomorpphic version of Moret-Bailly’s Theorem is Theorem 16.1.1 (for ). Since Grothendieck’s Section Conjecture remains open, the general anabelomorphic version of Moret-Bailly’s Theorem for anabelomorphically connected number fields is largely conjectural Theorem 16.3.3 and Conjecture 16.3.5. The theorem of [Moret-Bailly, 1989] emerges as a very special case of these results. However, Corollary 16.3.4 shows that this general anabelomorphic version of Moret-Bailly’s Theorem is true unconditionally for projective and affine spaces.
As an arithmetic application of Theorem 16.1.1, I prove an Anbelomorphic Connectivity Theorem for Elliptic Curves (see Theorem 16.2.1) which shows that if is an elliptic curve such that has semi-stable reduction at and if is any anabelomorphically connected number field then there exists an elliptic curve with and with potentially good reduction at all other non-archimedean primes of .
§ 1.5 Weak or basal anabelomorphy
Since I have suggested that anabelomorphy should be roughly understood as providing an anabelian way of base-change, so it is interesting to study the behavior of (say) a variety over when viewed over two anabelomorphic extensions of . This leads to the notion of weak or basal anabelomorphy studied in § 17. In Theorem 17.2.1, I show that for an elliptic curve over a -adic field, all the four quantities: the exponent of the discriminant, the exponent of the conductor, the Kodaira Symbol and the Tamagawa Number are weakly unamphoric. In particular, the bad reduction type of an elliptic curve appears to be sensitive to the differences between the arithmetic of strictly anabelomorphic -adic fields. In Theorem 17.4.2, I show that the Artin and Swan conductors of a higher genus curve are also weakly unamphoric. In particular, the phenomena observed for elliptic curves also occur in higher genus situation. One way to think about these results is that many familiar and frequently used operations, such as choosing a minimal equation for an elliptic curve over two anabelomorphic fields, are strongly tied to the subtle differences between the intertwining of addition and multiplication in the two fields.
In § 19, I show that -adic differential equations (in the sense of [André, 2003]) on a geometrically connected, smooth, quasi-projective and anabelomorphic varieties can also be synchronized under anabelomorphy. This should be thought of as “gluing -adic differential equations by their monodromy.” In particular, the Riemann-Hilbert Correspondence of [André, 2003] can be synchronized with respect to this gluing.
§ 1.6 Perfectoid spaces and anabelomorphy
§ 1.7 Relationship to Mochizuki’s approach
[This subsection was written by Shinichi Mochizuki and explains how the idea of anabelomorphy discussed in this paper relates to the idea of “Indeterminacy Ind1” [Mochizuki, 2021c, Page 416] (also see [Mochizuki, 2020, Page 104]) which plays a central role in [Mochizuki, 2021a, b, c, d].]
In the parlance of [Mochizuki, 2021a, b, c, d], anabelomorphy, in the case of absolute Galois groups of p-adic local fields, is closely related to Mochizuki’s indeterminacy (Ind1), i.e., to the -indeterminacy, where denotes the absolute Galois group of a p-adic local field, which, in [Mochizuki, 2021a, b, c, d], occurs at all nonarchimedean primes. In particular, the following results of the present paper: Theorem 4.1 (and the table following it), Theorem 9.1, and Theorem 17.2.1; (and the data tables after Theorem 17.2.1) provide explicit numerical insight concerning how automorphisms of that do not arise from field automorphisms, i.e., concerning automorphisms of the sort that arise in the (Ind1) indeterminacy of [Mochizuki, 2021a, b, c, d], can act in a fashion that fails to preserve differents, discriminants, and the Swan and Artin conductors, as well as several other quantities associated to elliptic curves and Galois representations that depend, in an essential way, on the additive structure of the p-adic field.
§ 1.8 A picturesque way of thinking about Anabelomorphy
One could think of anabelomorphy in the following picturesque way:
One has two parallel universes (in the sense of physics) of geometry/arithmetic over -adic fields and respectively. If are anabelomorphic (i.e. ) then there is a worm-hole or a conduit through which one can funnel arithmetic/geometric information in the -universe to the -universe through the choice of an isomorphism of Galois groups , which serves as a wormhole. Information is transfered by means of amphoric quantities, properties and algebraic structures. The and universes themselves follow different laws (of algebra) as addition has different meaning in the two anabelomorphic fields (in general). As one might expect, some information appears unscathed on the other side, while some is altered by its passage through the wormhole. Readers will find ample evidence of such phenomena throughout this paper.
§ 1.9 Summary
It should be clear to the readers, after reading this paper, that assimilation of this idea (and the idea of anabelomorphic connectivity) into the theory of Galois representations should have interesting consequences for number theory. Here I have considered anabelomorphy for number fields but interpolating between the number field case and my observation that perfectoid algebraic geometry is a form of anabelomorphy, it seems reasonable to imagine that anabelomorphy of higher dimensional fields will have applications to higher dimensional algebraic geometry as well.
§ 1.10 Acknowledgments
I met Jean-Marc Fontaine in 1994–1995 at the Tata Institute (Mumbai) where he taught a course on -adic Hodge theory. I was fortunate enough to learn -adic Hodge theory directly from him. In the coming years, Fontaine arranged my stays in Paris (1996, 1997, and 2003) which provided me an opportunity to further my understanding of -adic Hodge Theory from him while he (and a few others) were engaged in creating it. Influence of Fontaine’s ideas on this paper and my work on Arithmetic Teichmuller Spaces detailed in [Joshi, 2021, 2023b, 2023a, 2024b, 2024a] should be obvious. I dedicate this paper to the memory of Jean-Marc Fontaine.
The reflections recorded herein began during my stay at RIMS (Kyoto, Spring 2018). Support and hospitality from RIMS (Kyoto) is gratefully acknowledged. I thank Shinichi Mochizuki for many conversations and correspondence on his results documented in [Mochizuki, 2021a, b, c, d]. After the first version of this paper was posted online in March 2020, some readers strongly asserted that there is no relationship between this paper and [Mochizuki, 2021a, b, c, d], so I invited Mochizuki to explain the relationship between anabelomorphy and his ‘Indeterminacy Ind1’ and he obliged by contributing § 1.7.
I thank Yuichiro Hoshi for answering many questions on anabelian geometry. I also thank Yu Yang for promptly answering my questions about [Mochizuki, 2006]. Thanks are also due to Machiel van Frankenhuijsen for many conversations on the -conjecture and Mochizuki’s Anabelian Reconstruction Theory [Mochizuki, 2012, 2013, 2015]. I thank Taylor Dupuy for conversations around many topics treated here and for providing versions of his manuscripts [Dupuy and Hilado, 2020a], [Dupuy and Hilado, 2020b]. Taylor carefully read several early versions of this manuscript and provided number of suggestions and improvements for which I am extremely grateful. I also thank Tim Holzschuh for a careful reading of an early version of this manuscript and pointing out many typos. I thank Shinichi Mochizuki and Peter Scholze, for alerting me to some errors in the first version (March 2020) of this manuscript.
2 Anabelomorphy, Amphoras and Amphoric quantities
Let be a fixed prime number. Occasionally I will write for an arbitrary prime number not equal to . By a -adic field I mean a finite extension of . Let be a field and let be a geometrically connected, smooth quasi-projective variety over (the case is perfectly reasonable for understanding the definitions given below. By and large I will assume that is either a -adic field or a number field but the ideas presented here can be used in wider context.
For a field , let be a separable closure of (note the conflation of standard notation and ), be its absolute Galois group considered as a topological group, (resp. ) the inertia (resp. wild inertia) subgroup of .
§ 2.1 Definitions
Definition 2.1.1.
Let be two -adic fields or number fields.
-
(1)
I will say that are anabelomorphic or anabelomorphs (or anabelomorphs of each other) if their absolute Galois groups are topologically isomorphic . I will write if are anabelomorphic and will mean a specific isomorphism of topological groups.
-
(2)
Obviously if and then . So anabelomorphism is an equivalence relation on -adic fields.
-
(3)
The collection of all fields which are anabelomorphic to will be called the anabelomorphism class of .
-
(4)
I will say that is strictly anabelomorphic to or that is a strict anabelomorphism if but is not isomorphic to .
Remark 2.1.2.
By the observations of § 18, one can also extend the above definition to include perfectoid fields.
Definition 2.1.3.
Let be two -adic fields or number fields. A quantity or an algebraic structure or a property of is said to be an amphoric quantity (resp. amphoric algebraic structure, amphoric property) if this quantity (resp. alg. structure or property) depends only on the anabelomorphism class of . More precisely, if is an anabelomorphism of fields then , and also has property .
In § 2.4, the reader will find examples of illustrating the non-triviality of these definitions.
Definition 2.1.4.
Let be a field. I will say that is anabelomorphically rigid if whenever one has an anabelomorphism (with of the same sort as ), one has an isomorphism of fields .
§ 2.2 Anabelomorphy of quasi-projective varieties
The definition of anabelomorphy of fields readily extends to smooth varieties of higher dimensions. If is a geometrically connected, smooth quasi-projective variety over then write (resp. ) for its étale (resp. tempered) fundamental group of . If then both these groups coincide with .
Anabelomorphism (resp. tempered anabelomorphism) also defines an equivalence relation on smooth varieties over -adic fields.
Evidently isomorphic varieties over a -adic field are anabelomorphic (over that field).
Definition 2.2.1.
-
(1)
Let be two fields. I will say that are anabelomorphic or anabelomorphs (or anabelomorphs of each other) if and only if their absolute Galois groups are topologically isomorphic
-
(2)
More generally, if and are two geometrically connected, smooth, quasi-projective varieties, then I will say that is anabelomorphic to if one has a topological isomorphism of the étale fundamental groups
Especially, if and then and are anabelomorphic if and only if the fields and are anabelomorphic. If are -adic fields one may similarly define the term ‘tempered anabelomorphic.’
-
(3)
I will write if are anabelomorphic and the notation
will mean that we are given a specific isomorphism
of topological groups. For the case and , I will write if and are anabelomorphic.
-
(4)
I will say that is strictly anabelomorphic to or that is a strict anabelomorphism if but is not isomorphic to .
-
(5)
Obviously if and then . So anabelomorphy is an equivalence relation. The collection of all smooth, geometrically connected quasi-projective varieties which are anabelomorphic to will be called the anabelomorphism class of .
The following is fundamental in understanding anabelomorphy of varieties:
Proposition 2.2.2.
Suppose are finite fields, -adic fields or number fields. Let are geometrically connected, smooth, quasi-projective varieties and if
is an anabelomorphism between them, then one has an anabelomorphism
Proof.
This is [Mochizuki, 2012, Corollary 2.8(ii)].
Definition 2.2.3.
Let be a geometrically connected, smooth, quasi-projective variety over a field . I will say that is anabelomorphically rigid if any anabelomorphism (with of the same sort as ), one has an isomorphism of -schemes .
Remark 2.2.4.
Here I use term ‘same sort’ in the following sense: if is a -adic field then is of this type, if is a number field then so is ; if is a hyperbolic curve then is also a hyperbolic curve etc. It is, of course, possible that there may exist varieties of entirely distinct sorts which are all anabelomorphic to .
Definition 2.2.5.
Let be a geometrically connected, smooth, quasi-projective variety over a -adic field . A quantity or an algebraic structure or a property of associated to is said to be an amphoric quantity (resp. amphoric algebraic structure, amphoric property) if this quantity (resp. alg. structure or property) depends only on the anabelomorphism class of i.e. it depends only on the isomorphism class of the topological group . More precisely: if is an isomorphism of topological groups then takes the quantity (resp. algebraic structure , property ) for to the corresponding quantity (resp. alg. structure, property) of . If a quantity (resp. alg. structure, property) of which is not amphoric, then it will simply be said to be unamphoric or not amphoric quantity, algebraic structure or property.
For examples of amphoric quantities which have been know prior to this paper see section 2.4.
Definition 2.2.6.
The collection of all amphoric quantites, algebraic structures or properties of is called the amphora of the topological group .
Remark 2.2.7.
Let me caution the reader that elements of an amphoric algebraic structure need not be amphoric, more precisely, an isomorphism of an algebraic structures induced by an anabelomorphism may not be the identity isomorphism of this algebraic structure.
§ 2.3 Anabelomorphy and Galois representations
Since I am thinking of applications of anabelomorphy to Galois representations, it would be useful to allow some additional generality. Consider an auxiliary topological field which will serve as a coefficient field for representations of (for example for any prime including and will be more than adequate for my discussion). Let be a finite dimensional -vector space (as a topological vector space). Let be a continuous representation of . I will say that a quantity or an algebraic structure or a property of the triple is amphoric if it is determined by the anabelomorphism class of .
§ 2.4 Five fundamental theorems of Anabelomorphy
For the reader’s convenience I provide here five fundamental theorems of anabelian geometry upon which anabelomorphy rests. I have organized the results in a logical manner (as opposed to a chronological order).
Theorem 2.4.1 (First Fundamental Theorem of Anabelomorphy).
Number fields are anabelomorphically rigid i.e. if are number fields then is anabelomorphic to if and only if is isomorphic to i.e.
Proof.
The first fundamental theorem is a classical result due to Neukirch and Uchida. Modern proof of this result can be found in [Hoshi, 2015].
Theorem 2.4.2 (Second Fundamental Theorem of Anabelomorphy).
If are -adic fields then if and only if there is a topological isomorphism of their Galois groups equipped with the respective (upper numbering) inertia filtration i.e.
Proof.
This is the main theorem of [Mochizuki, 1997].
The following theorem is a combination of many different results proved by (Neukirch, Uchida, Jarden-Ritter, Mochizuki) in different time periods.
Theorem 2.4.3 (Third Fundamental Theorem of Anabelomorphy).
Let be a -adic field. Then
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(1)
The residue characteristic of is amphoric.
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(2)
The degree and the absolute ramification index are amphoric.
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(3)
The topological groups and (viewed as a topological -module) are amphoric.
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(4)
The inertia subgroup and the wild inertia subgroup are amphoric.
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(5)
The -adic cyclotomic character is amphoric.
Proof.
Remark 2.4.4.
Hoshi’s paper also provides a longer list of amphoric quantities, properties and alg. structures.
The next assertion is the Jarden-Ritter Theorem [Jarden and Ritter, 1979]. This provides a way of deciding if two fields are anabelomorphic or not in most important cases.
Theorem 2.4.5 (Fourth Fundamental Theorem of Anabelomorphy).
Let be -adic fields with and both contained in . Write (resp. ) be the maximal abelian subfield contained in . Then the following are equivalent:
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(1)
-
(2)
and .
Proof.
For a proof see [Jarden and Ritter, 1979].
Theorem 2.4.6 (Fifth Fundamental Theorem of Anabelomorphy).
Let be a -adic field and let (resp. ) be the inertia subgroup (resp. the wild inertia subgroup). Then and are topological characteristic subgroups of (i.e. invariant under all topological automorphisms of ).
These are five fundamental theorems of classical Anabelomorphy. To this list I would like to add the following elementary but useful result.
Theorem 2.4.7.
Let be a prime, let be an algebraic closure of and let be a positive integer. Let
Then is a finite union of disjoint anabelomorphism classes.
Proof.
Anabelomorphism is an equivalence relation on and hence partitions into a disjoint union of anabelomorphism classes and it is well-known that is a finite set. Hence there are finitely many anabelomorphism classes in .
3 Monoradicality is Amphoric
Let be a -adic field. An extension is a monoradical extension if it is of the form for some and in this case is a generator of . The following is proved in [Jarden and Ritter, 1979].
Theorem 3.1.
Monoradicality is amphoric and hence in particular, the degree of any monoradical extension is amphoric.
4 Discriminant and Different of a -adic field are unamphoric
For definition of the different and the discriminant of a -adic field see [Serre, 1979, Chap III]. [Serre, 1979] The following result is fundamental for many diophantine applications.
Theorem 4.1.
The different and the discriminant of a finite Galois extension are unamphoric.
Proof.
By Theorem [Serre, 1979, Chap III, Prop 6] it is sufficient to prove that the different of is unamphoric. By Theorem [Serre, 1979, Chap IV, Prop 4] the different depends on the ramification filtration for . So in general, there exist anabelomorphs with distinct differents and discriminants. Here is an explicit family of examples.
Let be an integer, an odd prime and let so and let . By Lemma 4.4 below one has an anabelomorphism and hence one has . But and are not isomorphic fields so by [Mochizuki, 1997] they have distinct inertia filtrations. I claim that they have distinct differents and discriminants. More precisely, one has the following formulae for the discriminants of (resp. ) [Viviani, 2004, Theorem 5.15 and 6.13].
(4.2) | |||||
(4.3) |
In particular, for these are equal to and respectively and evidently for any odd prime . This proves the assertion.
Lemma 4.4.
Let be any integer and any odd prime. Let and let and let . Then one has
Proof.
Both fields contain and by elementary Galois theory and Kummer theory one checks that and is the maximal abelian subfield of both and both have the same degree over . The Jarden-Ritter Theorem [Jarden and Ritter, 1979] says in this situation that the absolute Galois groups of are isomorphic i.e. . Hence the claim.
Let me set up some notation for my next result. For a -adic field write for the different of . This is an ideal of . Valuation on is normalized so that for any uniformizer of . In contrast to the fact that different and discriminants are unamphoric, one has the following elementary but useful bound given by [Mochizuki, 2021d, Prop. 1.3] (though this not stated in this form in loc. cit.).
Theorem 4.5 (Different Bound).
Let be a -adic field. Then there exists an absolute constant determined by the anabelomorphism class of such that for all one has
Proof.
Let . Let , be the residue field degree for and be the absolute ramification index. Then it is well-known, (see [Artin, 2006]) that one has
So it suffices to remark that are amphoric quantities and hence depend only on the anabelomorphism class of equivalently on the anabelomorphism class of . So now take
Hence the assertion.
[-7, 121] |
5 Unramifiedness and tame ramifiedness of a local Galois representation are amphoric
Let be a -adic field. In this section I consider continuous representations with values in some finite dimensional vector space over some coefficient field which will be a finite extension of one of the following fields: or a finite field . All representations will be assumed to be continuous (with the discrete topology on if is a finite field) without further mention.
Let be a representation of . Let be an anabelomorphism. Then as , so any -representation gives rise to a -representation by composing with and conversely, any -representation gives rise to a representation by composing with . One sees immediately that this isomorphism induces an equivalence between categories of finite dimensional continuous representations. In particular, the category of -representations is amphoric.
Now suppose is a -stable subspace. Let be an anabelomorphism. Then is also a stable subspace of . This is clear as for all . In particular, if is a reducible representation of then so is the associated -representation. Conversely, any reducible -representation provides a reducible representation. This discussion is summarized in the following elementary but useful result:
Proposition 5.1.
Let be a -adic field and let be a coefficient field.
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(1)
The category of finite dimensional -representations of is amphoric.
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(2)
Irreducibility of a -representation is an amphoric property.
Proof.
This is clear from the definitions.
Recall that a Galois representation is said to be an unramified representation (resp. tamely ramified) if (resp. .
Recall that is unramified (resp. tamely ramified) if the image (resp. ).
Theorem 5.2.
Let be a -adic local field. Unramifiedness (resp. tame ramifiedness) of are amphoric properties.
Proof.
This is clear from the definition of unramifiedness (resp. tame ramifiedness) and the fact that (resp. ) are amphoric (see [Hoshi, 2021, Proposition 3.6]).
6 Ordinarity of a local Galois representation is amphoric
Let me note that Mochizuki (in [Mochizuki, 2021a, b, c, d]) considered ordinary representations arising from Tate elliptic curves. In [Hoshi, 2018] Hoshi considered proper, hyperbolic curves with good ordinary reduction and the standard representation associated with the first étale cohomology of this curve. My observation (recorded here) which includes both the -adic and the -adic cases is that the general case is not any more difficult (I claim no originality or priority in the general case) and of fundamental importance in many applications.
Let be a continuous -representation of with a finite extension of (and ). Then is said to be an ordinary representation of if the image of the inertia subgroup of is unipotent. In [Fontaine, 1994b] this is called a semi-stable -adic representation of .
Theorem 6.1.
Assume . Then ordinarity of an -adic representation is an amphoric property.
Proof.
Let be a continuous Galois representation on on a finite dimensional vector space with a finite extension. Let be a -adic field with an isomorphism . By Theorem 2.4.6 [Mochizuki, 1997] or [Hoshi, 2021, Proposition 3.6] the inertia (resp. wild inertia) subgroups are amphoric. Then so the image of is also unipotent.
Now before I discuss the -adic case, let me recall that it was shown in [Mochizuki, 1997] that for any -adic field , the -adic cyclotomic character of is amphoric. Let be a -adic cyclotomic character. Recall from [Perrin-Riou, 1994] that a -adic representation with a finite dimensional -vector space is said to be an ordinary -adic representation of if there exist -stable filtration on consisting of -subspaces of such that the action of on is given by (as -representations).
Theorem 6.2.
Now assume . Then ordinarity of a -adic representation is an amphoric property.
Proof.
It is immediate from the Prop. 5.1 that the filtration is also -stable. By Theorem 2.4.5, (and hence its powers) are amphoric. By definition, for any and any ,
Now given an isomorphism , one has for all
and by Mochizuki’s Theorem 2.4.3, is the cyclotomic character of . Thus this condition is determined solely by the isomorphism class of .
Two dimensional ordinary (reducible) -adic representations play an important role in [Mochizuki, 2021a, b, c, d] (not merely because some arise from Tate elliptic curves) and I will return to this topic in Section 14 and especially Theorem 14.1.1.
Theorem 6.2 should be contrasted with the following result which combines fundamental results of Mochizuki and Hoshi [Mochizuki, 2012, Hoshi, 2013, 2018]:
Theorem 6.3.
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(1)
Let be an anabelomorphism of -adic fields. Then the following conditions are equivalent
-
(a)
For every Hodge-Tate representation , the composite is a Hodge-Tate representation of .
-
(b)
.
-
(a)
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(2)
There exists a prime and a -adic local field and an automorphism and a crystalline representation such that is not crystalline. In other words, in general crystalline-ness is an unamphoric property of .
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(3)
In particular, being crystalline, semi-stable or de Rham is not an amphoric property of a general -adic representation.
7 is unamphoric
Let me begin with a somewhat elementary, but surprising result which is still true (despite of the above unamphoricity results of Mochizuki and Hoshi on Hodge-Tate representations). This result is surprising because of Mochizuki’s Theorem (see [Mochizuki, 1997]) which says that the -adic completion is unamphoric. For -admissible representations see [Fontaine, 1994a].
Theorem 7.1.
Let be a -adic field and let be an anabelomorphism. Let be a -adic representation.
-
(1)
Then is -admissible if and only if is -admissible.
-
(2)
In particular, is pure of Hodge-Tate weight as a -module if and only if is pure of Hodge-Tate weight as a -module.
Proof.
A well-known theorem of Shankar Sen [Sen, 1980] or [Fontaine, 1994a, Proposition 3.2], is -admissible if and only if the image of inertia is finite. By the Third Fundamental Theorem of Anabelomorphy (Theorem 2.4.3) if is finite then so is . So the assertion follows.
Twisting by , one can assume that is Hodge-Tate of weight zero as a -representation. Then by Shankar Sen’s Theorem referred to earlier, image of under is finite. Hence the image of under is finite. This proves the assertion.
Now let me prove the following elementary reformulation of Mochizuki’s Theorem [Mochizuki, 2012, Theorem 3.5(ii)] which asserts that the property of being Hodge-Tate representation is unamphoric. My point is that my formulation (given below) shows more precisely why this happens. Let me set up some notation. Let be a -adic field and let be the kernel of the cyclotomic character . Let be the fixed field of . Let be an anabelomorphism. Let be the kernel of the cyclotomic character (note the conflation of notation made possible by the amphoricity of the cyclotomic character). Let be the fixed field of . By the amphoricity of the cyclotomic character one has an isomorphism and hence also of the quotients . Hence one observes that one has an anabelomorphism . Consider a -adic representation of . By a fundamental theorem of [Sen, 1980, Theorem 4], there exists an endomorphism of the -vector space . Another theorem of loc. cit (see [Sen, 1980, Corollary of Theorem 6]) asserts that -representation is Hodge-Tate if and only if is semi-simple and eigenvalues of are integers. Let me note that by [Sen, 1980, Theorem 5] one can always find a basis of such is given by a matrix with coefficients in . Let be the endomorphism of the -vector space (considering as a -representation through ).
Theorem 7.2.
Let be a -adic field. Let be a -adic representation of . Then is unamphoric. If is an anabelomorphism then is Hodge-Tate if and only if is semi-simple and has integer eigenvalues.
One way to understand this result is to say that is an invariant of which depends on the additive structure of .
8 The -invariant is unamphoric
Let be a -adic field and let be a two dimensional ordinary ( = reducible, semi-stable) representation of with coefficients in such that one has an exact sequence
Then one has an invariant, defined by [Greenberg, 1994], Fontaine, and others (see [Colmez, 2010] for all the definitions and their equivalence), called the -invariant of , denoted , which plays a central role in the theory of -adic -function of and related representations of . One of the simplest, but important, consequences of anabelomorphy is the following:
Theorem 8.1.
Let be a -adic field. Let be as above. Then the -invariant, , of is unamphoric.
For a more detailed discussion of for ordinary representations see Theorem 14.2.1.
Proof.
The representation is an extension whose class lives in
and this -vector space (of dimension ) is also described naturally by means of Kummer theory, I will write for this extension class. By [Nekovář, 1993], [Colmez, 2010], [Perrin-Riou, 1994] the space is described by two natural coordinates where is the -adic logarithm (with ). From [Nekovář, 1993], [Colmez, 2010] one see that
The assertion follows from the fact the for a unit is an unamphoric quantity (in general) as the additive structure of the field which comes into play here through the use of the -adic logarithm is not an amphoric quantity: two anabelomorphic fields may not be isomorphic as fields.
Theorem 8.2.
Let . Then the Hodge filtration on is unamphoric.
9 Artin and Swan Conductor of a local Galois representation are Unamphoric
For consequences of this in the context of elliptic curves and curves in general see Section 17. For Artin and Swan conductors see [Serre, 1979], [Katz, 1988, Chapter 1]. Coefficient field of our representations will be a finite extension with . The Artin conductor (resp. the Swan conductor) of an unramified (resp. tamely ramified) representation are zero. So one must assume that the wild inertia subgroup acts non-trivially for these conductors to be non-zero. The theorem is the following:
Theorem 9.1.
Let be a local Galois representation with such that the image of is non-trivial. Then the Artin and the Swan conductors of are unamphoric.
Proof.
It is enough to prove that the Swan conductor is unamphoric. This is clear as the Swan conductor is given in terms of the inertia filtration. Since is not an isomorphism of filtered groups (by [Mochizuki, 1997]) so the Artin and the Swan conductors of the representation is not the same as that of the -representation in general. To see the explicit dependence of the Artin (resp. Swan) conductors on the inertia filtration see [Serre, 1979], [Katz, 1988, Chap 1]. To illustrate my remark it is enough to give an example. Let and . Then . By the character table for this finite group (see [Viviani, 2004, Theorem 3.7]), there is a unique irreducible character of dimension . Let for denote the exponent of the Artin conductor of . Then by [Viviani, 2004, Cor. 5.14 and 6.12] one has
(9.2) | |||||
(9.3) |
Evidently .
The following two results are fundamental for many applications of anabelomorphy.
Theorem 9.4.
Let be an -adic representation of . Then there exists a unique, smallest integer such that in the anabelomorphism class of , there exists an such that the Swan conductor of the -representation is .
Proof.
Corollary 9.5 (Anabelomorphic Level Lowering).
In the anabelomorphism class of a -adic field , there exists an anabelomorphism such that for any -adic or an -representation , the -representation has the smallest Artin conductor.
10 Peu and Tres ramifiedness are unamphoric properties
In many theorems in the theory of Galois representations and modular forms, the notion of peu and tres ramifiée extensions plays an important role. For more on the notion of peu and tres ramifiée extensions readers should consult [Serre, 1987, Section 2.4], [Edixhoven, 1992]. Let me briefly recall the definitions. Let be a -adic field and be the maximal tamely ramified (resp. maximal unramified) subextension of such that with for all . Then is peu ramifiée if for all , otherwise is tres ramifiée.
Recall from [Edixhoven, 1992, Prop 8.2] that is peu ramifiée (i.e. the fixed field of its kernel is peu ramifiée) if and only arises from a finite flat group scheme over (the ring of integers of ).
Theorem 10.1.
The property of being peu ramifiée (resp. being tres ramifiée) extension (resp. representation) is unamphoric.
Proof.
Combining this with [Edixhoven, 1992, Prop 8.2] one gets:
Corollary 10.2.
Finite flatness of a -representation (into with a finite dimensional -vector space) is not an amphoric property.
Reader should contrast the above corollary with Theorem 12.3.1.
11 Frobenius elements are Amphoric
One has the following result of Uchida from [Jarden and Ritter, 1979, Lemma 3]:
Theorem 11.1.
Let be an anabelomorphism of -adic fields. If is a Frobenius element for . Then for any topological isomorphism , is a Frobenius element for .
This has the following important corollary.
Theorem 11.2.
Let be a -adic field and let be a finite dimensional continuous representation of in an -vector space with a finite extension and . Then the characteristic polynomial of Frobenius (= is amphoric. In particular, -functions of local Galois representations are amphoric.
Proof.
This is clear from the previous result.
12 Constructions of varieties via anabelomorphy
§ 12.1 Anabelomorphy and Affine spaces and Projective Spaces
For a -adic field , let be its ring of integers, and let be the topological group of all the non-zero elements of , let be the (topological) group of units.
Theorem 12.1.1.
Let be an anabelomorphism of -adic fields. Let be an integer. Then the anabelomorphism induces a homeomorphism
of topological spaces.
Proof.
By Theorem 2.4.3, one has an isomorphism of topological groups and . Now by means of the -adic logarithm, , for (resp. for ), one has an isomorphism of topological groups
and a similar isomorphism for . Using this isomorphism one deduces that one has a homeomorphism
This proves the assertion.
The following is now an immediate corollary:
Corollary 12.1.2.
Let be the multiplicative group (considered as an algebraic variety over a field of choice). Let be integers. Let (resp. ) considered as algebraic variety over (resp. ). Let be an anabelomorphism of -adic fields. Then one has an homeomorphism of topological spaces
Proof.
The proof is clear using Theorem 12.1.1.
Theorem 12.1.3.
Let be an anabelomorphism of -adic fields. Let be an integer. Then induces a homeomorphism of topological spaces:
Proof.
Let me prove this explicitly for . Let be an anabelomorphism. The topological space is described by two coordinate charts and one has a homeomorphism
and
and
The topological space is obtained by gluing using the homeomorphism
Now suppose . Thus the homeomorphism is constructed using this local description and the homeomorphisms
and
given above.
Now consider the general case of . The topological space is covered by opens subsets for and the intersections and are of the form considered in Corollary 12.1.2 for suitable choices of integers . Thus the assertion is now clear by the standard principles of gluing topological spaces and homeomorphisms between them.
The following corollary is an immediate consequence of the proof of Theorem 12.1.3.
Remark 12.1.4.
Let me remark that if are anabelomorphic -adic fields, then one has a trivial isomorphism of algebraic fundamental groups
So one can consider and as trivially anabelomorphic varieties.
§ 12.2 Anabelomorphy and Abelian varieties with multiplicative reduction
Let me begin with the simpler example of a Tate curve over a -adic field . By a Tate elliptic curve I will mean an elliptic curve with split multiplicative reduction over a -adic field . By Tate’s theorem [Silverman, 1994] a Tate elliptic curve over corresponds to the data of a discrete cyclic subgroup . The equation of the Tate curve is then given by
with explicitly given convergent power series in .
The main theorem is the following:
Theorem 12.2.1.
Let be a -adic field and let be a Tate elliptic curve over with Tate parameter . Let be a -adic field anabelomorphic to with an isomorphism . Then there exists a Tate elliptic curve with Tate parameter and an isomorphism of topological abelian groups
given by the isomorphism . The elliptic curve is given by Tate’s equation
Proof.
The anabelomorphism provides an isomorphism which provides, by the third fundamental theorem of anabelomorphy 2.4.3, an isomorphism of topological groups . Let . The map preserves the valuation of and hence and so by Tate’s Theorem one gets the Tate elliptic curve . The composite provides the isomorphism of topological groups . This proves the assertion.
This argument extends readily to Abelian varieties with multiplicative reduction via the uniformization theorem of [Mumford, 1972].
Theorem 12.2.2.
Let be a -adic field and let be an abelian variety of dimension given by a lattice in a -dimensional torus given by . Let be an anabelomorphism of -adic fields. Then there exists an abelian variety and a topological isomorphism of groups . If is polarized then so is .
Proof.
The lattice provides a lattice in using the isomorphism induced by induced by our anabelomorphism . The rest is immediate from the Mumford-Tate uniformization theorem. If is polarized, then constructing a polarization on is left as an exercise.
The following corollary is immediate:
Corollary 12.2.3.
In the notation of the above theorem, one has an isomorphism of groups:
in other words, and are anabelomorphic abelian varieties.
Proof.
Let . An étale cover of is an abelian variety with multiplicative reduction over some finite extension . The covering map provides an injective homomorphism of discrete subgroups corresponding to the étale covering . Since , any finite extension of gives a finite extension , this correspondence is given as follows corresponds to an open subgroup and the isomorphism provides an open subgroup which is an isomorphic image of under this isomorphism and is the fixed field of . Hence one has, in particular, that . Now construct an étale cover of over by transferring the data of the covering (which is an inclusion of discrete subgroups of finite index) to . By Mumford’s construction this gives a covering . The correspondence provides the required correspondence between étale coverings of and étale coverings of . This argument can be reversed. Starting with a covering of one can arrive at a covering of . Hence the result follows.
§ 12.3 Anabelomorphy of group-schemes of type over -adic fields
Let be a -adic field and be a commutative, finite flat group scheme of order and type over . Let be an anabelomorph of . Then the following shows that there is a commutative finite flat group scheme of type over which is obtained from . By [Raynaud, 1974] the group scheme is given by a system of equations
Fix an anabelomorphism . This induces isomorphism of topological groups . Let , for all be the inverse image of under this isomorphism. Then
provides a finite flat group scheme of type . Conversely, starting with a group scheme of this type over , one can use an anabelomorphism between to construct a group scheme over . Thus one has
Theorem 12.3.1.
An anabelomorphism of fields sets up a bijection between commutative finite group flat schemes of type over and respectively. This bijection does not preserve finite flat group schemes on either side.
13 Anabelomorphic Connectivity Theorem for Number Fields
The notion of anabelomorphy suggests the possibility of anabelomorphically modifying a number field at a finite number of places to create another number field which is anabelomorphically glued to the original one at a finite number of places and anabelomorphic connectivity theorems for such fields provide a way of passing geometric information between two anabelomorphically connected fields. This is the main theme of this section.
§ 13.1 Definition and examples
Definition 13.1.1.
I say that two number fields are anabelomorphically connected along and , if there exist non-archimedean places of (resp. non-archimedean places of ) and for each an anabelomorphism and for each the inclusion is dense. I will simply denote this by writing
Example 13.1.2.
Here is a basic collection of examples. Let be an odd prime, let be an integer. Let , . These are totally ramified at (see [Viviani, 2004]). Let (resp. ) be the unique prime of prime lying over in (resp. the unique prime of lying over in ). The completions of (resp. ) with respect to these unique primes are and respectively. By Lemma 4.4 one has an isomorphism of the local Galois groups
For each , the pairs and provide a basic example of an anabelomorphically connected pair of number fields (see 13.1.1). In particular, the number fields (and the unique primes be the primes lying over in ) are anabelomorphically connected along and :
Remark 13.1.3.
By the formulae for the discriminants of (see Lemma 4.4), one sees that the differents (and hence the discriminants) of anabelomorphically connected fields differ in general. This is a fundamental way in which local anabelomorphic modifications change global arithemtic data.
§ 13.2 Existence of anabelomorphically connected fields
The next step is to establish the existence of anabelomorphically connected fields. This is accomplished in Theorem 13.2.2 and the more general Theorem 13.2.4 which provide a systematic way of producing examples of anabelomorphically connected fields starting with a given number field.
In what follows, I will say that a number field is dense in a -adic field if there exists a place of such that the completion of at is (i.e. ).
I begin with the following easy lemma.
Lemma 13.2.1.
Let be -adic field. Then there exists a number field which is dense in .
Proof.
This is a well-known consequence of Krasner’s Lemma (see [Koblitz, 1984]). Let where is the residue characteristic of . Let be the minimal polynomial of . If then is algebraic and clearly is the dense number field one seeks. If this is not the case then choose sufficiently close to in . Then by Krasner’s Lemma (see loc. cit.) is irreducible and if is a root of then and hence is dense in .
Theorem 13.2.2 is a prototype of the more general result proved later (Theorem 13.2.4) and is included here for the convenience of the readers as it illustrates the main points of the general result.
Theorem 13.2.2 (Anabelomorphic Connectivity Theorem).
Let be a number field and let be a non-archimedean place of . Let be a local field anabelomorphic to . Then there exists a number field and non-archimedean place of such that
In particular, is anabelomorphic to . Equivalently .
Proof.
By Lemma 13.2.1, there exists a number field dense in . Let be the place corresponding to the dense embedding (i.e. ). Then and hence and hence . Thus the assertion follows.
Now let us move to the general case of connectivity along several primes simultaneously. From the point of view of applications of Mochizuki’s ideas this case is fundamental.
I will use the following (non-standard) terminology: a non-archimedean local field is a finite extension of for some (unspecified) prime . I say that an arbitrary, finite set of non-archimedean local fields (not all distinct and not all necessarily of the same residue characteristic) is a cohesive set of non-archimedean local fields if there exists a number field and for every , a dense inclusion such that the induced valuations on are all inequivalent.
Lemma 13.2.3 (Potential Cohesivity Lemma).
For every finite set of non-archimedean local fields (not all distinct and not necessarily of the same residue characteristic) there exist finite extensions such that is a cohesive system of non-archimedean local fields.
Proof.
By Lemma 13.2.1 the result is true for with . The general case will be proved by induction on . Suppose that the result has been established for the case of fields. So for every set of non-archimedean fields there exists finite extensions of non-archimedean fields and a number field which is dense inclusion for and the valuations induced on are all inequivalent. Choose such that .
Now suppose that is the residue characteristic of and . By Lemma 13.2.1 there exists a number field dense in . By Krasner’s Lemma one can choose to be algebraic and sufficiently close to such that . Now consider the finite extensions and (if is not a field then pick a direct factor of as this is a product of fields each of which is a finite extension of equipped with an embedding of , and similarly for ) for . Then for and . Write (for symmetry of notation). Then one sees that there exists a common number field contained in all of . If is not dense in each of one can extend further to achieve density. Similarly if the induced valuations on are not all inequivalent, one can extend further to achieve this as well.
Let me explain how the last two steps are carried out. To avoid notational chaos, I will prove the assertion for . So the situation is that one has two non-archimedean fields and a common number field contained in both of them. There are two possibilities: either residue characteristics of are equal or they are not equal. First assume that the residue characteristics are equal (say equal to ). Then are both finite extensions of and so there exists a finite extension containing both of them as subfields. Pick such an . Then there is a number field dense in . Now choose a number field , with , which is totally split at and such that are linearly disjoint over . Then let and since is completely split there exist two primes of lying over such that and . Thus the system is now cohesive as and are dense inclusions corresponding to distinct primes of .
Now assume have distinct residue characteristics and is a number field contained in both of them. If (resp. ) is the prime of corresponding to the inclusion (resp. ), then and are finite extensions of non-archimedean fields. One proceeds by descending induction on . By the primitive element theorem there exists an (resp. ) such that (resp. ). Choose an irreducible polynomial which is sufficiently close to the minimal polynomials of (resp. ) in and respectively. Then has a root in both (by Krasner’s Lemma). The field embeds in both and if (resp. ) is the prime lying over (resp. ) corresponding to the inclusion and are dense inclusions of in (resp. in ) and and similarly for . Thus by enlarging in this fashion one is eventually led to a cohesive system as claimed.
Now I can state and prove the general anabelomorphic connectivity theorem for number fields.
Theorem 13.2.4 (Anabelomorphic Connectivity Theorem II).
Let be a number field. Let be a finite set of non-archimedean places of . Let be arbitrary anabelomorphisms with non-archimedean local fields . Then there exist
-
(1)
finite extensions (for all i) and a dense embedding of a number field and places of induced by the embeddings (i.e. the collection of non-archimedean fields is cohesive) and
-
(2)
a finite extension and places of lying over the places of (for all ) together with anabelomorphisms .
-
(3)
Equivalently and for all .
In particular, given any number field and a collection of non-archimedean places of , there exists a finite extension and a number field which is anabelomorphically connected to along some place of lying over each of places of .
Proof.
By the Cohesivity Lemma (Lemma 13.2.3) one can replace by a cohesive collection with finite extensions and a number field dense in each such that the induced valuations on are all inequivalent. The finite extensions provide open subgroups of . Since one has anabelomorphisms , let be the inverse image of in . By continuity of , are open subgroups of . Let be the open subgroup of generated by the decomposition groups of all primes except and the open subgroups for . Let be the fixed field of (in our fixed algebraic closure of ). Let be the unique place of lying over the such that . Then by construction
and hence one has established that
Now let me prove some Theorems which will be useful in applying these results to arithmetic problems (such as those envisaged in [Mochizuki, 2021a, b, c, d]). I will begin with some preparatory lemmas which are well-known but difficult to find in the form I will need here.
Lemma 13.2.5.
Let be a -adic field. Then there exist infinitely many number fields with a dense embedding .
Proof.
This is easy to prove and is left as an exercise!
Theorem 13.2.6.
Let be a number field and let be a non-archimedean place of . Then there exist infinitely many anabelomorphically connected number fields . If is a strict anabelomorphism then are strictly anabelomorphically connected fields.
Proof.
By Lemma 13.2.5 there exist infinitely many number fields with a dense embedding .
Let be a number field which is dense in and let be the prime of corresponding to the embedding . Then one has anabelomorphically connected fields .
Theorem 13.2.7.
Let be a number field and let be a prime of lying over . Then there exist infinitely many anabelomorphically connected fields such that . If is strictly anabelomorphic to then is a strict anabelomorphic connectivity.
Proof.
Let us suppose that there is a anabelomorphically connected number field (with ) with maximal among all such fields. Let be the prime lying below (and hence also ) in . Choose a quadratic field which is completely split at and which is also totally split at any prime ramifying in . Then has no primes of ramification and hence by the Hermite-Minkowski Theorem, . Let . Then by construction is totally split at . Let be a prime of lying over of . Then and so one has anabelomorphisms and hence and which contradicts the maximality of .
14 The Ordinary Synchronization Theorem
A fundamental result discovered by Mochizuki (see [Mochizuki, 2012, 2013, 2015]) is the Synchronization of Geometric Cyclotomes. This plays a fundamental role in [Mochizuki, 2021a, b, c, d]. For a catalog of synchronizations in [Mochizuki, 2021a, b, c, d] see [Dupuy and Hilado, 2020b].
§ 14.1
The elementary result given below is inspired by Mochizuki’s result and is quite fundamental (despite the simplicity of its proof) in applications of anabelomorphy to Galois representations. This result asserts that two anabelomorphically connected number fields see the “same” ordinary two dimensional local Galois representations at primes on either side which are related through anabelomorphy. The theorem is the following:
Theorem 14.1.1 (The Ordinary Synchronization Theorem).
Let
be a pair of anabelomorphically connected number fields. Then one has for all primes (including ) and for all , an isomorphism of -vector spaces
This theorem is immediate from the following Lemma.
Lemma 14.1.2.
Let be two anabelomorphic -adic fields. Then one has an isomorphism of -vector spaces
Proof.
Let be an anabelomorphism. It is standard that one has
(continuous cohomology group). By Kummer Theory one knows that can be described as and one has a similar description for . Then one has isomorphisms of topological groups and hence also of subgroups compatible with their respective inclusions in (resp. ). Hence one has isomorphism of groups
This also compatible with projections to similar groups for . Thus one has an isomorphism of the inverse limits and hence in particular, on tensoring with .
Alternately one can simply invoke the fact that is an amphoric module. The two cohomologies depends only on the topology of . So the claim is obvious.
This proof leads to the following (which is useful in many applications)
Lemma 14.1.3 (Bootstrapping Lemma).
Let be an amphoric -module (i.e. an abelian topological group or a topological -module with a continuous action of which is determined by the anabelomorphism class of ). Then is amphoric.
Proof.
The proof is clear: continuous -cohomology is determined by the topology of and by the topological isomorphism class of . As is amphoric the result follows.
The following theorem is key in [Mochizuki, 2021a, b, c, d], but I think that this formulation illustrates an important point which is not stressed in loc. cit. where it occurs in the guise of the amphoricity of log-shell tensored with (for the log-shell see [Hoshi, 2021], [Dupuy and Hilado, 2020b]). Let be a -adic field. Let
be the (Fontaine) subspace of (ordinary) crystalline two dimensional -representations in .
Theorem 14.1.4.
Let be a pair of anabelomorphic -adic fields. Then one has an isomorphism of -vector spaces
In other words the space , of crystalline-ordinary two dimensional -representations of the form , of is amphoric!
Remark 14.1.5.
For readers of [Mochizuki, 2012, 2013, 2015] and [Mochizuki, 2021a, b, c, d] let me remark that is the log-shell tensored with (for a discussion of log-shells, see [Hoshi, 2019], [Dupuy and Hilado, 2020a], [Dupuy and Hilado, 2020b], [Mochizuki, 2015]). This is because one has an isomorphism of finite dimensional -vector spaces
where is the subgroup of -units of .
§ 14.2 Anabelomorphy and -adic Hodge Theory
Let me provide an important example of Anabelomorphy which has played a crucial role in the theory of Galois representations. The Colmez-Fontaine Theorem which was conjectured by Jean-Marc Fontaine which asserts that “every weakly admissible filtered module is an admissible filtered module” and proved by Fontaine and Colmez in [Colmez and Fontaine, 2000]. The proof proceeds by changing the Hodge filtration on a filtered -module.
This should be viewed as an example of anabelomorphy but carried out on the -adic Hodge structure.
The idea of [Colmez and Fontaine, 2000] is to replace the original Hodge filtration (which may make the module possibly inadmissible) by a new Hodge filtration so that the new module becomes admissible i.e. arises from a Galois representation. So in this situation the -adic Hodge filtration is considered mobile while other structures remain fixed. This allows one to keep the -adic field fixed.
Let me remark that by Theorem 8.1 one knows that the -invariant of an elliptic curve over a -adic field is unamphoric together with the fact that -invariant is related to the filtration of the -module (see [Mazur, 1994]). So the filtration is moving in some sense but the space on which the filtration is defined is also moving because the Hodge filtration for the -module lives in the -vector space , while the Hodge filtration for the -module lives in an -vector space.
As Mochizuki noted in his e-mail to me “it remains a significant challenge to find containers where the -vector space and -vector space can be compared.” My observation recorded below resolves this question raised by Mochizuki by showing that there is a natural way to compare these spaces under at least under a reasonable assumption.
Let be a -adic field and let be an anabelomorphism of -adic fields. Consider of . Suppose that is a de Rham representation of in the sense of [Fontaine, 1994a]. As was proved in [Hoshi, 2013] need not be de Rham. Suppose is ordinary. Then by [Perrin-Riou, 1994], is then semi-stable and hence also de Rham. By Theorem 6.2 one deduces that the -representation is also ordinary and hence also de Rham. Let me write for the -vector space associated to the de Rham representation of and write for the -vector space associated to the de Rham representation of .
Theorem 14.2.1.
Let be a -adic field, let be an anabelomorphism of -adic fields. Let be a de Rham representation of such that is also de Rham (this is the case for example if is ordinary). Then for all sufficiently large integers , there is a natural isomorphism of -vector spaces
Remark 14.2.2.
Note that the Hodge filtration on the -vector space is up to shifting, the filtration on the -vector space . However I do not know how to compare the Hodge filtrations on and .
Proof.
Let act on through the isomorphism . So is also a -module. Then as , one has an isomorphism of -vector spaces (given by ):
By a fundamental observation of [Bloch and Kato, 1990] there is a natural mapping, called the Bloch-Kato exponential,
which is an isomorphism for all sufficiently large . There is a similar isomorphism for since is also a de Rham representation of through . Now putting all this together the isomorphism in the theorem is obvious.
Corollary 14.2.3.
Let be a -adic field. Let be a -adic representation of . Let be an ordinary Galois representation of . Then for all sufficiently large , is an amphoric -vector space.
15 Automorphic Synchronization Theorems: Anabelomorphy and the local Langlands correspondence
This section is independent of the rest of the paper. I will assume that readers are familiar with the basic theory of automorphic representations at least for though the main result proved here is for . The representations in this section will be smooth, complex valued representations of . There is an automorphic analog of the Ordinary Synchronization Theorem (Theorem 14.1.1) which says that one can use an anabelomorphism to synchronize automorphic representations of and . Note that topological groups and are not topologically homeomorphic (except for ). I prove the automorphic synchronization theorem for principal series for for any and also for all irreducible admissible representations of for any odd prime .
§ 15.1 Anabelomorphisms and Weil-Deligne Groups
The following two lemmas will be used in the subsequent discussion.
Lemma 15.1.1.
Let be a -adic field. Let be the cardinality of the residue field of . Then
-
(1)
The homomorphism given by is amphoric.
-
(2)
the homomorphism defined by is amphoric.
Proof.
Lemma 15.1.2.
Let be a -adic field and let be an anabelomorphism. Let (resp. ) be the Weil group of (resp. ) and let (resp. ) be the Weil-Deligne group of (resp. ). Then one has topological isomorphisms
-
(1)
, and
-
(2)
which maps Frobenius element of to (and resp. for Weil-Deligne groups).
Proof.
The anabelomorphism gives an isomorphism . The cardinality of the residue field of is amphoric (see [Hoshi, 2021]). Let be the residue field of (and hence of ). Let be a Frobenius element for and let be the Frobenius element of corresponding to the Frobenius element of . Then is the fiber-product of the two arrows
Since it is now clear that and this preserves Frobenius elements (by Theorem 11.1). The assertion for Weil-Deligne groups is immediate from this and by the existence of given by the previous lemma and the definition of the Weil-Deligne group.
§ 15.2 Anabelomorphic Synchronization of Principal Representations
Assume that are -adic fields and is an anabelomorphism. Let me first show how to setup a bijective correspondence between principal series representations of and .
Let me begin with the case. In this case and is is an anabelomorphism then provides an isomorphism . Hence any character provides a character , and conversely, every character of determines a unique character of . Thus one obtains a bijection between admissible representations and admissible representations which is given by . The local Langlands correspondence sets up a bijection between admissible representations of and one dimensional representations of the Weil-Deligne group with . Hence one obtains a correspondence between representations of the Weil group and the Weil group of the appropriate sort.
Since the local Langlands Correspondence match -functions on either side and on the Galois side and as I have already established (Theorem 11.2) that local -functions on the Galois side are amphoric, so it follows that automorphic -functions are amphoric. Since conductors of characters are unamphoric (see Theorem 9.1), it follows that under anabelomorphy conductors are unamphoric. Moreover -factors require a choice of additive character and hence neither the conductor nor the -factors are amphoric (as both are dependent on the inertia filtration via its control of the additive structure–for example). Hence one has proved that
Theorem 15.2.1.
Let be a -adic field and let be an anabelomorphism of -adic fields. Then sets up a bijection between admissible representations of and admissible representations of . This correspondence is compatible with the local Langlands correspondence on either side. -functions of irreducible admissible representations are amphoric. The conductor and -factors are unamphoric.
Now let me discuss the for . The datum required to give a principal series representations of consists of an -tuple of continuous characters of with values in . The associated principal series representation is denoted by and every principal series representation is of this type.
The following theorem should be considered as the local automorphic analog of the ordinary synchronization theorem (Theorem 14.1.1). The first main theorem of the section is the following.
Theorem 15.2.2 (Automorphic Ordinary Synchronization Theorem).
Let be an anabelomorphism of -adic fields. Then there is a natural bijection between principal series representations of and principal series representations of which is given by
This correspondence takes irreducible principal series representations to irreducible principal series representations.
Proof.
The correspondence sets up a bijection between -tuples of continuous characters of and . Every principal series representation of is of the form (similarly for ) so the assertion is immediate.
Now to prove that an irreducible principal series representation is mapped to an irreducible principal series representation one it is sufficient to note that if then so is . So under this correspondence an irreducible representation is mapped to an irreducible representation.
§ 15.3 Anabelomorphic Synchronization of Supercuspidal representations for odd,
Now suppose and (i.e. is an odd prime). Then one knows that every supercuspidal representation of arise, up to twisting by one dimensional characters, by base change where is a quadratic extension, is a character such that if is the unique non-trivial element then .
Now suppose . Then there exists a unique quadratic field such that and is the open subgroup of index two corresponding to and is the corresponding open subgroup under . A character provides a character by composing with and if is the unique non-trivial element then evidently . Hence one obtains a supercuspidal representation where . Thus, under anabelomorphy , one has setup a correspondence
This procedure is symmetrical in and so this establishes a bijection between supercuspidal representations under both the sides.
Finally note that from my discussion of the principal series correspondence one sees that Steinberg representation of corresponding to the irreducible sub (resp. quotient) of (resp. ) is mapped to the corresponding object of .
Moreover, up to twisting by one dimensional characters, every irreducible admissible representation is one of the three types: irreducible principal series representation, a Steinberg representation or a supercuspidal representation. Further, any twist of an irreducible admissible representation of is mapped to the corresponding twist of the appropriate irreducible admissible representation. Hence the following is established:
Theorem 15.3.1 (Automorphic Synchronization Theorem).
Let be an odd prime and let be an anabelomorphism of -adic fields. Then this anabelomorphism induces a bijection between irreducible admissible representations of and . This correspondence takes (twists of) irreducible principal series to irreducible principal series, Steinberg to Steinberg and supercuspidal to supercuspidal representations.
The local Langlands correspondence is a bijection between complex, semi-simple representations of Weil-Deligne group and irreducible, admissible representations of . The correspondence maps an irreducible principal series ( are considered as characters of the Weil-Deligne group via the Artin map). The Steinberg representation maps to the special representation of the Weil-Deligne group. A supercuspidal representation is mapped to the irreducible Weil-Deligne representation which is obtained by induction of from to .
Now given an anabelomorphism and a Weil-Deligne representation , one can associate to it the Weil-Deligne representation . This evidently takes semi-simple representations to semi-simple representations and by construction, it is compatible with the local Langlands correspondence on both the sides.
Note that Artin conductors of representations on both the sides of the local Langlands correspondence are dependent on the ramification filtration and hence conductors are unamphoric (Theorem 9.1). The epsilon factors depend on additive structures (for example the data of an epsilon factor requires an additive character) and so epsilon factors are manifestly unamphoric. Thus one has proved:
Theorem 15.3.2 (Compatibility of the local Langlands Correspondence).
Let be an odd prime and let be anabelomorphic -adic fields. Then the local Langlands correspondence for is compatible with the automorphic synchronization provided by Theorem 15.3.1. -functions are amphoric but the conductors of Weil-Deligne representations and irreducible, admissible representations are unamphoric. Moreover epsilon factors are unamphoric.
Remark 15.3.3.
I expect that the above results are also true for , but their proofs will be a little more involved as there are many more representations to deal with.
Remark 15.3.4.
Let be a -adic field and let be an anabelomorphism of -adic fields. Then by [Hoshi, 2021] the Brauer group is amphoric and hence given a division algebra over , there exists a division algebra which corresponds to . It seems reasonable to expect that, at least for the case where (and hence ) is a quaternion division algebra, there exists synchronization of admissible representations of and which is compatible with the above constructions.
16 Anabelomorphic Density Theorems
Let me now illustrate fundamental arithmetic consequences of the anabelomorphic connectivity theorems (Theorems 13.2.2, 13.2.4).
§ 16.1 Anabelomorphic version of Moret-Bailly’s Theorem I
Let me begin with the following elementary but important result which should be considered to be the anabelomorphic analog of Moret-Baily’s Theorem [Moret-Bailly, 1989]. At the moment I do not know how to prove the full version of this theorem without assuming Grothendieck’s section conjecture, but already the version I prove below is enough to provide applications to elliptic curves. Let
then for any field , (see Theorem 16.3.3 for a general result). If we have an anabelomorphism then one has an isomorphism of topological groups and hence an isomorphism topological spaces (with the respective -adic topologies)
Theorem 16.1.1 (Anabelomorphic Density Theorem).
Let . Let be a number field. Let be an anabelomorphically connected number field. Then the inclusion
is dense for the -adic topology on the right and hence also Zariski dense.
Proof.
The proof is clear from the definition and the fact that the weak Approximation Theorem [Platonov and Rapinchuk, 1994, Chap 7, Prop. 7.1] holds for and hence also for its Zariski open subsets.
§ 16.2 Anabelomorphic Connectivity Theorem for Elliptic Curves
To understand arithmetic consequences of the above theorem, fix an identification of schemes
Then for any field , and composite mapping
allows to view the open subset as -invariants of elliptic curves over except for . If we have an anabelomorphism then one has an isomorphism of topological spaces (with the respective -adic topologies)
Theorem 16.2.1 (Anabelomorphically Connectivity Theorem for Elliptic Curves).
Let
be an anabelomorphically connected pair of number fields. Let be an elliptic curve over a number field with . Then there exists an elliptic curve such that
-
(1)
For all one has .
-
(2)
The -invariant of is integral at all non-archimedean places of except .
-
(3)
In particular, if has semi-stable reduction at then has semistable reduction at and one has for the Tate parameters of at (resp. at ).
-
(4)
has potential good reduction at all non-archimedean primes of except at .
Proof.
Let be the -invariant of . At any place of semi-stable reduction one has . Let be the given anabelomorphisms. Let . Then by the Theorem 16.1.1 one sees that
is dense. Hence there exists a which is sufficiently close to each of the and is -integral for all other non-archimedean valuations of .
By the well-known theorem of Tate [Silverman, 1985] there exists an elliptic curve with -invariant . By construction is sufficiently close to for each and as has semi-stable reduction at each the valuation of at each is negative. Moreover for other non-archimedean valuations of , is -integral by construction and so has potential good reduction at such .
As is sufficiently close to and the anabelomorphism preserves valuations on both the sides, the other assertions follow from the relationship between -invariants and Tate parameters at primes of semi-stable reduction.
A particularly useful consequence of this is the following:
Corollary 16.2.2.
Let be an elliptic curve with at least one prime of potentially semi-stable non-smooth reduction. Then there exists a pair of anabelomorphically connected number fields such that
-
(1)
is a finite extension
-
(2)
and has semi-stable reduction,
-
(3)
is the set of primes of semi-stable reduction of .
§ 16.3 Anabelomorphic version of Moret-Bailly’s Theorem II
Now let me prove a more general anabelomorphic density theorem. This section is a bit technical and skipped in the initial reading and is certainly independent of the rest of the paper. In this section by the phrase “assume Grothendieck’s section conjecture holds for ” I will mean that , and that there is some characterization of the image of this set with some reasonable functoriality in , and which depends only on the anabelomorphism class of . I will simply write to means the subset of sections which are characterized as arising from . This is not the standard terminology or notation.
Let me emphasize that the evidence for such an expectation at the moment is sparse. By a theorem of Mochizuki, one knows that if is an hyperbolic curve, then injects into the set of sections of (one may view Theorem 12.2.2 and Theorem 12.1.3 as some evidence of this as well).
Let me extend the notion of anabelomorphically connected number fields slightly. I will write
and say that are anabelomorphically connected along non-archimedean places of and non-archimedean places of if
Clearly this extends the notion introduced previously by allowing several primes of lying over a place of .
Let me begin with the following lemma which explains the role of Grothendieck’s section conjecture in the context of Moret-Bailly’s Theorem [Moret-Bailly, 1989].
Lemma 16.3.1.
Let us suppose that and are two geometrically connected, smooth, quasi-projective anabelomorphic varieties over -adic fields (i.e. is an isomorphism of topological groups and in particular, one has an anabelomorphism ). Assume that Grothendieck’s Section Conjecture holds for and . Then one has a natural bijection of sets
and in particular, if then .
Remark 16.3.2.
Note that in the context of the usual Moret-Bailly Theorem, the -adic fields are isomorphic so one may take and the section conjecture hypothesis in Lemma 16.3.1 is unnecessary in [Moret-Bailly, 1989]. My point is that anabelomorphy really underlies the sort of phenomena which lie at heart of [Moret-Bailly, 1989].
Proof of Lemma 16.3.1.
Let me remark that if and are two varieties over anabelomorphic fields such that
then Grothendieck’s section conjecture, which asserts that
is a bijection of sets, implies that there is a natural bijection of sets
and now the last assertion is obvious.
Theorem 16.3.3.
Let be a number field and let be a finite set of non-archimedean places of . Let be anabelomorphically connected number field. Let (resp. ) be a geometrically connected, smooth, quasi-projective variety over (resp. ). Suppose the following conditions are met:
-
(1)
and are anabelomorphic varieties for , and
-
(2)
for all , and
-
(3)
Grothendieck’s section conjecture holds for each and , and
-
(4)
suppose that one is given a non-empty open subset (in the -adic topology) .
Then there exists a finite extension and places of
-
(1)
such that one has the anabelomorphic connectivity chain
-
(2)
and, for all corresponding primes in the above connectivity chain, bijections
-
(3)
and a point whose image in (for all ) is contained in .
Corollary 16.3.4.
Let be anabelomorphically connected number fields as in Theorem 16.3.3. Then the assertion of Theorem 16.3.3 holds unconditionally i.e. without assuming Grothendieck’s Section Conjecture for the following two cases:
-
(1)
and , or
-
(2)
and .
Proof of Corollary 16.3.4.
This is immediate from the fact that by Theorem 12.1.3 (for the case and ) and by Theorem 12.1.1 (for and ), the hypothesis of the validity of the Section Conjecture in Theorem 16.3.3 can be circumvented.
Proof of Theorem 16.3.3.
The proof will use Lemma 16.3.1. By the hypothesis that are anabelomorphic, one has by Lemma 16.3.1, that for each , there is a natural bijection of sets
and hence the latter sets are non-empty because of our hypothesis.
Now the usual Moret-Bailly Theorem [Moret-Bailly, 1989] can be applied to with so there exists a finite extension which is totally split at all the primes into primes with and hence for each one has isomorphisms (for all ) and hence for each one has (for all ) and hence one has the stated anabelomorphic connectivity. The remaining conclusions are consequences of the usual Moret-Bailly Theorem.
Note that Grothendieck’s Section Conjecture is difficult. The following conjecture is adequate for most arithmetic applications.
Conjecture 16.3.5.
Let be a -adic field and let be a geometrically connected, smooth, quasi-projective variety over . Let be two anabelomorphic -adic fields containing . Let (resp. ). Then
-
(1)
There exists a finite extension and and an anabelomorphism such that there is a natural bijection of sets .
-
(2)
There is a Zariski dense open subset such that the induced mapping is a homeomorphism of topological spaces with respective topologies on either side.
17 Weak or Basal Anabelomorphy
§ 17.1 Definitions
As noted in § 1, one may think of anabelomorphy as an anabelian method of base change. In this section I want to elaborate on this base change aspect. To this effect let be a -adic field. Let be a geometrically connected, smooth, quasi-projective variety over . For any field extension , write for the base change of to . Consider the set
of all possible base change of to finite extensions . I define an equivalence relation on the set as follows.
Definition 17.1.1.
Let , then I will say that are weakly anabelomorphic or basally anabelomorphic if and only if .
The following is fundamental in understanding this:
Proposition 17.1.2.
Let be a geometrically connected, smooth, quasi-projective variety. Let .
-
(1)
Basal anabelomorphy is an equivalence relation on .
-
(2)
If and are anabelomorphic then they are also basally anabelomorphic.
Proof.
The first assertion is immediate from the properties of anabelomorphic of -adic fields. The second assertion follows from Proposition 2.2.2.
Remark 17.1.3.
The converse of Proposition 17.1.2(2) is not expected to hold in general.
Definition 17.1.4.
Let be a geometrically connected, smooth, quasi-projective variety over a -adic field . Let . Then a quantity or an algebraic structure or a property associated to is said to be an weakly or basally amphoric quantity (resp. weakly or basally amphoric algebraic structure, weakly or basally amphoric property) if this quantity (resp. alg. structure or property) depends only on the weak or basal anabelomorphism class of in . More precisely: if, for a pair , then one has (resp. algebraic structure , and the property holds for if and only if holds for . If a quantity (resp. alg. structure, property) of which is not weakly or basally amphoric, then it will simply be said to be weakly or basally unamphoric quantity, (resp. algebraic structure or property).
§ 17.2 Weak anabelomorphy and elliptic curves
The purpose of this subsection is to prove the following:
Theorem 17.2.1.
Let be an elliptic curve over a -adic field . Let be basally anabelomorphic. Then
-
(1)
has potential good reduction if and only if has potential good reduction.
-
(2)
has multiplicative reduction if and only if has multiplicative reduction.
-
(3)
In general, the following quantities are weakly unamphoric.
-
(a)
The valuation of the discriminant of ,
-
(b)
the exponent of conductor of .
-
(c)
The Kodaira Symbol of , and
-
(d)
the Tamagawa number of .
-
(a)
-
(4)
In particular, the number of irreducible components of the special fiber of is weakly unamphoric.
-
(5)
In particular, among all with , there is one for which is minimal.
Remark 17.2.2.
Let me say that in the semi-stable reduction case, numerical evidence suggests that the four quantities: valuation of the discriminant, the exponent of conductor of , the Kodaira Symbol of , and the Tamagawa number of are all weakly amphoric. But I do not know how to prove this at the moment.
Remark 17.2.3.
The first two assertions of Theorem 17.2.1 are similar to [Mochizuki, 2012, Theorem 2.14(ii)].
Corollary 17.2.4.
Let be an elliptic curve over a -adic field . Let be a finite extension of . Let be the minimal discriminant of . If has semi-stable reduction then let be its Tate parameter. Then
-
(1)
is a finite set.
-
(2)
If and both have semi-stable reduction then is a finite set.
In particular, under the above respective hypotheses, are bounded in the anabelomorphism class of .
Proof of Theorem 17.2.1.
Let be the -invariant of . Then so write for this quantity. The important point in the proof is the determination of the order of in and under weak anabelomorphy. This is given by [Jarden and Ritter, 1979, Lemma 2] or [Hoshi, 2021, Proposition 2.2]. By [Silverman, 1985, Chap VII, Prop 5.5] has potential good reduction if and only if . If then -invariant is integral in both and (because it is already so in ). So assume . Then if and only if and if and only if . This proves the first assertion.
Using [Silverman, 1985, Chap VII, Prop. 5.1] one sees that has multiplicative reduction if and only if and as if and only if one similarly gets (2).
So it remains to prove the other assertions. To prove these assertions it suffices to give examples. Let me remark that these examples also show that the hypothesis of stable reduction in [Mochizuki, 2012, Theorem 2.14(ii)] cannot be relaxed. The last assertion is immediate from the penultimate one as the Kodaira Symbol of also encodes the number of irreducible components of the special fiber.
Let , let and . Then as it can be easily checked using [Viviani, 2004]. Both of these field have degree
Let and and be as above. Let be the minimal discriminant (over the relevant field), be the exponent of the conductor, the list of Kodaira Symbols and the definition of the Tamagawa number are in [Silverman, 1994]. The following table shows the values for and .
Curve | Kodaira Symbol | Tamagawa Number | ||
2 |
Here is another example let and let be as above. Then one has
Curve | Kodaira Symbol | Tamagawa Number | ||
---|---|---|---|---|
10 |
§ 17.3 Additional numerical examples
Here are two more random examples where all the four quantities are simultaneously different..
Let
and let
Curve | Kodaira Symbol | Tamagawa Number | ||
---|---|---|---|---|
For the same fields as in the previous example and for the curve
Curve | Kodaira Symbol | Tamagawa Number | ||
---|---|---|---|---|
Now let me provide two examples for . Again these are examples (taken from my data) where all the four quantities are simultaneously different. Let , , (these fields are considered in [Jarden and Ritter, 1979]). By loc. cit. and are anabelomorphic of degree and totally ramified extensions of .
Then
Curve | Kodaira Symbol | Tamagawa Number | ||
---|---|---|---|---|
Then
Curve | Kodaira Symbol | Tamagawa Number | ||
---|---|---|---|---|
For additional examples see Table 17.3. These examples reveal that Tate’s algorithm [Silverman, 1994, Chapter IV, 9.4] for determining the special fiber of an elliptic curve over a -adic field is dependent on the additive structure of the field–especially steps 6 and beyond are strongly dependent on the additive structure of the field.
The tables, Table 17.3 and Table 17.5 on next two pages are fragments from my data which were generated by randomized searches. One notes from Table 17.3 that the hypothesis of potential good reduction in Theorem 17.2.1 cannot be relaxed. Numerical data of Table 17.5 suggests that if has semistable reduction, then the four quantities considered above are weakly amphoric.
These computations were carried out using SageMath [Stein et al., 2017].
§ 17.4 Weak anabelomorphy of Artin Conductors, Swan Conductors and Discriminants of curves
These results provide a complement to the results of the earlier section on Swan Conductors. More generally, let be a -adic field and let be a geometrically connected, smooth quasi-projective variety over . Let be anabelomorphic -adic fields containing . Write and .
Lemma 17.4.1.
Let be an anabelomorphism of -adic fields. Let (resp. ) be the maximal unramified extension of (resp. ). Then
Proof.
Since the inertia subgroup is amphoric by Theorem 2.4.2 and by the fact that is the fixed field of , the result is obvious.
For geometric applications it is convenient to work with a strictly Henselian ring. As Artin and Swan conductors are unaffected by passage to unramified extensions, this passage to strictly Henselian rings is harmless. In particular, one can work over . By the above lemma, and hence one can affect the passage to a strictly Henselian ring without affecting anabelomorphic data.
If is a geometrically connected, smooth, proper variety and (resp. ) is the geometric generic fiber (resp. special fiber) of a regular, proper model then one has a discriminant defined as in [Saito, 1988]. This coincides with the usual discriminant if is an elliptic curve. The main theorem of loc. cit. asserts that if is a curve then by loc. cit. one has
Let
be the Swan conductor of .
Theorem 17.4.2.
Let be a -adic field and let be a geometrically connected, smooth proper variety over . Let be a prime.
-
(1)
is weakly unamphoric.
-
(2)
Suppose is one dimensional i.e. a curve. Then is weakly unamphoric.
-
(3)
In particular, if is an elliptic curve then is weakly unamphoric.
Proof.
Let be anabelomorphic -adic fields containing . Write and . In Theorem 9.1, I have shown that Artin and Swan conductors of Galois representations are unamphoric. The last two assertions are the main theorems of [Saito, 1988]. The Artin and the Swan conductors are explicitly dependent on the ramification filtration.
So the weak anamphoricity of the quantities is clear from Saito’s formula and the above examples. But let me prove a more refined claim here which provides a better way of understanding this behavior by means of Saito’s formula.
Let be a -representation in a finite dimension -vector space (with a prime) such that the image of the wild inertia subgroup is finite.
I claim, in fact, that the breaks in the break-decomposition of (see [Katz, 1988, Lemma 1.5]) are unamphoric. If is a strict anabelomorphism then the and have distinct ramification filtrations and the proof of the break-decomposition shows that the break-decomposition is dependent on the ramification filtration. Hence the break-decomposition itself is unamphoric in general. Hence the Swan conductor which is a measure of the breaks in the break-decomposition is unamphoric.
The above proof also provided the unamphoricity of the break-decomposition which is recorded below:
Theorem 17.4.3.
Let be a -adic field and let be a continuous representation of in a -vector space such that the wild inertia subgroup operates through a finite quotient. Then the break-decomposition of is unamphoric. In particular, the breaks in the break-decomposition are unamphoric.
Remark 17.4.4.
I expect that using the algorithm for finding minimal models for genus two curves one can hope to find genus two examples of the above phenomenon similar to the examples for elliptic curves provided earlier.
18 Perfectoid algebraic geometry as an example of anabelomorphy
Now let me record the following observation which I made in the course of writing [Joshi, 2019] regarding the relationship between perfectoid algebraic geometry of [Scholze, 2012] and the idea of anabelomorphy as described in this paper.
§ 18.1 Anabelomorphy of perfectoid fields
Let be a complete perfectoid field of characteristic zero (see [Scholze, 2012, Section 3]). Let be its tilt (see [Scholze, 2012, Lemma 3.3]). The following basic examples will be useful in understanding this section.
Example 18.1.1.
Consider -adic completions respectively of
and
Then are both perfectoid fields. Let be the tilts [Scholze, 2012] of respectively with an isometry
The following is a formulation of [Scholze, 2012, Theorem 3.7] from the point of view of anabelomorphy:
Theorem 18.1.2.
Let be perfectoid fields with an isometry between their respective tilts. Then one has anabelomorphisms of perfectoid fields
These anabelomorphisms are in fact compatible with the inertia filtrations on the absolute Galois groups of all the perfectoid fields involved and hence the filtered group does not identify the perfectoid field uniquely.
Proof.
Let (resp. ) be the absolute Galois group of (resp. ). Then by [Scholze, 2012, Theorem 3.7] one has an isomorphism
and also the similar isomorphism for
Since , one has an isomorphism . Putting these together one obtains
This proves the assertion.
Remark 18.1.3.
The two fields described in Example 18.1.1 have isometric tilts and hence are anabelomorphic perfectoid fields.
§ 18.2 Anabelomorphy of perfectoid spaces
Now let me explain that the main theorem of [Scholze, 2012] provides the perfectoid analog of anabelomorphy (in all dimensions).
Suppose that is a perfectoid field. Let be a perfectoid space over [Scholze, 2012, Definition 6.15], which I will assume to be reasonable, to avoid inane pathologies. Let be its tilt (see [Scholze, 2012, Definition 6.16]). Let be its étale fundamental group for a suitable choice of geometric base point. This allows one to talk about anabelomorphisms of perfectoid spaces. Then one has the following:
Theorem 18.2.1.
Let be perfectoid fields with isometric tilts. Let be a perfectoid space and suppose that is another perfectoid space with isomorphism of the tilts
Then one has anabelomorphisms of perfectoid spaces
Proof.
This is a consequence of the stronger assertion [Scholze, 2012, Theorem 7.12] which implies that the categories of finite étale covers of and are equivalent.
Other examples of this phenomenon arise in the theory of Diamonds [Scholze, 2017]:
Theorem 18.2.2.
Let be anabelomorphic -adic fields (i.e. ), there exist geometric spaces, more precisely there exist diamonds, and such that
Remark 18.2.3.
The formation of (resp. ) requires (resp. ). By [Mochizuki, 1997], if are strictly anabelomorphic, then the fields , resp. , are not isomorphic if equipped with the actions of (resp. ). Let me also remark that the construction of (resp. ) via Lubin-Tate modules using multiplicative structure (as opposed to additive structure) should be considered similar to the construction of [Joshi, 2019] of the universal formal group with multiplicative monoid actions and its relation to Lubin-Tate formal groups.
19 Anabelomorphy for -adic differential equations
This section is independent of the rest of the paper. A reference for this material contained in this section is [André, 2003]. Here I provide a synchronization theorem for -adic differential equations in the sense of [André, 2003, Chap. III, Section 3]. Let be a geometrically connected, smooth, quasi-projective variety over a -adic field . Let denote the strictly analytic Berkovitch space associated to . By the Riemann-Hilbert Correspondence, I mean [André, 2003, Chapter III, Theorem 3.4.6].
Theorem 19.1 (Synchronization of -adic differential equations).
Let and be two geometrically connected, smooth, quasi-projective varieties over -adic fields and . Assume that and are anabelomorphic strictly analytic spaces (i.e. (where the fundamental groups with respect to a -rational (resp. an -rational) base point)). Then there exists a natural bijection between -adic differentials on and which associates to a -adic differential equation on , a -adic differential equation such that the associated (discrete) monodromy representation of is given composing with .
Let be a geometrically connected, smooth, quasi-projective variety over a -adic field . Let be anabelomorphic -adic fields containing . Then given any . Then one can consider our -adic differential equation as a -adic differential equation on and . In particular, it is possible to ask if there are quantities, properties algebraic structures associated to a differential equation on which are weakly unamphoric (i.e. with respect to anabelomorphisms ). When I speak of a weakly amphoric quantity (resp. property, alg. structure) associated to a -adic differential equation, I mean weak amphoricity (resp. weak unamphoricity) with respect to anabelomorphisms .
An important invariant of interest is the index of irregularity of a -adic differential equation at a singular point. Since it is well-known that the analog, in theory of differential equations, of the local index of irregularity is the Swan conductor of a Galois representation. Hence, the following conjecture is natural given my earlier results Theorem 9.1 on the weak unamphoricity of the Swan conductor:
Conjecture 19.2 (Index of Irregularity is weakly unamphoric).
In the situation of the above corollary, assume that is a curve (i.e. ) and let be a finite extension. Then the index of irregularity of a -adic differential equation on is weakly unamphoric. More generally, the irregularity module of the differential equation over is weakly unamphoric ( need not be a curve for this).
Remark 19.3.
I do not have any evidence for this conjecture at the moment except for my analogy with my results on the Swan conductor (Theorem 9.1) and the well-known analogy between the Swan conductor and the index of irregularity.
20 Anabelomorphy at Archimedean primes
In [Mochizuki, 2012, 2013, 2015] and especially in [Mochizuki, 2021a, b, c, d] the theory of elliptic curves at archimedean primes poses some difficulty (this is also discussed in [Dupuy and Hilado, 2020b]). The reason is this: on one hand any pure -Hodge structure is semi-simple, on the other hand there are no one dimensional -Hodge structures of weight one, and so the Hodge structure of an elliptic curve is indecomposable as a -Hodge structure. This is in contrast to the situation at the non-archimedean primes of semi-stable reduction (where the Galois representation is in fact reducible). I want to explain how to circumvent this difficulty and provide a description parallel to Theorem 14.1.1 at infinity. One should think of Theorem 20.6 (see below) as the Ordinary Synchronization Theorem at Infinity. The theory of this section, especially Theorem 20.11 should also be compared with [Mochizuki, 2009] where Mochizuki constructs Galois cohomology classes (in corresponding to -functions on an elliptic curve.
For the Diophantine applications which Mochizuki considers in [Mochizuki, 2021a, b, c, d], let be a number field which one typically assumes to have no real embeddings. Let be an elliptic curve and assume that the Faltings height of is large. By the known facts about Faltings height, corresponds to and equivalently this means that the Schottky (uniformization) parameter of is small.
Schottky uniformization of elliptic curves says that one has an isomorphism of complex abelian manifolds
at infinity (let me remind the readers that Tate’s Theory of -adic uniformization of elliptic curves is modeled on Schottky uniformization of elliptic curves). So the theory of elliptic curves of large Faltings height corresponds to the theory of complex tori with a small Schottky parameter. To describe this in parallel with the Theory of Tate curves at non-archimedean primes, let me begin by recalling the following well-known fact from mixed Hodge Theory ([Carlson, 1987], [Deligne, 1997])
Lemma 20.1.
One has an isomorphism of abelian groups:
In particular, the Schottky parameter provides a unique mixed Hodge structure
(not to be confused with the usual Hodge structure which is of weight one. The mixed Hodge structure comes equipped with a weight filtration and unipotent monodromy (see [Deligne, 1997]). In particular, let me recall the formula from [Deligne, 1997]:
(20.2) | |||||
(20.3) | |||||
(20.4) | |||||
(20.5) |
The mapping is given by and is given by . Then one has an exact sequence of mixed Hodge structures
whose class in is given by .
Now let with and let where is a suitable Jacobi Theta function on . For , and hence provides us a mixed Hodge structure given by .
Thus I have proved the following:
Theorem 20.6.
Let be an elliptic curve with Schottky parameter such that . Then
-
(1)
there is mixed Hodge structure whose extension class corresponds to , and
-
(2)
there is a mixed Hodge structure whose extension class corresponds to the -value .
Remark 20.7.
Remark 20.8.
Comparing the definition above of and with the formula of Fontaine for -invariant, I define the -invariant . If then ! So is the -invariant of the elliptic curve at archimedean primes and anabelomorphy changes the -invariant at all the places.
Let me remark that the construction given above can be extended to provide results over a geometric base scheme (see [Deligne, 1997]). For example let be an elliptic curve and let . Let be a meromorphic function on which is an invertible function on . More generally, one can consider any open subset of and consider i.e. an invertible function on . Then there exists a variation of mixed Hodge structures (over ) such that under the natural identification
the extension class corresponding to is equal to . The mixed Hodge structure is constructed as follows (see [Deligne, 1997]). Let be a locally free module with basis . The connection (with log-poles at ) on is defined by
The rest of the data required to define a variation of mixed Hodge structures is defined by the formulae above. Let me remark that the triple consisting of the bundle together with the connection and the Hodge filtration is the data of an indigenous bundle (equivalently a rank two oper) on .
So one can apply this consideration to a chosen such as a theta function on which does not vanish on the open set . By the theory of theta functions, up to scaling by a constant, there is a unique function with this property, denoted by . Note that a theta function is, strictly speaking, not a function on the curve as it is quasi-periodic. But by [Whittaker and Watson, 1996], the logarithmic derivative of any of the four standard theta functions with periods satisfies
(20.9) | |||||
(20.10) |
More precisely, there is a vector bundle on of rank two and a connection on , with log-poles at , which on the universal cover of is given by the connection matrix as above with . At any rate, the connection defined by the above formula on descends to (with log-poles at ). Hence one has proved that
Theorem 20.11.
Let be an elliptic curve with Schottky parameter such that and let . Let be a Theta function on which does not vanish on and normalized so that . Then there is a variation of mixed Hodge structures over , denoted
such that the extension class of corresponds to (here is the group of holomorphic functions which are invertible on ). This class is compatible with the class constructed above.
Remark 20.12.
Let me remark that this construction is anabelomorphic. Here is how one sees this in greater generality. Let be a non-proper hyperbolic Riemann surface, its topological fundamental group. Let be the group ring and be the augmentation ideal. By well-known results for each , carries a mixed Hodge structure and good unipotent variations of mixed Hodge structures on of nilpotence with values in (or a real field) arise precisely from finite dimensional representations of such that the natural map is a morphism of mixed Hodge structures ([Hain and Zucker, 1987, Theorem ]). The Yoneda ext-group in the category of good unipotent variations of mixed Hodge structure on , denoted is also described, by [Carlson and Hain, 1989, Theorem 12.1] in an essentially anabelomorphic way, as follows:
The cohomology is Beilinson’s Absolute Hodge Cohomology. The middle isomorphism makes it clear that the group of extensions on the right is anabelomorphic (in the complex analytic space ).
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