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On Mochizuki’s Idea of Anabelomorphy and its applications

Kirti Joshi

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 pp-adic field is determined by its absolute Galois group equipped with the upper numbering ramification filtration [Mochizuki, 1997].

The case of pp-adic fields is already quite non-trivial and hence this Introduction will focus on this case. Two pp-adic fields K,LK,L 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 pp-adic fields. Isomorphic pp-adic fields are anabelomorphic, but there exist many non-isomorphic but anabelomorphic pp-adic fields (Lemma 4.4).

A quantity (resp. a property, an algebraic structure) associated with a pp-adic field is said to be amphoric if it depends only on the anabelomorphism class of KK i.e. if two pp-adic fields K,LK,L in the same anabelomorphism class have the same quantity (resp. same property, isomorphic algebraic structures). The amphora of GKG_{K} is the collection of all quantities, properties, algebraic structures associated with KK which depend only on the anabelomorphism class of KK. For example if KK is a pp-adic local field, then the following are examples of an amphoric quantity, property, algebraic structures respectively: the residue characteristic pp of KK, the property of unramifiedness of K/pK/{\mathbb{Q}}_{p}, and the topological group KK^{*} (Theorem 2.4.3).

The existence of anabelomorphic pp-adic fields which are not isomorphic means that within the anabelomorphism class of KK, the additive structure of a pp-adic field KK deforms or wiggles around while the multiplicative structure of KK (i.e. the topological group KK^{*}) 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 pp-adic fields K,LK,L are anabelomorphic, one can view representations of GKG_{K} as representations of GLG_{L}. Thus Anabelomorphy of pp-adic fields has immediate applications to the theory of representations of the absolute Galois group of a pp-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 pp-adic field is a Galois theoretic stand-in for the additive structure of a pp-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 ΦSen\Phi_{\rm Sen} under anabelomorphy. In Theorem 8.1, I show that the 𝔏\mathfrak{L}-invariant (which given, for a Tate elliptic curve with Tate parameter qq, by 𝔏=logK(q)ordK(q)\mathfrak{L}=\frac{\log_{K}(q)}{\mathop{\rm ord}\nolimits_{K}({q})}) is unamphoric. Another important observation is that the Fontaine subspace of ordinary crystalline two dimensional representations of GKG_{K} 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 pp-adic field (or a local field of characteristic p>0p>0). So the natural question which arises is this: If two pp-adic fields K,LK,L 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 pp-adic fields KLK\leftrightsquigarrow L, one can also synchronize or match local automorphic principle series representations of GLn(K){\rm GL}_{n}(K) and GLn(L){\rm GL}_{n}(L) i.e. the principal series representations are amphoric (here K,LK,L are only assumed to be anabelomorphic and there may be not exist any (abstract) field isomorphism between them at all). If p2p\neq 2 and n=2n=2, then one can also synchronize supercuspidal representations of GL2(K){\rm GL_{2}}(K) and GL2(L){\rm GL_{2}}(L) in a manner compatible with the Local Langlands Correspondence (§ 15, Theorem 15.2.2, Theorem 15.3.2). The situation for GLn{\rm GL}_{n} (n>2n>2) 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 pp-adic field and the case of étale fundamental groups of varieties over number fields or pp-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 MM 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 pp-adic topologies for anabelomorphically connected number fields. Simplest version of this anabelomorpphic version of Moret-Bailly’s Theorem is Theorem 16.1.1 (for 1{0,1,}{\mathbb{P}}^{1}-\{0,1,\infty\}). 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 E/KE/K is an elliptic curve such that EE has semi-stable reduction at v1,,vn{v}_{1},\ldots,{v}_{n} and if (K,{v1,,vn})(K,{w1,,wn})\left({K},\{{v}_{1},\ldots,{v}_{n}\}\right)\leftrightsquigarrow\left({K^{\prime}},\{{w}_{1},\ldots,{w}_{n}\}\right) is any anabelomorphically connected number field then there exists an elliptic curve E/KE^{\prime}/K^{\prime} with ordvi(jE)=ordwi(jE)\mathop{\rm ord}\nolimits_{v_{i}}(j_{E})=\mathop{\rm ord}\nolimits_{w_{i}}(j_{E^{\prime}}) and with potentially good reduction at all other non-archimedean primes of KK^{\prime}.

§ 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 p{\mathbb{Q}}_{p} when viewed over two anabelomorphic extensions of p{\mathbb{Q}}_{p}. 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 EE over a pp-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 pp-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 pp-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 pp-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

In § 18, I show that anabelomorphy also appears non-trivially in the theory of perfectoid fields and perfectoid spaces considered in [Scholze, 2012].

§ 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 Aut(G){\rm Aut}(G)-indeterminacy, where GG 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 GG 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 pp-adic fields KK and LL respectively. If K,LK,L are anabelomorphic (i.e. KLK\leftrightsquigarrow L) then there is a worm-hole or a conduit through which one can funnel arithmetic/geometric information in the KK-universe to the LL-universe through the choice of an isomorphism of Galois groups GKGLG_{K}\simeq G_{L}, which serves as a wormhole. Information is transfered by means of amphoric quantities, properties and algebraic structures. The KK and LL universes themselves follow different laws (of algebra) as addition has different meaning in the two anabelomorphic fields K,LK,L (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 pp-adic Hodge theory. I was fortunate enough to learn pp-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 pp-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 abcabc-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 pp be a fixed prime number. Occasionally I will write \ell for an arbitrary prime number not equal to pp. By a pp-adic field I mean a finite extension of p{\mathbb{Q}}_{p}. Let KK be a field and let X/KX/K be a geometrically connected, smooth quasi-projective variety over KK (the case X=Spec(K)X={\rm Spec}(K) is perfectly reasonable for understanding the definitions given below. By and large I will assume that KK is either a pp-adic field or a number field but the ideas presented here can be used in wider context.

For a field KK, let K¯\bar{K} be a separable closure of KK (note the conflation of standard notation KsepK^{sep} and K¯\bar{K}), GK=Gal(K¯/K)G_{K}={\rm Gal}(\bar{K}/K) be its absolute Galois group considered as a topological group, IKGKI_{K}\subset G_{K} (resp. PKGKP_{K}\subset G_{K}) the inertia (resp. wild inertia) subgroup of GKG_{K}.

§ 2.1  Definitions

Definition 2.1.1.

Let K,LK,L be two pp-adic fields or number fields.

  1. (1)

    I will say that K,LK,L are anabelomorphic or anabelomorphs (or anabelomorphs of each other) if their absolute Galois groups are topologically isomorphic GKGLG_{K}\simeq G_{L}. I will write KLK\leftrightsquigarrow L if K,LK,L are anabelomorphic and α:KL\alpha:K\leftrightsquigarrow L will mean a specific isomorphism α:GKGL\alpha:G_{K}\to G_{L} of topological groups.

  2. (2)

    Obviously if LLL\leftrightsquigarrow L^{\prime} and LL′′L^{\prime}\leftrightsquigarrow L^{\prime\prime} then LL′′L\leftrightsquigarrow L^{\prime\prime}. So anabelomorphism is an equivalence relation on pp-adic fields.

  3. (3)

    The collection of all fields LL which are anabelomorphic to KK will be called the anabelomorphism class of KK.

  4. (4)

    I will say that KK is strictly anabelomorphic to LL or that KLK\leftrightsquigarrow L is a strict anabelomorphism if KLK\leftrightsquigarrow L but KK is not isomorphic to LL.

Remark 2.1.2.

By the observations of § 18, one can also extend the above definition to include perfectoid fields. \bullet

Definition 2.1.3.

Let K,LK,L be two pp-adic fields or number fields. A quantity QKQ_{K} or an algebraic structure AKA_{K} or a property 𝒫\mathscr{P} of KK 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 KK. More precisely, if α:KL\alpha:K\leftrightsquigarrow L is an anabelomorphism of fields then QK=QLQ_{K}=Q_{L}, AKALA_{K}\simeq A_{L} and LL also has property 𝒫\mathscr{P}.

In § 2.4, the reader will find examples of illustrating the non-triviality of these definitions.

Definition 2.1.4.

Let KK be a field. I will say that KK is anabelomorphically rigid if whenever one has an anabelomorphism KLK\leftrightsquigarrow L (with LL of the same sort as X/KX/K), one has an isomorphism of fields KLK\simeq L.

§ 2.2  Anabelomorphy of quasi-projective varieties

The definition of anabelomorphy of fields readily extends to smooth varieties of higher dimensions. If X/KX/K is a geometrically connected, smooth quasi-projective variety over KK then write ΠX/K\Pi_{X/K} (resp. ΠX/Ktemp\Pi^{temp}_{X/K}) for its étale (resp. tempered) fundamental group of X/KX/K. If X=Spec(K)X={\rm Spec}(K) then both these groups coincide with GKG_{K}.

Anabelomorphism (resp. tempered anabelomorphism) also defines an equivalence relation on smooth varieties over pp-adic fields.

Evidently isomorphic varieties over a pp-adic field are anabelomorphic (over that field).

Definition 2.2.1.
  1. (1)

    Let K,LK,L be two fields. I will say that K,LK,L are anabelomorphic or anabelomorphs (or anabelomorphs of each other) if and only if their absolute Galois groups are topologically isomorphic

    GKGL.G_{K}\simeq G_{L}.
  2. (2)

    More generally, if X/KX/K and Y/LY/L are two geometrically connected, smooth, quasi-projective varieties, then I will say that X/KX/K is anabelomorphic to Y/LY/L if one has a topological isomorphism of the étale fundamental groups

    ΠX/KΠY/L.\Pi_{X/K}\simeq\Pi_{Y/L}.

    Especially, if X=Spec(K)X={\rm Spec}(K) and Y=Spec(L)Y={\rm Spec}(L) then X/KX/K and Y/LY/L are anabelomorphic if and only if the fields KK and LL are anabelomorphic. If K,LK,L are pp-adic fields one may similarly define the term ‘tempered anabelomorphic.’

  3. (3)

    I will write X/KY/LX/K\leftrightsquigarrow Y/L if X/K,Y/LX/K,Y/L are anabelomorphic and the notation

    α:X/KY/L\alpha:X/K\leftrightsquigarrow Y/L

    will mean that we are given a specific isomorphism

    α:ΠX/KΠY/L\alpha:\Pi_{X/K}{\lx@xy@svg{\hbox{\raise 0.0pt\hbox{\kern 3.0pt\hbox{\ignorespaces\ignorespaces\ignorespaces\hbox{\vtop{\kern 0.0pt\offinterlineskip\halign{\entry@#!@&&\entry@@#!@\cr&\crcr}}}\ignorespaces{\hbox{\kern-3.0pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise 0.0pt\hbox{$\textstyle{{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern 9.27777pt\raise 4.62312pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.62312pt\hbox{$\scriptstyle{\simeq}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern 27.0pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}{\hbox{\kern 27.0pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise 0.0pt\hbox{$\textstyle{}$}}}}}}}\ignorespaces}}}}\ignorespaces}\Pi_{Y/L}

    of topological groups. For the case X=Spec(K)X={\rm Spec}(K) and Y=Spec(L)Y={\rm Spec}(L), I will write KLK\leftrightsquigarrow L if KK and LL are anabelomorphic.

  4. (4)

    I will say that X/KX/K is strictly anabelomorphic to Y/LY/L or that X/KY/LX/K\leftrightsquigarrow Y/L is a strict anabelomorphism if X/KY/LX/K\leftrightsquigarrow Y/L but X/KX/K is not isomorphic to Y/LY/L.

  5. (5)

    Obviously if X/LX/LX/L\leftrightsquigarrow X^{\prime}/L^{\prime} and X/LX′′/L′′X^{\prime}/L^{\prime}\leftrightsquigarrow X^{\prime\prime}/L^{\prime\prime} then X/LX′′/L′′X/L\leftrightsquigarrow X^{\prime\prime}/L^{\prime\prime}. So anabelomorphy is an equivalence relation. The collection of all smooth, geometrically connected quasi-projective varieties Y/LY/L which are anabelomorphic to X/KX/K will be called the anabelomorphism class of X/KX/K.

The following is fundamental in understanding anabelomorphy of varieties:

Proposition 2.2.2.

Suppose K,LK,L are finite fields, pp-adic fields or number fields. Let X/K,Y/LX/K,Y/L are geometrically connected, smooth, quasi-projective varieties and if

X/KY/LX/K\leftrightsquigarrow Y/L

is an anabelomorphism between them, then one has an anabelomorphism

KL.K\leftrightsquigarrow L.

Proof.

This is [Mochizuki, 2012, Corollary 2.8(ii)].

Definition 2.2.3.

Let X/KX/K be a geometrically connected, smooth, quasi-projective variety over a field KK. I will say that X/KX/K is anabelomorphically rigid if any anabelomorphism α:X/KY/L\alpha:X/K\leftrightsquigarrow Y/L (with Y/LY/L of the same sort as X/KX/K), one has an isomorphism of {\mathbb{Z}}-schemes XYX\simeq Y.

Remark 2.2.4.

Here I use term ‘same sort’ in the following sense: if KK is a pp-adic field then LL is of this type, if KK is a number field then so is LL; if X/KX/K is a hyperbolic curve then Y/LY/L 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 X/KX/K. \bullet

Definition 2.2.5.

Let X/KX/K be a geometrically connected, smooth, quasi-projective variety over a pp-adic field KK. A quantity QX/KQ_{X/K} or an algebraic structure AX/KA_{X/K} or a property of 𝒫X/K\mathscr{P}_{X/K} associated to X/KX/K 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 X/KX/K i.e. it depends only on the isomorphism class of the topological group ΠX/K\Pi_{X/K}. More precisely: if α:ΠX/KΠY/L\alpha:\Pi_{X/K}\simeq\Pi_{Y/L} is an isomorphism of topological groups then α\alpha takes the quantity QX/KQ_{X/K} (resp. algebraic structure AX/KA_{X/K}, property 𝒫X/K\mathscr{P}_{X/K}) for X/KX/K to the corresponding quantity (resp. alg. structure, property) of Y/LY/L. If a quantity (resp. alg. structure, property) of X/KX/K 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 X/KX/K is called the amphora of the topological group ΠX/K\Pi_{X/K}.

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. \bullet

§ 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 EE which will serve as a coefficient field for representations of GKG_{K} (for example E=E={\mathbb{Q}}_{\ell} for any prime \ell including =p\ell=p and =\ell=\infty will be more than adequate for my discussion). Let V/EV/E be a finite dimensional EE-vector space (as a topological vector space). Let ρ:GKGL(V)\rho:G_{K}\to{\rm GL}(V) be a continuous representation of GKG_{K}. I will say that a quantity or an algebraic structure or a property of the triple (GK,ρ,V)(G_{K},\rho,V) is amphoric if it is determined by the anabelomorphism class of KK.

§ 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 K,LK,L are number fields then KK is anabelomorphic to LL if and only if KK is isomorphic to LL i.e.

KLKL.K\leftrightsquigarrow L\iff K\simeq L.

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 K,LK,L are pp-adic fields then KLK\simeq L if and only if there is a topological isomorphism of their Galois groups equipped with the respective (upper numbering) inertia filtration i.e. (GK,GK)(GL,GL)(G_{K},G_{K}^{\small{\bullet}})\simeq(G_{L},G_{L}^{\small{\bullet}})

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 KK be a pp-adic field. Then

  1. (1)

    The residue characteristic pp of KK is amphoric.

  2. (2)

    The degree [K:p][K:{\mathbb{Q}}_{p}] and eKe_{K} the absolute ramification index are amphoric.

  3. (3)

    The topological groups KK^{*} and 𝒪K{\mathscr{O}}_{K}^{*} (viewed as a topological p{\mathbb{Z}}_{p}-module) are amphoric.

  4. (4)

    The inertia subgroup IKI_{K} and the wild inertia subgroup PKP_{K} are amphoric.

  5. (5)

    The pp-adic cyclotomic character χp:GKp\chi_{p}:G_{K}\to{\mathbb{Z}}_{p}^{*} is amphoric.

Proof.

For modern proof of the first three assertions see [Hoshi, 2021]; for the last assertion see [Mochizuki, 1997].

Remark 2.4.4.

Hoshi’s paper also provides a longer list of amphoric quantities, properties and alg. structures. \bullet

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 K,LK,L be pp-adic fields with ζpK\zeta_{p}\in K and both K,LK,L contained in ¯p{\bar{{\mathbb{Q}}}}_{p}. Write KK0pK\supseteq K^{0}\supseteq{\mathbb{Q}}_{p} (resp. LL0pL\supseteq L^{0}\supseteq{\mathbb{Q}}_{p}) be the maximal abelian subfield contained in KK. Then the following are equivalent:

  1. (1)

    KLK\leftrightsquigarrow L

  2. (2)

    [K:p]=[L:p][K:{\mathbb{Q}}_{p}]=[L:{\mathbb{Q}}_{p}] and K0=L0K^{0}=L^{0}.

Proof.

For a proof see [Jarden and Ritter, 1979].

Theorem 2.4.6 (Fifth Fundamental Theorem of Anabelomorphy).

Let KK be a pp-adic field and let IKGKI_{K}\subseteq G_{K} (resp. PKGKP_{K}\subseteq G_{K}) be the inertia subgroup (resp. the wild inertia subgroup). Then IKI_{K} and PKP_{K} are topological characteristic subgroups of GKG_{K} (i.e. invariant under all topological automorphisms of GKG_{K}).

Proof.

For proofs see [Mochizuki, 1997] or [Hoshi, 2021].

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 pp be a prime, let ¯p{\bar{{\mathbb{Q}}}}_{p} be an algebraic closure of p{\mathbb{Q}}_{p} and let N1N\geq 1 be a positive integer. Let

N={K:K¯p and [K:p]N}.\mathscr{F}_{N}=\left\{K:K\subset{\bar{{\mathbb{Q}}}}_{p}\text{ and }[K:{\mathbb{Q}}_{p}]\leq N\right\}.

Then N\mathscr{F}_{N} is a finite union of disjoint anabelomorphism classes.

Proof.

Anabelomorphism is an equivalence relation on N\mathscr{F}_{N} and hence partitions N\mathscr{F}_{N} into a disjoint union of anabelomorphism classes and it is well-known that N\mathscr{F}_{N} is a finite set. Hence there are finitely many anabelomorphism classes in N\mathscr{F}_{N}.

3 Monoradicality is Amphoric

Let KK be a pp-adic field. An extension M/KM/K is a monoradical extension if it is of the form M=K(xm)M=K(\sqrt[m]{x}) for some xKx\in K and in this case xx is a generator of M/KM/K. 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 pp-adic field are unamphoric

For definition of the different and the discriminant of a pp-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 K/pK/{\mathbb{Q}}_{p} are unamphoric.

Proof.

By Theorem [Serre, 1979, Chap III, Prop 6] it is sufficient to prove that the different of K/pK/{\mathbb{Q}}_{p} is unamphoric. By Theorem [Serre, 1979, Chap IV, Prop 4] the different depends on the ramification filtration for K/pK/{\mathbb{Q}}_{p}. So in general, there exist anabelomorphs K,LK,L with distinct differents and discriminants. Here is an explicit family of examples.

Let r1r\geq 1 be an integer, pp an odd prime and let Kr=p(ζpr,ppr)K_{r}={\mathbb{Q}}_{p}(\zeta_{p^{r}},\sqrt[p^{r}]{p}) so FrKrF_{r}\subset K_{r} and let Lr=p(ζpr,1+ppr)L_{r}={\mathbb{Q}}_{p}(\zeta_{p^{r}},\sqrt[p^{r}]{1+p}). By Lemma 4.4 below one has an anabelomorphism KrLrK_{r}\leftrightsquigarrow L_{r} and hence one has GLrGKrG_{L_{r}}\simeq G_{K_{r}}. But KrK_{r} and LrL_{r} 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 Kr/pK_{r}/{\mathbb{Q}}_{p} (resp. Lr/pL_{r}/{\mathbb{Q}}_{p}) [Viviani, 2004, Theorem 5.15 and 6.13].

(4.2) vp(δ(Kr/p))\displaystyle v_{p}(\delta(K_{r}/{\mathbb{Q}}_{p})) =\displaystyle= rp2r1(p1)+p(p2r1p+1)p(p2r3+1p+1),\displaystyle rp^{2r-1}(p-1)+p\left(\frac{p^{2r}-1}{p+1}\right)-p\left(\frac{p^{2r-3}+1}{p+1}\right),
(4.3) vp(δ(Lr/p))\displaystyle v_{p}(\delta(L_{r}/{\mathbb{Q}}_{p})) =\displaystyle= pr(rpr(r+1)pr1)+2(p2r1p+1).\displaystyle p^{r}\left(r\cdot p^{r}-(r+1)\cdot p^{r-1}\right)+2\left(\frac{p^{2r}-1}{p+1}\right).

In particular, for r=1r=1 these are equal to 2p(p1)+12p(p-1)+1 and p22p^{2}-2 respectively and evidently 2p(p1)+1p222p(p-1)+1\neq p^{2}-2 for any odd prime pp. This proves the assertion.

Lemma 4.4.

Let r1r\geq 1 be any integer and pp any odd prime. Let Fr=p(ζpr)F_{r}={\mathbb{Q}}_{p}(\zeta_{p^{r}}) and let Kr=p(ζpr,ppr)K_{r}={\mathbb{Q}}_{p}(\zeta_{p^{r}},\sqrt[p^{r}]{p}) and let Lr=p(ζpr,1+ppr)L_{r}={\mathbb{Q}}_{p}(\zeta_{p^{r}},\sqrt[p^{r}]{1+p}). Then one has

GLrGKr equivalently KrLr equivalently Kr and Lr are anabelomorphic.G_{L_{r}}\simeq G_{K_{r}}\text{ equivalently }K_{r}\leftrightsquigarrow L_{r}\text{ equivalently }K_{r}\text{ and }L_{r}\text{ are anabelomorphic}.

Proof.

Both fields contain Fr=p(ζpr)F_{r}={\mathbb{Q}}_{p}(\zeta_{p^{r}}) and by elementary Galois theory and Kummer theory one checks that FrKrF_{r}\subset K_{r} and FrLrF_{r}\subset L_{r} is the maximal abelian subfield of both Kr,LrK_{r},L_{r} and both Kr,LrK_{r},L_{r} have the same degree over p{\mathbb{Q}}_{p}. The Jarden-Ritter Theorem [Jarden and Ritter, 1979] says in this situation that the absolute Galois groups of Kr,LrK_{r},L_{r} are isomorphic i.e. KrLrK_{r}\leftrightsquigarrow L_{r}. Hence the claim.

Let me set up some notation for my next result. For a pp-adic field K/pK/{\mathbb{Q}}_{p} write 𝔡(K/p)\mathfrak{d}(K/{\mathbb{Q}}_{p}) for the different of K/pK/{\mathbb{Q}}_{p}. This is an ideal of 𝒪K{\mathscr{O}}_{K}. Valuation on 𝒪K{\mathscr{O}}_{K} is normalized so that vK(π)=1v_{K}(\pi)=1 for any uniformizer π\pi of 𝒪K{\mathscr{O}}_{K}. 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 KK be a pp-adic field. Then there exists an absolute constant A=A(K)0A=A(K)\geq 0 determined by the anabelomorphism class of KK such that for all LKL\leftrightsquigarrow K one has

vL(𝔡(L/p))A.v_{L}(\mathfrak{d}(L/{\mathbb{Q}}_{p}))\leq A.

Proof.

Let LKL\leftrightsquigarrow K. Let n=[L:p]n=[L:{\mathbb{Q}}_{p}], f=f(L/p)f=f(L/{\mathbb{Q}}_{p}) be the residue field degree for L/pL/{\mathbb{Q}}_{p} and e=e(L/p)e=e(L/{\mathbb{Q}}_{p}) be the absolute ramification index. Then it is well-known, (see [Artin, 2006]) that one has

vL(𝔡(L/p))e1+nf.v_{L}(\mathfrak{d}(L/{\mathbb{Q}}_{p}))\leq e-1+\frac{n}{f}.

So it suffices to remark that n,f,en,f,e are amphoric quantities and hence depend only on the anabelomorphism class of LL equivalently on the anabelomorphism class of KK. So now take

A(K)=supLK(vL(𝔡(L/p)))e1+nf.A(K)=\sup_{L\leftrightsquigarrow K}(v_{L}(\mathfrak{d}(L/{\mathbb{Q}}_{p})))\leq e-1+\frac{n}{f}.

Hence the assertion.

Table 4.1: Fragment of data on unamphoricity of discriminants of anabelomorphic fields. Let L=(ζ9,a9)L={\mathbb{Q}}(\zeta_{9},\sqrt[9]{a}) the table lists pairs [a,v(dL/p)][a,v(d_{L/{\mathbb{Q}}_{p}})]
[a,v3(dL/p)][a,v_{3}(d_{L/{\mathbb{Q}}_{p}})]
[3,165][3,165]
[4,121][4,121]
[-7, 121]
[10ζ94+5ζ9225ζ9+5,189][10\zeta_{9}^{4}+5\zeta_{9}^{2}-25\zeta_{9}+5,189]
[15ζ955ζ9425ζ9+5,165][-15\zeta_{9}^{5}-5\zeta_{9}^{4}-25\zeta_{9}+5,165]
[15ζ9210ζ9,189][15\zeta_{9}^{2}-10\zeta_{9},189]
[10ζ95+10ζ945ζ9370ζ92+15ζ95,181][-10\zeta_{9}^{5}+10\zeta_{9}^{4}-5\zeta_{9}^{3}-70\zeta_{9}^{2}+15\zeta_{9}-5,181]
[20ζ955ζ94+10ζ9315ζ92+5ζ9+10,197][-20\zeta_{9}^{5}-5\zeta_{9}^{4}+10\zeta_{9}^{3}-15\zeta_{9}^{2}+5\zeta_{9}+10,197]
[5ζ95+105ζ94+5ζ92+20ζ915,189][-5\zeta_{9}^{5}+105\zeta_{9}^{4}+5\zeta_{9}^{2}+20\zeta_{9}-15,189]
[10ζ95+20ζ92+5ζ95,197][10\zeta_{9}^{5}+20\zeta_{9}^{2}+5\zeta_{9}-5,197]
[5ζ955ζ94150ζ9310ζ92+5ζ925,157][-5\zeta_{9}^{5}-5\zeta_{9}^{4}-150\zeta_{9}^{3}-10\zeta_{9}^{2}+5\zeta_{9}-25,157]
[5ζ94+5ζ9220ζ9+15,181][-5\zeta_{9}^{4}+5\zeta_{9}^{2}-20\zeta_{9}+15,181]
[30ζ95+5ζ94+5ζ935ζ9,165][-30\zeta_{9}^{5}+5\zeta_{9}^{4}+5\zeta_{9}^{3}-5\zeta_{9},165]
[3ζ94+z33ζ92+33ζ94,145][-3\zeta_{9}^{4}+z^{3}-3\zeta_{9}^{2}+33\zeta_{9}-4,145]
[6ζ922,141][-6\zeta_{9}^{2}-2,141]
[22ζ95+2ζ94+6ζ93+2ζ9+6,181][22\zeta_{9}^{5}+2\zeta_{9}^{4}+6\zeta_{9}^{3}+2\zeta_{9}+6,181]
[2ζ9426ζ93+2ζ9212,181][2\zeta_{9}^{4}-26\zeta_{9}^{3}+2\zeta_{9}^{2}-12,181]
[2ζ952ζ942ζ92+4ζ92,197][2\zeta_{9}^{5}-2\zeta_{9}^{4}-2\zeta_{9}^{2}+4\zeta_{9}-2,197]
[6ζ95+10ζ922ζ9+2,181][-6\zeta_{9}^{5}+10\zeta_{9}^{2}-2\zeta_{9}+2,181]
[3ζ946ζ9+3,157][-3\zeta_{9}^{4}-6\zeta_{9}+3,157]
[39ζ95+87ζ949ζ9315ζ912,197][39\zeta_{9}^{5}+87\zeta_{9}^{4}-9\zeta_{9}^{3}-15\zeta_{9}-12,197]
[3ζ95+6ζ9424ζ93+21ζ92+18ζ93,189][-3\zeta_{9}^{5}+6\zeta_{9}^{4}-24\zeta_{9}^{3}+21\zeta_{9}^{2}+18\zeta_{9}-3,189]
[6ζ95+3ζ94+3ζ933ζ92+3ζ93,197][6\zeta_{9}^{5}+3\zeta_{9}^{4}+3\zeta_{9}^{3}-3\zeta_{9}^{2}+3\zeta_{9}-3,197]
[3ζ953ζ94+6ζ948,181][3\zeta_{9}^{5}-3\zeta_{9}^{4}+6\zeta_{9}-48,181]
[3ζ95+6ζ943ζ9312ζ923,189][-3\zeta_{9}^{5}+6\zeta_{9}^{4}-3\zeta_{9}^{3}-12\zeta_{9}^{2}-3,189]

5 Unramifiedness and tame ramifiedness of a local Galois representation are amphoric

Let KK be a pp-adic field. In this section I consider continuous GKG_{K} representations with values in some finite dimensional vector space over some coefficient field EE which will be a finite extension of one of the following fields: ,p{\mathbb{Q}}_{\ell},{\mathbb{Q}}_{p} or a finite field 𝔽p{\mathbb{F}}_{p}. All representations will be assumed to be continuous (with the discrete topology on VV if EE is a finite field) without further mention.

Let ρ:GKGL(V)\rho:G_{K}\to{\rm GL}(V) be a representation of GKG_{K}. Let α:KL\alpha:K\leftrightsquigarrow L be an anabelomorphism. Then as α:GKGL\alpha:G_{K}\simeq G_{L}, so any GKG_{K}-representation gives rise to a GLG_{L}-representation by composing with α1:GLGK\alpha^{-1}:G_{L}\to G_{K} and conversely, any GLG_{L}-representation gives rise to a GKG_{K} representation by composing with α:GKGL\alpha:G_{K}\to G_{L}. One sees immediately that this isomorphism induces an equivalence between categories of finite dimensional continuous representations. In particular, the category of GKG_{K}-representations is amphoric.

Now suppose WVW\subset V is a GKG_{K}-stable subspace. Let α:GLGK\alpha:G_{L}\to G_{K} be an anabelomorphism. Then WW is also a GLG_{L} stable subspace of VV. This is clear as ρ(α(g))(W)ρ(W)W\rho(\alpha(g))(W)\subseteq\rho(W)\subseteq W for all gGLg\in G_{L}. In particular, if ρ\rho is a reducible representation of GKG_{K} then so is the associated GLG_{L}-representation. Conversely, any reducible GLG_{L}-representation provides a reducible GKG_{K} representation. This discussion is summarized in the following elementary but useful result:

Proposition 5.1.

Let KK be a pp-adic field and let EE be a coefficient field.

  1. (1)

    The category of finite dimensional EE-representations of GKG_{K} is amphoric.

  2. (2)

    Irreducibility of a GKG_{K}-representation is an amphoric property.

Proof.

This is clear from the definitions.

Recall that a Galois representation ρ:GKGL(V)\rho:G_{K}\to{\rm GL}(V) is said to be an unramified representation (resp. tamely ramified) if ρ(IK)={1}\rho(I_{K})=\{1\} (resp. ρ(PK)={1}\rho(P_{K})=\{1\}.

Recall that ρ:GKGL(V)\rho:G_{K}\to{\rm GL}(V) is unramified (resp. tamely ramified) if the image ρ(IK)=1\rho(I_{K})=1 (resp. ρ(PK)=1\rho(P_{K})=1).

Theorem 5.2.

Let KK be a pp-adic local field. Unramifiedness (resp. tame ramifiedness) of ρ:GKGL(V)\rho:G_{K}\to{\rm GL}(V) are amphoric properties.

Proof.

This is clear from the definition of unramifiedness (resp. tame ramifiedness) and the fact that IKI_{K} (resp. PKP_{K}) 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 \ell-adic and the pp-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 ρ:GKGL(V)\rho:G_{K}\to{\rm GL}(V) be a continuous EE-representation of GKG_{K} with EE\supseteq{\mathbb{Q}}_{\ell} a finite extension of {\mathbb{Q}}_{\ell} (and p\ell\neq p). Then (ρ,V)(\rho,V) is said to be an ordinary representation of GKG_{K} if the image ρ(IK)\rho(I_{K}) of the inertia subgroup of GKG_{K} is unipotent. In [Fontaine, 1994b] this is called a semi-stable \ell-adic representation of GKG_{K}.

Theorem 6.1.

Assume p\ell\neq p. Then ordinarity of an \ell-adic representation ρ:GKGL(V)\rho:G_{K}\to{\rm GL}(V) is an amphoric property.

Proof.

Let ρ:GKGL(V)\rho:G_{K}\to{\rm GL}(V) be a continuous Galois representation on GKG_{K} on a finite dimensional EE vector space with E/E/{\mathbb{Q}}_{\ell} a finite extension. Let LL be a pp-adic field with an isomorphism α:GLGK\alpha:G_{L}\simeq G_{K}. By Theorem 2.4.6 [Mochizuki, 1997] or [Hoshi, 2021, Proposition 3.6] the inertia (resp. wild inertia) subgroups are amphoric. Then ρ(α(IL))ρ(IK)\rho(\alpha(I_{L}))\subset\rho(I_{K}) so the image of ILI_{L} is also unipotent.

Now before I discuss the pp-adic case, let me recall that it was shown in [Mochizuki, 1997] that for any pp-adic field KK, the pp-adic cyclotomic character of GKG_{K} is amphoric. Let χp:GKp\chi_{p}:G_{K}\to{\mathbb{Z}}_{p}^{*} be a pp-adic cyclotomic character. Recall from [Perrin-Riou, 1994] that a pp-adic representation ρ:GKGL(V)\rho:G_{K}\to{\rm GL}(V) with VV a finite dimensional p{\mathbb{Q}}_{p}-vector space is said to be an ordinary pp-adic representation of GKG_{K} if there exist GKG_{K}-stable filtration {Vi}\{V_{i}\} on VV consisting of p{\mathbb{Q}}_{p}-subspaces of VV such that the action of IKI_{K} on gri(V)\rm gr_{i}(V) is given by χpi\chi^{i}_{p} (as GKG_{K}-representations).

Theorem 6.2.

Now assume =p\ell=p. Then ordinarity of a pp-adic representation ρ:GKGL(V)\rho:G_{K}\to{\rm GL}(V) is an amphoric property.

Proof.

It is immediate from the Prop. 5.1 that the filtration ViV_{i} is also GLG_{L}-stable. By Theorem 2.4.5, χp\chi_{p} (and hence its powers) are amphoric. By definition, for any vViv\in V_{i} and any gIKg\in I_{K},

ρ(g)(v)=χpi(g)v+Vi+1.\rho(g)(v)=\chi_{p}^{i}(g)v+V_{i+1}.

Now given an isomorphism α:GLGK\alpha:G_{L}\to G_{K}, one has for all gGLg\in G_{L}

ρ(α(g))(v)=χpi(α(g))v+Vi+1,\rho(\alpha(g))(v)=\chi_{p}^{i}(\alpha(g))v+V_{i+1},

and by Mochizuki’s Theorem 2.4.3, χpα\chi_{p}\circ\alpha is the cyclotomic character of GLG_{L}. Thus this condition is determined solely by the isomorphism class of GKG_{K}.

Two dimensional ordinary (reducible) pp-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.
  1. (1)

    Let α:KL\alpha:K\leftrightsquigarrow L be an anabelomorphism of pp-adic fields. Then the following conditions are equivalent

    1. (a)

      For every Hodge-Tate representation ρ:GKGL(V)\rho:G_{K}\to{\rm GL}(V), the composite ρα\rho\circ\alpha is a Hodge-Tate representation of GLG_{L}.

    2. (b)

      KLK\simeq L.

  2. (2)

    There exists a prime pp and a pp-adic local field KK and an automorphism α:GKGK\alpha:G_{K}\to G_{K} and a crystalline representation ρ:GKGL(V)\rho:G_{K}\to{\rm GL}(V) such that ρα:GKGL(V)\rho\circ\alpha:G_{K}\to{\rm GL}(V) is not crystalline. In other words, in general crystalline-ness is an unamphoric property of ρ:GKGL(V)\rho:G_{K}\to{\rm GL}(V).

  3. (3)

    In particular, being crystalline, semi-stable or de Rham is not an amphoric property of a general pp-adic representation.

7 ΦSen\Phi_{\rm Sen} 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 pp-adic completion K¯^\hat{\bar{K}} is unamphoric. For K¯^\hat{\bar{K}}-admissible representations see [Fontaine, 1994a].

Theorem 7.1.

Let KK be a pp-adic field and let α:LK\alpha:L\leftrightsquigarrow K be an anabelomorphism. Let ρ:GKGL(V)\rho:G_{K}\to{\rm GL}(V) be a pp-adic representation.

  1. (1)

    Then VV is K¯^\hat{\bar{K}}-admissible if and only if ρα\rho\circ\alpha is L¯^\hat{\bar{L}}-admissible.

  2. (2)

    In particular, VV is pure of Hodge-Tate weight mm as a GKG_{K}-module if and only if VV is pure of Hodge-Tate weight mm as a GLG_{L}-module.

Proof.

A well-known theorem of Shankar Sen [Sen, 1980] or [Fontaine, 1994a, Proposition 3.2], VV is K¯^\hat{\bar{K}}-admissible if and only if the image of inertia ρ(IK)\rho(I_{K}) is finite. By the Third Fundamental Theorem of Anabelomorphy (Theorem 2.4.3) if ρ(IK)\rho(I_{K}) is finite then so is ρ(α(IL))\rho(\alpha(I_{L})). So the assertion follows.

Twisting VV by χpm\chi_{p}^{-m}, one can assume that VV is Hodge-Tate of weight zero as a GKG_{K}-representation. Then by Shankar Sen’s Theorem referred to earlier, image of IKI_{K} under ρ\rho is finite. Hence the image of ILI_{L} under ρα\rho\circ\alpha 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 KK be a pp-adic field and let HKGKH_{K}\subset G_{K} be the kernel of the cyclotomic character χp:GKp\chi_{p}:G_{K}\to{\mathbb{Z}}_{p}^{*}. Let K=K¯HKK_{\infty}=\bar{K}^{H_{K}} be the fixed field of HKH_{K}. Let α:LK\alpha:L\leftrightsquigarrow K be an anabelomorphism. Let HLGLH_{L}\subset G_{L} be the kernel of the cyclotomic character χp:GLp\chi_{p}:G_{L}\to{\mathbb{Z}}_{p}^{*} (note the conflation of notation made possible by the amphoricity of the cyclotomic character). Let L=L¯HLL_{\infty}=\bar{L}^{H_{L}} be the fixed field of HLH_{L}. By the amphoricity of the cyclotomic character one has an isomorphism HLHKH_{L}\simeq H_{K} and hence also of the quotients GK/HKGL/HLG_{K}/H_{K}\simeq G_{L}/H_{L}. Hence one observes that one has an anabelomorphism LKL_{\infty}\leftrightsquigarrow K_{\infty}. Consider a pp-adic representation ρ:GKGL(V)\rho:G_{K}\to{\rm GL}(V) of GKG_{K}. By a fundamental theorem of [Sen, 1980, Theorem 4], there exists an endomorphism ΦSenEnd((VK¯^)HK)\Phi_{\rm Sen}\in\rm{End}((V\otimes\hat{\bar{K}})^{H_{K}}) of the KK_{\infty}-vector space (VK¯^)HK(V\otimes\hat{\bar{K}})^{H_{K}}. Another theorem of loc. cit (see [Sen, 1980, Corollary of Theorem 6]) asserts that GKG_{K}-representation VV is Hodge-Tate if and only if ΦSen\Phi_{\rm Sen} is semi-simple and eigenvalues of ΦSen\Phi_{\rm Sen} are integers. Let me note that by [Sen, 1980, Theorem 5] one can always find a basis of (VK¯^)HK(V\otimes\hat{\bar{K}})^{H_{K}} such ΦSen\Phi_{\rm Sen} is given by a matrix with coefficients in KK. Let ΦSenα\Phi_{\rm Sen}^{\alpha} be the endomorphism of the LL_{\infty}-vector space (VL¯^)HL(V\otimes\hat{\bar{L}})^{H_{L}} (considering VV as a GLG_{L}-representation through α\alpha).

Theorem 7.2.

Let KK be a pp-adic field. Let ρ:GKGL(V)\rho:G_{K}\to{\rm GL}(V) be a pp-adic representation of GKG_{K}. Then ΦSen\Phi_{\rm Sen} is unamphoric. If α:LK\alpha:L\leftrightsquigarrow K is an anabelomorphism then ρα:GLGL(V)\rho\circ\alpha:G_{L}\to{\rm GL}(V) is Hodge-Tate if and only if ΦSenα\Phi_{\rm Sen}^{\alpha} is semi-simple and has integer eigenvalues.

One way to understand this result is to say that ΦSen\Phi_{\rm Sen} is an invariant of ρ:GKGL(V)\rho:G_{K}\to{\rm GL}(V) which depends on the additive structure of KK.

8 The 𝔏\mathfrak{L}-invariant is unamphoric

Let KK be a pp-adic field and let VV be a two dimensional ordinary ( = reducible, semi-stable) representation of GKG_{K} with coefficients in p{\mathbb{Q}}_{p} such that one has an exact sequence

0p(1)Vp(0)0.0\to{\mathbb{Q}}_{p}(1)\to V\to{\mathbb{Q}}_{p}(0)\to 0.

Then one has an invariant, defined by [Greenberg, 1994], Fontaine, and others (see [Colmez, 2010] for all the definitions and their equivalence), called the 𝔏\mathfrak{L}-invariant of VV, denoted 𝔏(V)\mathfrak{L}(V), which plays a central role in the theory of pp-adic LL-function of VV and related representations of GKG_{K}. One of the simplest, but important, consequences of anabelomorphy is the following:

Theorem 8.1.

Let KK be a pp-adic field. Let VV be as above. Then the 𝔏\mathfrak{L}-invariant, 𝔏(V)\mathfrak{L}(V), of VV is unamphoric.

For a more detailed discussion of DdR(V)D_{dR}(V) for ordinary representations see Theorem 14.2.1.

Proof.

The representation VV is an extension whose class lives in

ExtGK1(p(0),p(1))=H1(GK,p(1)),{\rm Ext}\,^{1}_{G_{K}}({\mathbb{Q}}_{p}(0),{\mathbb{Q}}_{p}(1))=H^{1}(G_{K},{\mathbb{Q}}_{p}(1)),

and this p{\mathbb{Q}}_{p}-vector space (of dimension [K:p]+1[K:{\mathbb{Q}}_{p}]+1) is also described naturally by means of Kummer theory, I will write qVq_{V} for this extension class. By [Nekovář, 1993], [Colmez, 2010], [Perrin-Riou, 1994] the space H1(GK,p(1))H^{1}(G_{K},{\mathbb{Q}}_{p}(1)) is described by two natural coordinates (logK(qV),ordK(qV))(\log_{K}(q_{V}),\mathop{\rm ord}\nolimits_{K}(q_{V})) where logK\log_{K} is the pp-adic logarithm (with logK(p)=0\log_{K}(p)=0). From [Nekovář, 1993], [Colmez, 2010] one see that

𝔏(V)=logK(qV)ordK(qV).\mathfrak{L}(V)=\frac{\log_{K}(q_{V})}{\mathop{\rm ord}\nolimits_{K}(q_{V})}.

The assertion follows from the fact the logK(u)\log_{K}(u) for a unit u𝒪Ku\in{\mathscr{O}}_{K}^{*} is an unamphoric quantity (in general) as the additive structure of the field KK which comes into play here through the use of the pp-adic logarithm is not an amphoric quantity: two anabelomorphic fields KLK\leftrightsquigarrow L may not be isomorphic as fields.

This has the following important (even for [Mochizuki, 2021a, b, c, d]) consequence:

Theorem 8.2.

Let VExtGK1(p(0),p(1))V\in{\rm Ext}\,^{1}_{G_{K}}({\mathbb{Q}}_{p}(0),{\mathbb{Q}}_{p}(1)). Then the Hodge filtration on DdR(V)D_{dR}(V) is unamphoric.

Proof.

From [Colmez, 2010] one sees that 𝔏(V)\mathfrak{L}(V) controls the Hodge filtration on the filtered (ϕ,N)(\phi,N)-module DdR(V)D_{dR}(V). Therefore one deduces that anabelomorphy changes the pp-adic Hodge filtration. See Section 14.2 for additional comments on this.

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 GKG_{K} representations will be a finite extension E/E/{\mathbb{Q}}_{\ell} with p\ell\neq p. 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 ρ:GKGL(V)\rho:G_{K}\to{\rm GL}(V) be a local Galois representation with E=E={\mathbb{Q}}_{\ell} such that the image of PKP_{K} is non-trivial. Then the Artin and the Swan conductors of ρ:GKGL(V)\rho:G_{K}\to{\rm GL}(V) 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 GKGLG_{K}\simeq G_{L} is not an isomorphism of filtered groups (by [Mochizuki, 1997]) so the Artin and the Swan conductors of the GLG_{L} representation GLGKGL(V)G_{L}\to G_{K}\to{\rm GL}(V) is not the same as that of the GKG_{K}-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 K1=p(ζp,1+pp)K_{1}={\mathbb{Q}}_{p}(\zeta_{p},\sqrt[p]{1+p}) and K2=p(ζp,pp)K_{2}={\mathbb{Q}}_{p}(\zeta_{p},\sqrt[p]{p}). Then Gal(K1/p)/p(/p)Gal(K2/p){\rm Gal}(K_{1}/{\mathbb{Q}}_{p})\simeq{\mathbb{Z}}/p\rtimes({\mathbb{Z}}/p)^{*}\simeq{\rm Gal}(K_{2}/{\mathbb{Q}}_{p}). By the character table for this finite group (see [Viviani, 2004, Theorem 3.7]), there is a unique irreducible character χ\chi of dimension p1p-1. Let fi(χ)f_{i}(\chi) for i=1,2i=1,2 denote the exponent of the Artin conductor of χ\chi. Then by [Viviani, 2004, Cor. 5.14 and 6.12] one has

(9.2) f1(χ)\displaystyle f_{1}(\chi) =\displaystyle= p\displaystyle p
(9.3) f2(χ)\displaystyle f_{2}(\chi) =\displaystyle= 2p1.\displaystyle 2p-1.

Evidently f1(χ)f2(χ)f_{1}(\chi)\neq f_{2}(\chi).

The following two results are fundamental for many applications of anabelomorphy.

Theorem 9.4.

Let ρ:GKGL(V)\rho:G_{K}\to{\rm GL}(V) be an \ell-adic representation of GKG_{K}. Then there exists a unique, smallest integer x0x\geq 0 such that in the anabelomorphism class of KK, there exists an LKL\leftrightsquigarrow K such that the Swan conductor of the GLG_{L}-representation GLGKGL(V)G_{L}\to G_{K}\to{\rm GL}(V) is xx.

Proof.

By [Katz, 1988, Prop. 1.9] or [Serre, 1979], the Swan conductor is an integer 0\geq 0. So one can pick an LKL\leftrightsquigarrow K such that the Swan conductor is minimal.

Corollary 9.5 (Anabelomorphic Level Lowering).

In the anabelomorphism class of a pp-adic field KK, there exists an anabelomorphism α:LK\alpha:L\leftrightsquigarrow K such that for any {\mathbb{Q}}_{\ell}-adic or an 𝔽{\mathbb{F}}_{\ell}-representation ρ:GKGL(V)\rho:G_{K}\to{\rm GL}(V), the GLG_{L}-representation ρα:GLGKGL(V)\rho\circ\alpha:G_{L}\to G_{K}\to{\rm GL}(V) 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 KK be a pp-adic field and KKtKnrpK\supseteq K^{t}\supseteq K^{nr}\supseteq{\mathbb{Q}}_{p} be the maximal tamely ramified (resp. maximal unramified) subextension of K/pK/{\mathbb{Q}}_{p} such that K=Knr(x1p,,xmp)K=K^{nr}(\sqrt[p]{x_{1}},\cdots,\sqrt[p]{x_{m}}) with xiKnr(Knr)px_{i}\in K^{nr}-(K^{nr})^{p} for all ii. Then KK is peu ramifiée if vKnr(xi)=0modpv_{K_{nr}}(x_{i})=0\bmod{p} for all ii, otherwise KK is tres ramifiée.

Recall from [Edixhoven, 1992, Prop 8.2] that ρ¯:GKGLn(𝔽¯q)\bar{\rho}:G_{K}\to{\rm GL}_{n}({\bar{\mathbb{F}}_{q}}) is peu ramifiée (i.e. the fixed field of its kernel is peu ramifiée) if and only ρ¯\bar{\rho} arises from a finite flat group scheme over 𝒪K{\mathscr{O}}_{K} (the ring of integers of KK).

Theorem 10.1.

The property of being peu ramifiée (resp. being tres ramifiée) extension (resp. representation) is unamphoric.

Proof.

It will be sufficient to prove that there exist pp-adic fields KLK\leftrightsquigarrow L such that K/pK/{\mathbb{Q}}_{p} is peu ramifiée and L/pL/{\mathbb{Q}}_{p} is tres ramifiée. Let K=p(ζp,pp)K={\mathbb{Q}}_{p}(\zeta_{p},\sqrt[p]{p}) and L=p(ζp,1+pp)L={\mathbb{Q}}_{p}(\zeta_{p},\sqrt[p]{1+p}). Then by [Jarden and Ritter, 1979] or by (Lemma 4.4) one has GKGLG_{K}\simeq G_{L} and by definition of [Serre, 1987, Section 2.4], KK is tres ramifiée and LL is peu ramifiée. Hence the claim.

Combining this with [Edixhoven, 1992, Prop 8.2] one gets:

Corollary 10.2.

Finite flatness of a GKG_{K}-representation (into GL(V){\rm GL}(V) with VV a finite dimensional 𝔽q{\mathbb{F}_{q}}-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 KLK\leftrightsquigarrow L be an anabelomorphism of pp-adic fields. If σGK\sigma\in G_{K} is a Frobenius element for KK. Then for any topological isomorphism α:GKGL\alpha:G_{K}{\lx@xy@svg{\hbox{\raise 0.0pt\hbox{\kern 3.0pt\hbox{\ignorespaces\ignorespaces\ignorespaces\hbox{\vtop{\kern 0.0pt\offinterlineskip\halign{\entry@#!@&&\entry@@#!@\cr&\crcr}}}\ignorespaces{\hbox{\kern-3.0pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise 0.0pt\hbox{$\textstyle{{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern 9.27777pt\raise 4.62312pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.62312pt\hbox{$\scriptstyle{\simeq}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern 27.0pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}{\hbox{\kern 27.0pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise 0.0pt\hbox{$\textstyle{}$}}}}}}}\ignorespaces}}}}\ignorespaces}G_{L}, α(σ)\alpha(\sigma) is a Frobenius element for LL.

This has the following important corollary.

Theorem 11.2.

Let KK be a pp-adic field and let ρ:GKGL(V)\rho:G_{K}\to{\rm GL}(V) be a finite dimensional continuous representation of GKG_{K} in an EE-vector space with E/E/{\mathbb{Q}}_{\ell} a finite extension and p\ell\neq p. Then the characteristic polynomial of Frobenius (=det(1Tρ(Frobp))\det(1-T\rho(Frob_{p})) is amphoric. In particular, LL-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 pp-adic field KK, let 𝒪K{\mathscr{O}}_{K} be its ring of integers, and let K=K{0}K^{*}=K-\{0\} be the topological group of all the non-zero elements of KK, let 𝒪K𝒪K{\mathscr{O}}_{K}^{*}\subset{\mathscr{O}}_{K} be the (topological) group of units.

Theorem 12.1.1.

Let α:KL\alpha:K\leftrightsquigarrow L be an anabelomorphism of pp-adic fields. Let n1n\geq 1 be an integer. Then the anabelomorphism α:KL\alpha:K\leftrightsquigarrow L induces a homeomorphism

α:𝔸n(K)𝔸n(L)\alpha:\mathbb{A}^{n}(K){\lx@xy@svg{\hbox{\raise 0.0pt\hbox{\kern 3.0pt\hbox{\ignorespaces\ignorespaces\ignorespaces\hbox{\vtop{\kern 0.0pt\offinterlineskip\halign{\entry@#!@&&\entry@@#!@\cr&\crcr}}}\ignorespaces{\hbox{\kern-3.0pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise 0.0pt\hbox{$\textstyle{{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern 9.27777pt\raise 4.62312pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.62312pt\hbox{$\scriptstyle{\simeq}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern 27.0pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}{\hbox{\kern 27.0pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise 0.0pt\hbox{$\textstyle{}$}}}}}}}\ignorespaces}}}}\ignorespaces}\mathbb{A}^{n}(L)

of topological spaces.

Proof.

By Theorem 2.4.3, one has an isomorphism of topological groups KLK^{*}\simeq L^{*} and 𝒪K𝒪L{\mathscr{O}}_{K}^{*}\simeq{\mathscr{O}}_{L}^{*}. Now by means of the pp-adic logarithm, logK\log_{K}, for KK (resp. logL\log_{L} for LL), one has an isomorphism of topological groups

logK:K𝒪Kpp,\log_{K}:K\simeq{\mathscr{O}}_{K}^{*}\otimes_{{\mathbb{Z}}_{p}}{\mathbb{Q}}_{p},

and a similar isomorphism for LL. Using this isomorphism one deduces that one has a homeomorphism

𝔸n(K)=KnLn=𝔸n(L).\mathbb{A}^{n}(K)=K^{n}\simeq L^{n}=\mathbb{A}^{n}(L).

This proves the assertion.

The following is now an immediate corollary:

Corollary 12.1.2.

Let 𝔾m\mathbb{G}_{m} be the multiplicative group (considered as an algebraic variety over a field of choice). Let a,b1a,b\geq 1 be integers. Let XK=𝔸a×𝔾mbX_{K}=\mathbb{A}^{a}\times\mathbb{G}_{m}^{b} (resp. XL=𝔸a×𝔾mbX_{L}=\mathbb{A}^{a}\times\mathbb{G}_{m}^{b}) considered as algebraic variety over KK (resp. LL). Let KLK\leftrightsquigarrow L be an anabelomorphism of pp-adic fields. Then one has an homeomorphism of topological spaces

X(K)=𝔸a(K)×𝔾mb(K)𝔸a(L)×𝔾mb(L)=X(L).X(K)=\mathbb{A}^{a}(K)\times\mathbb{G}_{m}^{b}(K)\simeq\mathbb{A}^{a}(L)\times\mathbb{G}_{m}^{b}(L)=X(L).

Proof.

The proof is clear using Theorem 12.1.1.

Theorem 12.1.3.

Let α:KL\alpha:K\leftrightsquigarrow L be an anabelomorphism of pp-adic fields. Let n1n\geq 1 be an integer. Then α:KL\alpha:K\leftrightsquigarrow L induces a homeomorphism of topological spaces:

α:n(K)n(L)\alpha:{\mathbb{P}}^{n}(K){\lx@xy@svg{\hbox{\raise 0.0pt\hbox{\kern 3.0pt\hbox{\ignorespaces\ignorespaces\ignorespaces\hbox{\vtop{\kern 0.0pt\offinterlineskip\halign{\entry@#!@&&\entry@@#!@\cr&\crcr}}}\ignorespaces{\hbox{\kern-3.0pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise 0.0pt\hbox{$\textstyle{{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern 9.27777pt\raise 4.62312pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.62312pt\hbox{$\scriptstyle{\simeq}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern 27.0pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}{\hbox{\kern 27.0pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise 0.0pt\hbox{$\textstyle{}$}}}}}}}\ignorespaces}}}}\ignorespaces}{\mathbb{P}}^{n}(L)

Proof.

Let me prove this explicitly for n=1n=1. Let KLK\leftrightsquigarrow L be an anabelomorphism. The topological space 1(K){\mathbb{P}}^{1}(K) is described by two coordinate charts U1,U21(K)U_{1},U_{2}\subset{\mathbb{P}}^{1}(K) and one has a homeomorphism

U1𝔸1(K)=KU_{1}\simeq\mathbb{A}^{1}(K)=K

and

U2=𝔸1(K)=KU_{2}=\mathbb{A}^{1}(K)=K

and

U1U2K.U_{1}\cap U_{2}\simeq K^{*}.

The topological space 1(K){\mathbb{P}}^{1}(K) is obtained by gluing U1,U2U_{1},U_{2} using the homeomorphism

U1U2Kxx1K=U1U2.U_{1}\cap U_{2}\simeq K^{*}{\lx@xy@svg{\hbox{\raise 0.0pt\hbox{\kern 3.0pt\hbox{\ignorespaces\ignorespaces\ignorespaces\hbox{\vtop{\kern 0.0pt\offinterlineskip\halign{\entry@#!@&&\entry@@#!@\cr&\crcr}}}\ignorespaces{\hbox{\kern-3.0pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise 0.0pt\hbox{$\textstyle{{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern 3.70766pt\raise 6.15pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.75pt\hbox{$\scriptstyle{x\longmapsto x^{-1}}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern 27.0pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}{\hbox{\kern 27.0pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise 0.0pt\hbox{$\textstyle{}$}}}}}}}\ignorespaces}}}}\ignorespaces}K^{*}=U_{1}\cap U_{2}.

Now suppose KLK\leftrightsquigarrow L. Thus the homeomorphism 1(K)1(L){\mathbb{P}}^{1}(K)\simeq{\mathbb{P}}^{1}(L) is constructed using this local description and the homeomorphisms

𝔸1(K)𝔸1(L)\mathbb{A}^{1}(K)\simeq\mathbb{A}^{1}(L)

and

KLK^{*}\simeq L^{*}

given above.

Now consider the general case of n1n\geq 1. The topological space n(K){\mathbb{P}}^{n}(K) is covered by n+1n+1 opens subsets Uj𝔸n(K)U_{j}\simeq\mathbb{A}^{n}(K) for j=0,,nj=0,\ldots,n and the intersections UiUjU_{i}\cap U_{j} and UiUjUkU_{i}\cap U_{j}\cap U_{k} are of the form 𝔸a(K)×𝔾mb(K)\mathbb{A}^{a}(K)\times\mathbb{G}_{m}^{b}(K) considered in Corollary 12.1.2 for suitable choices of integers a,b1a,b\geq 1. 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 KLK\leftrightsquigarrow L are anabelomorphic pp-adic fields, then one has a trivial isomorphism of algebraic fundamental groups

π1(n/K)GKGLπ1(n/L).\pi_{1}({\mathbb{P}}^{n}/K)\simeq G_{K}\simeq G_{L}\simeq\pi_{1}({\mathbb{P}}^{n}/L).

So one can consider n/K{\mathbb{P}}^{n}/K and n/L{\mathbb{P}}^{n}/L as trivially anabelomorphic varieties. \bullet

§ 12.2  Anabelomorphy and Abelian varieties with multiplicative reduction

Let me begin with the simpler example of a Tate curve over a pp-adic field KK. By a Tate elliptic curve I will mean an elliptic curve with split multiplicative reduction over a pp-adic field KK. By Tate’s theorem [Silverman, 1994] a Tate elliptic curve over KK corresponds to the data of a discrete cyclic subgroup qKKq_{K}^{\mathbb{Z}}\subset K^{*}. The equation of the Tate curve is then given by

y2+xy=x3+a4(qK)x+a6(qK),y^{2}+xy=x^{3}+a_{4}(q_{K})x+a_{6}(q_{K}),

with explicitly given convergent power series a4(qK),a6(qK)a_{4}(q_{K}),a_{6}(q_{K}) in qKq_{K}.

The main theorem is the following:

Theorem 12.2.1.

Let KK be a pp-adic field and let E/KE/K be a Tate elliptic curve over KK with Tate parameter qKKq_{K}\in K^{*}. Let LL be a pp-adic field anabelomorphic to KK with an isomorphism α:GKGL\alpha:G_{K}\simeq G_{L}. Then there exists a Tate elliptic curve E/LE^{\prime}/L with Tate parameter qLq_{L} and an isomorphism of topological abelian groups

E(K)E(L),E(K)\simeq E^{\prime}(L),

given by the isomorphism α:GKGL\alpha:G_{K}\to G_{L}. The elliptic curve E/LE^{\prime}/L is given by Tate’s equation

y2+xy=x3+a4(qL)x+a6(qL).y^{2}+xy=x^{3}+a_{4}(q_{L})x+a_{6}(q_{L}).

Proof.

The anabelomorphism α:KL\alpha:K\leftrightsquigarrow L provides an isomorphism α:GKGL\alpha:G_{K}\simeq G_{L} which provides, by the third fundamental theorem of anabelomorphy 2.4.3, an isomorphism of topological groups α:KL\alpha:K^{*}\simeq L^{*}. Let qL=α(qK)q_{L}=\alpha(q_{K}). The map α\alpha preserves the valuation of qKq_{K} and hence |qL|<1|q_{L}|<1 and so by Tate’s Theorem one gets the Tate elliptic curve E/LE^{\prime}/L. The composite KLL/qLK^{*}\to L^{*}\to L^{*}/q_{L}^{\mathbb{Z}} provides the isomorphism of topological groups E(K)E(L)E(K)\simeq E^{\prime}(L). 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 KK be a pp-adic field and let A/KA/K be an abelian variety of dimension g1g\geq 1 given by a lattice ΛA(K)g=K××K\Lambda_{A}\subset(K^{*})^{g}=K^{*}\times\cdots\times K^{*} in a gg-dimensional torus given by KK. Let α:KL\alpha:K\leftrightsquigarrow L be an anabelomorphism of pp-adic fields. Then there exists an abelian variety A/LA^{\prime}/L and a topological isomorphism of groups A(K)A(L)A(K)\simeq A^{\prime}(L). If A/KA/K is polarized then so is A/LA^{\prime}/L.

Proof.

The lattice ΛK\Lambda_{K} provides a lattice ΛL\Lambda_{L} in L××LL^{*}\times\cdots\times L^{*} using the isomorphism K××KL××LK^{*}\times\cdots\times K^{*}\simeq L^{*}\times\cdots\times L^{*} induced by KLK^{*}\simeq L^{*} induced by our anabelomorphism α:KL\alpha:K\leftrightsquigarrow L. The rest is immediate from the Mumford-Tate uniformization theorem. If AA is polarized, then constructing a polarization on AA^{\prime} 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:

π1(A/K)π1(A/L),\pi_{1}(A/K)\simeq\pi_{1}(A^{\prime}/L),

in other words, A/KA/K and A/LA^{\prime}/L are anabelomorphic abelian varieties.

Proof.

Let g=dim(A)g=\dim(A). An étale cover of A/KA/K is an abelian variety with multiplicative reduction B/KB/K^{\prime} over some finite extension K/KK^{\prime}/K. The covering map provides an injective homomorphism of discrete subgroups ΛAΛB(K)g\Lambda_{A}\to\Lambda_{B}\subset(K^{{}^{\prime}*})^{g} corresponding to the étale covering BAB\to A. Since KLK\leftrightsquigarrow L, any finite extension KK^{\prime} of KK gives a finite extension L/LL^{\prime}/L, this correspondence is given as follows KK^{\prime} corresponds to an open subgroup HGKH\subset G_{K} and the isomorphism GKGLG_{K}\to G_{L} provides an open subgroup HH^{\prime} which is an isomorphic image of HH under this isomorphism and LL^{\prime} is the fixed field of HH^{\prime}. Hence one has, in particular, that KLK^{\prime}\leftrightsquigarrow L^{\prime}. Now construct an étale cover of AA^{\prime} over LL^{\prime} by transferring the data of the covering ΛAΛB\Lambda_{A}\hookrightarrow\Lambda_{B} (which is an inclusion of discrete subgroups of finite index) to (L)n(L)n(L^{*})^{n}\hookrightarrow(L^{{}^{\prime}*})^{n}. By Mumford’s construction this gives a covering BAB^{\prime}\to A^{\prime}. The correspondence B/KB/LB/K^{\prime}\longmapsto B^{\prime}/L^{\prime} provides the required correspondence between étale coverings of A/KA/K and étale coverings of A/LA^{\prime}/L. This argument can be reversed. Starting with a covering of AA^{\prime} one can arrive at a covering of AA. Hence the result follows.

§ 12.3  Anabelomorphy of group-schemes of type (p,p,,p)(p,p,\cdots,p) over pp-adic fields

Let KK be a pp-adic field and 𝒢/K\mathscr{G}/K be a commutative, finite flat group scheme of order prp^{r} and type (p,p,,p)(p,p,\cdots,p) over KK. Let LL be an anabelomorph of KK. Then the following shows that there is a commutative finite flat group scheme \mathscr{H} of type (p,p,,p)(p,p,\cdots,p) over LL which is obtained from 𝒢\mathscr{G}. By [Raynaud, 1974] the group scheme 𝒢\mathscr{G} is given by a system of equations

Xip=δiXi+1,δiK, for all i,i+1/r.X_{i}^{p}=\delta_{i}X_{i+1},\qquad\delta_{i}\in K^{*},\text{ for all }i,i+1\in{\mathbb{Z}}/r{\mathbb{Z}}.

Fix an anabelomorphism α:GLGK\alpha:G_{L}\to G_{K}. This induces isomorphism of topological groups LKL^{*}\to K^{*}. Let τiL\tau_{i}\in L^{*}, for all i/ri\in{\mathbb{Z}}/r{\mathbb{Z}} be the inverse image of δi\delta_{i} under this isomorphism. Then

Yip=τiYi+1 for all i,i+1/r,Y_{i}^{p}=\tau_{i}Y_{i+1}\text{ for all }i,i+1\in{\mathbb{Z}}/r{\mathbb{Z}},

provides a finite flat group scheme /L\mathscr{H}/L of type (p,p,,p)(p,p,\cdots,p). Conversely, starting with a group scheme of this type over LL, one can use an anabelomorphism between L,KL,K to construct a group scheme over KK. Thus one has

Theorem 12.3.1.

An anabelomorphism of fields L,KL,K sets up a bijection between commutative finite group flat schemes of type (p,p,,p)(p,p,\cdots,p) over LL and KK 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 K,KK,K^{\prime} are anabelomorphically connected along v1,,vn{v}_{1},\ldots,{v}_{n} and w1,,wn{w}_{1},\ldots,{w}_{n}, if there exist non-archimedean places v1,,vnv_{1},\ldots,v_{n} of KK (resp. non-archimedean places w1,,wnw_{1},\ldots,w_{n} of KK^{\prime}) and for each i=1,,ni=1,\ldots,n an anabelomorphism KviKwiK_{v_{i}}\leftrightsquigarrow K^{\prime}_{w_{i}} and for each ii the inclusion KKwiK^{\prime}\hookrightarrow K_{w_{i}}^{\prime} is dense. I will simply denote this by writing

(K,{v1,,vn})(K,{w1,,wn}),\left({K},\{v_{1},\ldots,v_{n}\}\right)\leftrightsquigarrow\left({K^{\prime}},\{w_{1},\ldots,w_{n}\}\right),

Example 13.1.2.

Here is a basic collection of examples. Let pp be an odd prime, let r1r\geq 1 be an integer. Let Kr=(ζpr,ppr)K_{r}={\mathbb{Q}}(\zeta_{p^{r}},\sqrt[p^{r}]{p}), Kr=(ζpr,1+ppr)K_{r}^{\prime}={\mathbb{Q}}(\zeta_{p^{r}},\sqrt[p^{r}]{1+p}). These are totally ramified at pp (see [Viviani, 2004]). Let 𝔭{\mathfrak{p}} (resp. 𝔭{\mathfrak{p}}^{\prime}) be the unique prime of KrK_{r} prime lying over pp in KrK_{r} (resp. the unique prime of KrK^{\prime}_{r} lying over pp in KrK^{\prime}_{r}). The completions of KrK_{r} (resp. KrK_{r}^{\prime}) with respect to these unique primes are Kr,𝔭=p(ζpr,ppr)K_{r,{\mathfrak{p}}}={\mathbb{Q}}_{p}(\zeta_{p^{r}},\sqrt[p^{r}]{p}) and Kr,𝔭=p(ζpr,ppr)K^{\prime}_{r,{\mathfrak{p}}^{\prime}}={\mathbb{Q}}_{p}(\zeta_{p^{r}},\sqrt[p^{r}]{p}) respectively. By Lemma 4.4 one has an isomorphism of the local Galois groups

Kr,𝔭Kr,𝔭.K_{r,{\mathfrak{p}}}\leftrightsquigarrow K^{\prime}_{r,{\mathfrak{p}}^{\prime}}.

For each r1r\geq 1, the pairs (Kr,{𝔭})(K_{r},\{{\mathfrak{p}}\}) and (Kr,{𝔭r})(K_{r}^{\prime},\{{\mathfrak{p}}_{r}\}) provide a basic example of an anabelomorphically connected pair of number fields (see 13.1.1). In particular, the number fields Kr=(ζpr,ppr),Kr=(ζpr,1+ppr)K_{r}={\mathbb{Q}}(\zeta_{p^{r}},\sqrt[p^{r}]{p}),K^{\prime}_{r}={\mathbb{Q}}(\zeta_{p^{r}},\sqrt[p^{r}]{1+p}) (and the unique primes 𝔭r,𝔭r{\mathfrak{p}}_{r},{\mathfrak{p}}_{r}^{\prime} be the primes lying over pp in Kr,KrK_{r},K^{\prime}_{r}) are anabelomorphically connected along 𝔭r{\mathfrak{p}}_{r} and 𝔭r{\mathfrak{p}}_{r}^{\prime}:

(Kr,{𝔭r})(Kr,{𝔭r}).\left({K_{r}},\{{\mathfrak{p}}_{r}\}\right)\leftrightsquigarrow\left({K^{\prime}_{r}},\{{\mathfrak{p}}^{\prime}_{r}\}\right).

Remark 13.1.3.

By the formulae for the discriminants of Kr,KrK_{r},K_{r}^{\prime} (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. \bullet

§ 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 MM is dense in a pp-adic field LL if there exists a place vv of MM such that the completion MvM_{v} of MM at vv is LL (i.e. Mv=LM_{v}=L).

I begin with the following easy lemma.

Lemma 13.2.1.

Let LL be pp-adic field. Then there exists a number field MLM\subset L which is dense in LL.

Proof.

This is a well-known consequence of Krasner’s Lemma (see [Koblitz, 1984]). Let L=p(x)L={\mathbb{Q}}_{p}(x) where pp is the residue characteristic of LL. Let fp[X]f\in{\mathbb{Q}}_{p}[X] be the minimal polynomial of xx. If f(X)[X]f(X)\in{\mathbb{Q}}[X] then xx is algebraic and clearly M=(x)M={\mathbb{Q}}(x) is the dense number field one seeks. If this is not the case then choose g(X)[X]g(X)\in{\mathbb{Q}}[X] sufficiently close to f(X)f(X) in p[X]{\mathbb{Q}}_{p}[X]. Then by Krasner’s Lemma (see loc. cit.) gg is irreducible and if x0x_{0} is a root of g(X)g(X) then p(x0)=p(x){\mathbb{Q}}_{p}(x_{0})={\mathbb{Q}}_{p}(x) and hence M=(x0)M={\mathbb{Q}}(x_{0}) is dense in LL.

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 KK be a number field and let vv be a non-archimedean place of KK. Let LL be a local field anabelomorphic to KvK_{v}. Then there exists a number field KK^{\prime} and non-archimedean place ww of KK^{\prime} such that

KwLKv.K^{\prime}_{w}\simeq L\leftrightsquigarrow K_{v}.

In particular, KwK^{\prime}_{w} is anabelomorphic to KvK_{v}. Equivalently (K,{v})(K,{w})\left({K},\{v\}\right)\leftrightsquigarrow\left({K^{\prime}},\{w\}\right).

Proof.

By Lemma 13.2.1, there exists a number field KLK^{\prime}\subset L dense in LL. Let ww be the place corresponding to the dense embedding KLK^{\prime}\hookrightarrow L (i.e. Kw=LK^{\prime}_{w}=L). Then KwLKvK^{\prime}_{w}\simeq L\leftrightsquigarrow K_{v} and hence KwKvK^{\prime}_{w}\leftrightsquigarrow K_{v} and hence (K,{v})(K,{w})\left({K},\{v\}\right)\leftrightsquigarrow\left({K^{\prime}},\{w\}\right). 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 p{\mathbb{Q}}_{p} for some (unspecified) prime pp. I say that an arbitrary, finite set of non-archimedean local fields {L1,,Ln}\{L_{1},\cdots,L_{n}\} (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 MM and for every ii, a dense inclusion MLiM\hookrightarrow L_{i} such that the induced valuations on MM are all inequivalent.

Lemma 13.2.3 (Potential Cohesivity Lemma).

For every finite set {L1,,Ln}\{L_{1},\cdots,L_{n}\} of non-archimedean local fields (not all distinct and not necessarily of the same residue characteristic) there exist finite extensions Li/LiL_{i}^{\prime}/L_{i} such that {L1,,Ln}\{L_{1}^{\prime},\cdots,L_{n}^{\prime}\} is a cohesive system of non-archimedean local fields.

Proof.

By Lemma 13.2.1 the result is true for n=1n=1 with L1=L1L_{1}^{\prime}=L_{1}. The general case will be proved by induction on nn. Suppose that the result has been established for the case of n1n-1 fields. So for every set L1,,Ln1L_{1},\ldots,L_{n-1} of non-archimedean fields there exists finite extensions L1,,Ln1L_{1}^{\prime},\ldots,L^{\prime}_{n-1} of non-archimedean fields and a number field MLiM\in L_{i}^{\prime} which is dense inclusion for i=1,,n1i=1,\ldots,n-1 and the valuations induced on MM are all inequivalent. Choose αM\alpha\in M such that (α)=M{\mathbb{Q}}(\alpha)=M.

Now suppose that pp is the residue characteristic of LnL_{n} and Ln=p(xn)L_{n}={\mathbb{Q}}_{p}(x_{n}). By Lemma 13.2.1 there exists a number field dense in LnL_{n}. By Krasner’s Lemma one can choose βLn\beta\in L_{n} to be algebraic and sufficiently close to xnx_{n} such that Ln=p(β)=p(xn)L_{n}={\mathbb{Q}}_{p}(\beta)={\mathbb{Q}}_{p}(x_{n}). Now consider the finite extensions Ln=Ln(α)L_{n}^{\prime}=L_{n}(\alpha) and Li′′=Li(β)L_{i}^{\prime\prime}=L_{i}^{\prime}(\beta) (if Ln(α)L_{n}(\alpha) is not a field then pick a direct factor of Ln(α)L_{n}\otimes{\mathbb{Q}}(\alpha) as this is a product of fields each of which is a finite extension of LnL_{n} equipped with an embedding of (α){\mathbb{Q}}(\alpha), and similarly for β\beta) for i=1,,n1i=1,\ldots,n-1. Then (α,β)Li′′{\mathbb{Q}}(\alpha,\beta)\subset L_{i}^{\prime\prime} for i=1,,n1i=1,\ldots,n-1 and (α,β)Ln{\mathbb{Q}}(\alpha,\beta)\subset L_{n}^{\prime}. Write Ln′′=LnL_{n}^{\prime\prime}=L_{n}^{\prime} (for symmetry of notation). Then one sees that there exists a common number field MM contained in all of Li′′L_{i}^{\prime\prime}. If MM is not dense in each of Li′′L_{i}^{\prime\prime} one can extend Li′′L_{i}^{\prime\prime} further to achieve density. Similarly if the induced valuations on MM are not all inequivalent, one can extend Li′′L_{i}^{\prime\prime} 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 n=2n=2. So the situation is that one has two non-archimedean fields L1,L2L_{1},L_{2} and a common number field MM contained in both of them. There are two possibilities: either residue characteristics of L1,L2L_{1},L_{2} are equal or they are not equal. First assume that the residue characteristics are equal (say equal to pp). Then L1,L2L_{1},L_{2} are both finite extensions of p{\mathbb{Q}}_{p} and so there exists a finite extension LL containing both of them as subfields. Pick such an LL. Then there is a number field MM^{\prime} dense in LL. Now choose a number field FF, with [F:]>1[F:{\mathbb{Q}}]>1, which is totally split at pp and such that M,FM^{\prime},F are linearly disjoint over {\mathbb{Q}}. Then let M′′=MFLM^{\prime\prime}=MF\hookrightarrow L and since FF is completely split there exist two primes v1v2v_{1}\neq v_{2} of M′′M^{\prime\prime} lying over pp such that Mv1′′=LM^{\prime\prime}_{v_{1}}=L and Mv2′′=LM^{\prime\prime}_{v_{2}}=L. Thus the system L1=L,L2=LL_{1}=L,L_{2}=L is now cohesive as M′′L1=LM^{\prime\prime}\hookrightarrow L_{1}=L and M′′L2=LM^{\prime\prime}\hookrightarrow L_{2}=L are dense inclusions corresponding to distinct primes of M′′M^{\prime\prime}.

Now assume L1,L2L_{1},L_{2} have distinct residue characteristics and MM is a number field contained in both of them. If v1v_{1} (resp. v2v_{2}) is the prime of MM corresponding to the inclusion ML1M\hookrightarrow L_{1} (resp. ML2M\hookrightarrow L_{2}), then Mv1L1M_{v_{1}}\hookrightarrow L_{1} and Mv2L2M_{v_{2}}\hookrightarrow L_{2} are finite extensions of non-archimedean fields. One proceeds by descending induction on [L1,Mv1],[L2,Mv2][L_{1},M_{v_{1}}],[L_{2},M_{v_{2}}]. By the primitive element theorem there exists an x1L1x_{1}\in L_{1} (resp. x2L2x_{2}\in L_{2}) such that L1=Mv1(x1)L_{1}=M_{v_{1}}(x_{1}) (resp. L2=Mv2(x2)L_{2}=M_{v_{2}}(x_{2})). Choose an irreducible polynomial fM[X]f\in M[X] which is sufficiently close to the minimal polynomials of x1x_{1} (resp. x2x_{2}) in L1[X]L_{1}[X] and L2[X]L_{2}[X] respectively. Then ff has a root in both L1,L2L_{1},L_{2} (by Krasner’s Lemma). The field M=M[X]/(f)M^{\prime}=M[X]/(f) embeds in both L1,L2L_{1},L_{2} and if v1v_{1}^{\prime} (resp. v2v_{2}^{\prime}) is the prime lying over v1v_{1} (resp. v2v_{2}) corresponding to the inclusion ML1M^{\prime}\hookrightarrow L_{1} and ML2M^{\prime}\hookrightarrow L_{2} are dense inclusions of MM^{\prime} in Mv1L1M^{\prime}_{v_{1}}\subset L_{1} (resp. MM in Mv2L2M^{\prime}_{v_{2}}\hookrightarrow L_{2}) and [L1,Mv1]<[L1,Mv1][L_{1},M^{\prime}_{v_{1}^{\prime}}]<[L_{1},M_{v_{1}}] and similarly for L2L_{2}. Thus by enlarging MM 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 KK be a number field. Let v1,,vn{v}_{1},\ldots,{v}_{n} be a finite set of non-archimedean places of KK. Let αi:KviLi\alpha_{i}:K_{v_{i}}\leftrightsquigarrow L_{i} be arbitrary anabelomorphisms with non-archimedean local fields L1,,LnL_{1},\ldots,L_{n}. Then there exist

  1. (1)

    finite extensions Li/LiL_{i}^{\prime}/L_{i} (for all i) and a dense embedding of a number field MLiM\subset L_{i}^{\prime} and places w1,,wn{w}_{1},\ldots,{w}_{n} of MM induced by the embeddings MLiM^{\prime}\hookrightarrow L_{i}^{\prime} (i.e. the collection {Li}\{L_{i}^{\prime}\} of non-archimedean fields is cohesive) and

  2. (2)

    a finite extension K/KK^{\prime}/K and places u1,,un{u}_{1},\ldots,{u}_{n} of KK^{\prime} lying over the places viv_{i} of KK (for all ii) together with anabelomorphisms KuiLiK^{\prime}_{u_{i}}\leftrightsquigarrow L_{i}^{\prime}.

  3. (3)

    Equivalently (K,{u1,,un})(M,{w1,,wn})\left({K^{\prime}},\{{u}_{1},\ldots,{u}_{n}\}\right)\leftrightsquigarrow\left({M^{\prime}},\{{w}_{1},\ldots,{w}_{n}\}\right) and ui|viu_{i}|v_{i} for all i=1,,ni=1,\ldots,n.

In particular, given any number field KK and a collection of non-archimedean places of KK, there exists a finite extension K/KK^{\prime}/K and a number field MM^{\prime} which is anabelomorphically connected to KK^{\prime} along some place of KK^{\prime} lying over each of places v1,,vn{v}_{1},\ldots,{v}_{n} of KK.

Proof.

By the Cohesivity Lemma (Lemma 13.2.3) one can replace L1,,LnL_{1},\ldots,L_{n} by a cohesive collection L1,,LnL_{1}^{\prime},\ldots,L_{n}^{\prime} with Li/LiL_{i}^{\prime}/L_{i} finite extensions and a number field MLiM^{\prime}\subset L_{i}^{\prime} dense in each LiL_{i}^{\prime} such that the induced valuations on MM^{\prime} are all inequivalent. The finite extensions Li/LiL_{i}^{\prime}/L_{i} provide open subgroups HiGLiH_{i}^{\prime}\subset G_{L_{i}} of GLiG_{L_{i}}. Since one has anabelomorphisms αi:KviLi\alpha_{i}:K_{v_{i}}\leftrightsquigarrow L_{i}, let Hi=α1(Hi)H_{i}=\alpha^{-1}(H_{i}^{\prime}) be the inverse image of HiH_{i}^{\prime} in GviG_{v_{i}}. By continuity of αi\alpha_{i}, HiH_{i}^{\prime} are open subgroups of GviG_{v_{i}}. Let GGKG^{\prime}\subset G_{K} be the open subgroup of GKG_{K} generated by the decomposition groups of all primes except v1,,vnv_{1},\ldots,v_{n} and the open subgroups HiH_{i} for i=1,ni=1,\ldots n. Let KK^{\prime} be the fixed field of GG^{\prime} (in our fixed algebraic closure of KK). Let uiu_{i} be the unique place of KK^{\prime} lying over the viv_{i} such that GKuiHiG_{K^{\prime}_{u_{i}}}\simeq H_{i}. Then by construction

GKuiHiHiGLiGMwiG_{K^{\prime}_{u_{i}}}\simeq H_{i}\simeq H^{\prime}_{i}\simeq G_{L_{i}^{\prime}}\simeq G_{M_{w_{i}}}

and hence one has established that

(K,{u1,,un})(M,{v1,,vn}).\left({K^{\prime}},\{{u}_{1},\ldots,{u}_{n}\}\right)\leftrightsquigarrow\left({M^{\prime}},\{{v}_{1},\ldots,{v}_{n}\}\right).

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 LL be a pp-adic field. Then there exist infinitely many number fields MM with a dense embedding MLM\hookrightarrow L.

Proof.

This is easy to prove and is left as an exercise!

Theorem 13.2.6.

Let KK be a number field and let vv be a non-archimedean place of KK. Then there exist infinitely many anabelomorphically connected number fields (K,{v})(K,{w})\left({K},\{v\}\right)\leftrightsquigarrow\left({K^{\prime}},\{w\}\right). If K𝔭LK_{\mathfrak{p}}\leftrightsquigarrow L is a strict anabelomorphism then (K,{𝔭})(K,{𝔮})\left({K},\{{\mathfrak{p}}\}\right)\leftrightsquigarrow\left({K^{\prime}},\{\mathfrak{q}\}\right) are strictly anabelomorphically connected fields.

Proof.

By Lemma 13.2.5 there exist infinitely many number fields KK^{\prime} with a dense embedding KLK^{\prime}\hookrightarrow L.

Let KK^{\prime} be a number field which is dense in LL and let 𝔮\mathfrak{q} be the prime of KK^{\prime} corresponding to the embedding KLK^{\prime}\hookrightarrow L. Then one has anabelomorphically connected fields (K,{𝔭})(K,{𝔮})\left({K},\{{\mathfrak{p}}\}\right)\leftrightsquigarrow\left({K^{\prime}},\{\mathfrak{q}\}\right).

Theorem 13.2.7.

Let KK be a number field and let 𝔭{\mathfrak{p}} be a prime of KK lying over pp. Then there exist infinitely many anabelomorphically connected fields (K,{𝔭})(M,{𝔮})\left({K},\{{\mathfrak{p}}\}\right)\leftrightsquigarrow\left({M},\{\mathfrak{q}\}\right) such that deg(M/)\deg(M/{\mathbb{Q}})\to\infty. If K𝔭K_{{\mathfrak{p}}} is strictly anabelomorphic to LL then (K,{𝔭})(M,{𝔮})\left({K},\{{\mathfrak{p}}\}\right)\leftrightsquigarrow\left({M},\{\mathfrak{q}\}\right) is a strict anabelomorphic connectivity.

Proof.

Let us suppose that there is a anabelomorphically connected number field (with (K,{𝔭})(M,{𝔮})\left({K},\{{\mathfrak{p}}\}\right)\leftrightsquigarrow\left({M},\{\mathfrak{q}\}\right)) with deg(M/)\deg(M/{\mathbb{Q}}) maximal among all such fields. Let pp be the prime lying below 𝔮\mathfrak{q} (and hence also 𝔭{\mathfrak{p}}) in {\mathbb{Z}}. Choose a quadratic field FF which is completely split at pp and which is also totally split at any prime ramifying in MM. Then FMF\cap M has no primes of ramification and hence by the Hermite-Minkowski Theorem, FM=F\cap M={\mathbb{Q}}. Let M=FMM^{\prime}=FM. Then by construction M/MM^{\prime}/M is totally split at 𝔮\mathfrak{q}. Let 𝔮\mathfrak{q}^{\prime} be a prime of MM^{\prime} lying over 𝔮\mathfrak{q} of MM. Then M𝔮M𝔮M^{\prime}_{\mathfrak{q}^{\prime}}\simeq M_{\mathfrak{q}} and so one has anabelomorphisms K𝔭M𝔮M𝔮K_{\mathfrak{p}}\leftrightsquigarrow M_{\mathfrak{q}}\leftrightsquigarrow M^{\prime}_{\mathfrak{q}^{\prime}} and hence (K,{𝔭})(M,{𝔮})\left({K},\{{\mathfrak{p}}\}\right)\leftrightsquigarrow\left({M^{\prime}},\{\mathfrak{q}^{\prime}\}\right) and deg(M)>deg(M)\deg(M^{\prime})>\deg(M) which contradicts the maximality of deg(M)\deg(M).

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

(K,{v1,,vn})(K,{w1,,wn})\left({K},\{{v}_{1},\ldots,{v}_{n}\}\right)\leftrightsquigarrow\left({K^{\prime}},\{{w}_{1},\ldots,{w}_{n}\}\right)

be a pair of anabelomorphically connected number fields. Then one has for all primes \ell (including pp) and for all ii, an isomorphism of {\mathbb{Q}}_{\ell}-vector spaces

ExtGvi1((0),(1))ExtGwi1((0),(1)).{\rm Ext}\,^{1}_{G_{v_{i}}}({\mathbb{Q}}_{\ell}(0),{\mathbb{Q}}_{\ell}(1))\simeq{\rm Ext}\,^{1}_{G_{w_{i}}}({\mathbb{Q}}_{\ell}(0),{\mathbb{Q}}_{\ell}(1)).

This theorem is immediate from the following Lemma.

Lemma 14.1.2.

Let KLK\leftrightsquigarrow L be two anabelomorphic pp-adic fields. Then one has an isomorphism of {\mathbb{Q}}_{\ell}-vector spaces

ExtGK1((0),(1))ExtGL1((0),(1)).{\rm Ext}\,^{1}_{G_{K}}({\mathbb{Q}}_{\ell}(0),{\mathbb{Q}}_{\ell}(1))\simeq{\rm Ext}\,^{1}_{G_{L}}({\mathbb{Q}}_{\ell}(0),{\mathbb{Q}}_{\ell}(1)).

Proof.

Let α:KL\alpha:K\leftrightsquigarrow L be an anabelomorphism. It is standard that one has

ExtGK1((0),(1))H1(GK,(1)){\rm Ext}\,^{1}_{G_{K}}({\mathbb{Q}}_{\ell}(0),{\mathbb{Q}}_{\ell}(1))\simeq H^{1}(G_{K},{\mathbb{Q}}_{\ell}(1))

(continuous cohomology group). By Kummer Theory one knows that H1(GK,(1))H^{1}(G_{K},{\mathbb{Q}}_{\ell}(1)) can be described as (proj limK/Kn)\left(\projlim K^{*}/K^{*\ell^{n}}\right)\otimes{\mathbb{Q}}_{\ell} and one has a similar description for GLG_{L}. Then one has isomorphisms of topological groups KLK^{*}\to L^{*} and hence also of subgroups (K)n(L)n(K^{*})^{\ell^{n}}\simeq(L^{*})^{\ell^{n}} compatible with their respective inclusions in KK^{*} (resp. LL^{*}). Hence one has isomorphism of groups

K(K)nL(L)n.\frac{K^{*}}{(K^{*})^{\ell^{n}}}\simeq\frac{L^{*}}{(L^{*})^{\ell^{n}}}.

This also compatible with projections to similar groups for n1\ell^{n-1}. Thus one has an isomorphism of the inverse limits and hence in particular, on tensoring with {\mathbb{Q}}_{\ell}.

Alternately one can simply invoke the fact that (1){\mathbb{Q}}_{\ell}(1) is an amphoric GKGLG_{K}\simeq G_{L} module. The two cohomologies depends only on the topology of GKGLG_{K}\simeq G_{L}. So the claim is obvious.

This proof leads to the following (which is useful in many applications)

Lemma 14.1.3 (Bootstrapping Lemma).

Let VV be an amphoric GKG_{K}-module (i.e. an abelian topological group or a topological p{\mathbb{Z}}_{p}-module with a continuous action of GKG_{K} which is determined by the anabelomorphism class of KK). Then Hi(GK,V)H^{i}(G_{K},V) is amphoric.

Proof.

The proof is clear: continuous GKG_{K}-cohomology is determined by the topology of GG and by the topological isomorphism class of VV. As VV 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 p{\mathbb{Q}}_{p} (for the log-shell see [Hoshi, 2021], [Dupuy and Hilado, 2020b]). Let KK be a pp-adic field. Let

Hf1(GK,p(1))H1(GK,p(1))H^{1}_{f}(G_{K},{\mathbb{Q}}_{p}(1))\subset H^{1}(G_{K},{\mathbb{Q}}_{p}(1))

be the (Fontaine) subspace of (ordinary) crystalline two dimensional GKG_{K}-representations in ExtGK1(p(0),p(1)){\rm Ext}\,^{1}_{G_{K}}({\mathbb{Q}}_{p}(0),{\mathbb{Q}}_{p}(1)).

Theorem 14.1.4.

Let KLK\leftrightsquigarrow L be a pair of anabelomorphic pp-adic fields. Then one has an isomorphism of p{\mathbb{Q}}_{p}-vector spaces

Hf1(GK,p(1))Hf1(GL,p(1)).H^{1}_{f}(G_{K},{\mathbb{Q}}_{p}(1))\simeq H_{f}^{1}({G_{L}},{\mathbb{Q}}_{p}(1)).

In other words the space Hf1(GK,p(1))H^{1}_{f}(G_{K},{\mathbb{Q}}_{p}(1)), of crystalline-ordinary two dimensional p{\mathbb{Q}}_{p}-representations of the form 0p(1)Vp(0)00\to{\mathbb{Q}}_{p}(1)\to V\to{\mathbb{Q}}_{p}(0)\to 0, of GKG_{K} is amphoric!

Remark 14.1.5.

For readers of [Mochizuki, 2012, 2013, 2015] and [Mochizuki, 2021a, b, c, d] let me remark that Hf1(GK,p(1))H^{1}_{f}(G_{K},{\mathbb{Q}}_{p}(1)) is the log-shell tensored with p{\mathbb{Q}}_{p} (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 p{\mathbb{Q}}_{p}-vector spaces

Hf1(GK,p(1))(limn𝒪K/𝒪Kpn)pUKp,H^{1}_{f}(G_{K},{\mathbb{Q}}_{p}(1))\simeq\left(\varprojlim_{n}{\mathscr{O}}_{K}^{*}/{\mathscr{O}}_{K}^{*p^{n}}\right)\otimes{\mathbb{Q}}_{p}\simeq U_{K}\otimes{\mathbb{Q}}_{p},

where UKU_{K} is the subgroup of 11-units of 𝒪K{\mathscr{O}}_{K}^{*}. \bullet

§ 14.2  Anabelomorphy and pp-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 (ϕ,N)(\phi,N) module is an admissible filtered (ϕ,N)(\phi,N) module” and proved by Fontaine and Colmez in [Colmez and Fontaine, 2000]. The proof proceeds by changing the Hodge filtration on a filtered (ϕ,N)(\phi,N)-module.

This should be viewed as an example of anabelomorphy but carried out on the pp-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 pp-adic Hodge filtration is considered mobile while other structures remain fixed. This allows one to keep the pp-adic field KK fixed.

Let me remark that by Theorem 8.1 one knows that the 𝔏\mathfrak{L}-invariant of an elliptic curve over a pp-adic field is unamphoric together with the fact that 𝔏\mathfrak{L}-invariant is related to the filtration of the (ϕ,N)(\phi,N)-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 GKG_{K}-module VV lives in the KK-vector space Dst(V)D_{st}(V), while the Hodge filtration for the GLG_{L}-module VV lives in an LL-vector space.

As Mochizuki noted in his e-mail to me “it remains a significant challenge to find containers where the KK-vector space DdR(ρ,V)D_{dR}(\rho,V) and LL-vector space DdR(ρα,V)D_{dR}(\rho\circ\alpha,V) 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 KK be a pp-adic field and let α:LK\alpha:L\leftrightsquigarrow K be an anabelomorphism of pp-adic fields. Consider ρ:GKGL(V)\rho:G_{K}\to{\rm GL}(V) of GKG_{K}. Suppose that VV is a de Rham representation of GKG_{K} in the sense of [Fontaine, 1994a]. As was proved in [Hoshi, 2013] ρα:GLGL(V)\rho\circ\alpha:G_{L}\to{\rm GL}(V) need not be de Rham. Suppose VV is ordinary. Then by [Perrin-Riou, 1994], VV is then semi-stable and hence also de Rham. By Theorem 6.2 one deduces that the GLG_{L}-representation ρα:GLGL(V)\rho\circ\alpha:G_{L}\to{\rm GL}(V) is also ordinary and hence also de Rham. Let me write DdR(ρ,V)D_{dR}(\rho,V) for the KK-vector space associated to the de Rham representation ρ:GKGL(V)\rho:G_{K}\to{\rm GL}(V) of GKG_{K} and write DdR(ρα,V)D_{dR}(\rho\circ\alpha,V) for the LL-vector space associated to the de Rham representation ρα:GLGL(V)\rho\circ\alpha:G_{L}\to{\rm GL}(V) of GLG_{L}.

Theorem 14.2.1.

Let KK be a pp-adic field, let α:LK\alpha:L\leftrightsquigarrow K be an anabelomorphism of pp-adic fields. Let ρ:GKGL(V)\rho:G_{K}\to{\rm GL}(V) be a de Rham representation of GKG_{K} such that ρα:GLGL(V)\rho\circ\alpha:G_{L}\to{\rm GL}(V) is also de Rham (this is the case for example if VV is ordinary). Then for all sufficiently large integers k>0k>0, there is a natural isomorphism of p{\mathbb{Q}}_{p}-vector spaces

DdR(ρ,V(k))DdR(ρα,V(k)).D_{dR}({\rho,V(k)})\simeq D_{dR}({\rho\circ\alpha,V(k)}).

Remark 14.2.2.

Note that the Hodge filtration on the KK-vector space DdR(ρ,V(k))D_{dR}(\rho,V(k)) is up to shifting, the filtration on the KK-vector space DdR(ρ,V)D_{dR}(\rho,V). However I do not know how to compare the Hodge filtrations on DdR(ρ,V(k))D_{dR}({\rho,V(k)}) and DdR(ρα,V(k))D_{dR}({\rho\circ\alpha,V(k)}). \bullet

Proof.

Let GLG_{L} act on VV through the isomorphism α\alpha. So VV is also a GLG_{L}-module. Then as GKGLG_{K}\simeq G_{L}, one has an isomorphism of p{\mathbb{Q}}_{p}-vector spaces (given by α\alpha):

H1(GK,V)H1(GL,V).H^{1}(G_{K},V)\simeq H^{1}(G_{L},V).

By a fundamental observation of [Bloch and Kato, 1990] there is a natural mapping, called the Bloch-Kato exponential,

expBK:DdR(ρ,V(k))H1(GK,V(k))\exp_{BK}:D_{dR}(\rho,V(k))\to H^{1}(G_{K},V(k))

which is an isomorphism for all sufficiently large k>0k>0. There is a similar isomorphism for LL since VV is also a de Rham representation of GLG_{L} through α\alpha. Now putting all this together the isomorphism in the theorem is obvious.

Corollary 14.2.3.

Let KK be a pp-adic field. Let ρ:GKGL(V)\rho:G_{K}\to{\rm GL}(V) be a pp-adic representation of GKG_{K}. Let VV be an ordinary Galois representation of GKG_{K}. Then for all sufficiently large kk, DdR(ρ,V(k))D_{dR}(\rho,V(k)) is an amphoric p{\mathbb{Q}}_{p}-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 GLn{\rm GL}_{n} though the main result proved here is for GL2{\rm GL}_{2}. The representations in this section will be smooth, complex valued representations of GLn(K){\rm GL}_{n}(K). There is an automorphic analog of the Ordinary Synchronization Theorem (Theorem 14.1.1) which says that one can use an anabelomorphism KLK\leftrightsquigarrow L to synchronize automorphic representations of GLn(K){\rm GL}_{n}(K) and GLn(L){\rm GL}_{n}(L). Note that topological groups GLn(K){\rm GL}_{n}(K) and GLn(L){\rm GL}_{n}(L) are not topologically homeomorphic (except for n=1n=1). I prove the automorphic synchronization theorem for principal series for GLn(K){\rm GL}_{n}(K) for any n1n\geq 1 and also for all irreducible admissible representations of GL2(K){\rm GL_{2}}(K) for any odd prime pp.

§ 15.1  Anabelomorphisms and Weil-Deligne Groups

The following two lemmas will be used in the subsequent discussion.

Lemma 15.1.1.

Let KK be a pp-adic field. Let qq be the cardinality of the residue field of KK. Then

  1. (1)

    The homomorphism ordK:K\mathop{\rm ord}\nolimits_{K}:K^{*}\to{\mathbb{Z}} given by xordK(x)x\longmapsto\mathop{\rm ord}\nolimits_{K}(x) is amphoric.

  2. (2)

    the homomorphism :K\left\|-\right\|:K^{*}\to{\mathbb{R}}^{*} defined by x=qordK(x)\left\|x\right\|=q^{-\mathop{\rm ord}\nolimits_{K}(x)} is amphoric.

Proof.

By [Jarden and Ritter, 1979] qq is amphoric. It is clear that the second assertion follows from the first. So it is sufficient to prove the first assertion. This is done in [Hoshi, 2021, Proposition 2.2].

Lemma 15.1.2.

Let KK be a pp-adic field and let α:KL\alpha:K\leftrightsquigarrow L be an anabelomorphism. Let WKW_{K} (resp. WLW_{L}) be the Weil group of KK (resp. LL) and let WKW_{K}^{\prime} (resp. WLW_{L}^{\prime}) be the Weil-Deligne group of KK (resp. LL). Then one has topological isomorphisms

  1. (1)

    WKWLW_{K}\simeq W_{L}, and

  2. (2)

    WKWLW_{K}^{\prime}\simeq W_{L}^{\prime}

which maps Frobenius element of WKW_{K} to WLW_{L} (and resp. for Weil-Deligne groups).

Proof.

The anabelomorphism α:KL\alpha:K\leftrightsquigarrow L gives an isomorphism α:GKGL\alpha:G_{K}\to G_{L}. The cardinality qq of the residue field of KK is amphoric (see [Hoshi, 2021]). Let 𝔽q{\mathbb{F}_{q}} be the residue field of KK (and hence of LL). Let FrobKGK{\rm Frob}_{K}\in G_{K} be a Frobenius element for KK and let FrobL=α(FrobK){\rm Frob}_{L}=\alpha({\rm Frob}_{K}) be the Frobenius element of LL corresponding to the Frobenius element of GKG_{K}. Then WKW_{K} is the fiber-product of the two arrows

FrobK\textstyle{{\rm Frob}_{K}^{{\mathbb{Z}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}GK\textstyle{G_{K}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Gal(𝔽¯q/𝔽q).\textstyle{{\rm Gal}(\bar{\mathbb{F}}_{q}/{\mathbb{F}_{q}}).}

Since GKGLG_{K}\simeq G_{L} it is now clear that WKWLW_{K}\simeq W_{L} and this preserves Frobenius elements (by Theorem 11.1). The assertion for Weil-Deligne groups is immediate from this and by the existence of :K\left\|-\right\|:K^{*}\to{\mathbb{R}}^{*} given by the previous lemma and the definition of the Weil-Deligne group.

§ 15.2  Anabelomorphic Synchronization of Principal Representations

Assume that K,LK,L are pp-adic fields and α:KL\alpha:K\leftrightsquigarrow L is an anabelomorphism. Let me first show how to setup a bijective correspondence between principal series representations of GLn(K){\rm GL}_{n}(K) and GLn(L){\rm GL}_{n}(L).

Let me begin with the n=1n=1 case. In this case GL1(K)=K{\rm GL}_{1}(K)=K^{*} and is α:LK\alpha:L\leftrightsquigarrow K is an anabelomorphism then α\alpha provides an isomorphism α:LK\alpha:L^{*}\to K^{*}. Hence any character χ:GL1(K)\chi:{\rm GL}_{1}(K)\to{\mathbb{C}}^{*} provides a character χα:L\chi\circ\alpha:L^{*}\to{\mathbb{C}}^{*}, and conversely, every character of LL^{*} determines a unique character of KK^{*}. Thus one obtains a bijection between admissible GL1(K){\rm GL}_{1}(K) representations and admissible GL1(L){\rm GL}_{1}(L) representations which is given by χχα\chi\longmapsto\chi\circ\alpha. The local Langlands correspondence sets up a bijection between admissible representations of GL1(K){\rm GL}_{1}(K) and one dimensional representations of the Weil-Deligne group with N=0N=0. Hence one obtains a correspondence between representations of the Weil group WKW_{K} and the Weil group WLW_{L} of the appropriate sort.

Since the local Langlands Correspondence match LL-functions on either side and on the Galois side and as I have already established (Theorem 11.2) that local LL-functions on the Galois side are amphoric, so it follows that automorphic LL-functions are amphoric. Since conductors of characters are unamphoric (see Theorem 9.1), it follows that under anabelomorphy conductors are unamphoric. Moreover ε\varepsilon-factors require a choice of additive character and hence neither the conductor nor the ε\varepsilon-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 KK be a pp-adic field and let α:LK\alpha:L\leftrightsquigarrow K be an anabelomorphism of pp-adic fields. Then χχα\chi\longmapsto\chi\circ\alpha sets up a bijection between admissible representations of GL1(K){\rm GL}_{1}(K) and admissible representations of GL1(L){\rm GL}_{1}(L). This correspondence is compatible with the local Langlands correspondence on either side. LL-functions of irreducible admissible representations are amphoric. The conductor and ε\varepsilon-factors are unamphoric.

Now let me discuss the GLn(K){\rm GL}_{n}(K) for n2n\geq 2. The datum required to give a principal series representations of GLn(K){\rm GL}_{n}(K) consists of an nn-tuple of continuous characters (χ1,,χn)(\chi_{1},\ldots,\chi_{n}) of KK^{*} with values in {\mathbb{C}}^{*}. The associated principal series representation is denoted by π(χ1,,χn)\pi(\chi_{1},\ldots,\chi_{n}) 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 α:KL\alpha:K\leftrightsquigarrow L be an anabelomorphism of pp-adic fields. Then there is a natural bijection between principal series representations of GLn(K){\rm GL}_{n}(K) and principal series representations of GLn(L){\rm GL}_{n}(L) which is given by

π(χ1,,χn)π(χ1α,,χnα).\pi(\chi_{1},\ldots,\chi_{n})\longmapsto\pi(\chi_{1}\circ\alpha,\ldots,\chi_{n}\circ\alpha).

This correspondence takes irreducible principal series representations to irreducible principal series representations.

Proof.

The correspondence (χ1,,χn)(χ1α,,χnα)(\chi_{1},\ldots,\chi_{n})\longmapsto(\chi_{1}\circ\alpha,\ldots,\chi_{n}\circ\alpha) sets up a bijection between nn-tuples of continuous characters of KK^{*}\to{\mathbb{C}}^{*} and LL^{*}\to{\mathbb{C}}^{*}. Every principal series representation π\pi of GLn(K){\rm GL}_{n}(K) is of the form π=π(χ1,,χn)\pi=\pi(\chi_{1},\ldots,\chi_{n}) (similarly for GLn(L){\rm GL}_{n}(L)) 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 χi×χj=±1\chi_{i}\times\chi_{j}=\left\|-\right\|^{\pm 1} then so is χiαχjα=±1α\chi_{i}\circ\alpha\cdot\chi_{j}\circ\alpha=\left\|-\right\|^{\pm 1}\circ\alpha. So under this correspondence an irreducible representation π\pi is mapped to an irreducible representation.

§ 15.3  Anabelomorphic Synchronization of Supercuspidal representations for pp odd, n=2n=2

Now suppose n=2n=2 and p3p\geq 3 (i.e. pp is an odd prime). Then one knows that every supercuspidal representation π\pi of GL2(K){\rm GL_{2}}(K) arise, up to twisting by one dimensional characters, by base change π=BC(K1/K,χ)\pi=BC(K_{1}/K,\chi) where K1KK_{1}\supseteq K is a quadratic extension, χ:K1\chi:K_{1}^{*}\to{\mathbb{C}}^{*} is a character such that if τGal(K1/K)\tau\in{\rm Gal}(K_{1}/K) is the unique non-trivial element then χτχ\chi^{\tau}\neq\chi.

Now suppose α:LK\alpha:L\leftrightsquigarrow K. Then there exists a unique quadratic field L1/LL_{1}/L such that K1L1K_{1}\leftrightsquigarrow L_{1} and Gal(K¯/K1)GK{\rm Gal}(\bar{K}/K_{1})\subset G_{K} is the open subgroup of index two corresponding to K1/KK_{1}/K and GL1GLG_{L_{1}}\subseteq G_{L} is the corresponding open subgroup under α\alpha. A character χ:K1\chi:K_{1}^{*}\to{\mathbb{C}}^{*} provides a character L1L_{1}^{*}\to{\mathbb{C}}^{*} by composing with α:L1K1\alpha:L_{1}^{*}\to K_{1}^{*} and if τ:Gal(L1/L)\tau^{\prime}:{\rm Gal}(L_{1}/L) is the unique non-trivial element then evidently (χα)τχα(\chi\circ\alpha)^{\tau^{\prime}}\neq\chi\circ\alpha. Hence one obtains a supercuspidal representation π=BC(L1/L,χ)\pi^{\prime}=BC(L_{1}/L,\chi^{\prime}) where χ=χα\chi^{\prime}=\chi\circ\alpha. Thus, under anabelomorphy KLK\leftrightsquigarrow L, one has setup a correspondence

BC(K1/K,χ)BC(L1/L,χα).BC(K_{1}/K,\chi)\longmapsto BC(L_{1}/L,\chi\circ\alpha).

This procedure is symmetrical in LL and KK 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 GL2(K){\rm GL_{2}}(K) corresponding to the irreducible sub (resp. quotient) of π(1,)\pi(1,\left\|-\right\|) (resp. π(1,1)\pi(1,\left\|-\right\|^{-1})) is mapped to the corresponding object of GL2(L){\rm GL_{2}}(L).

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 GL2(K){\rm GL_{2}}(K) 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 pp be an odd prime and let LKL\leftrightsquigarrow K be an anabelomorphism of pp-adic fields. Then this anabelomorphism induces a bijection between irreducible admissible representations of GL2(K){\rm GL_{2}}(K) and GL2(L){\rm GL_{2}}(L). 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 WKW_{K}^{\prime} and irreducible, admissible representations of GL2(K){\rm GL_{2}}(K). The correspondence maps an irreducible principal series π(χ1,χ2)χ1χ2\pi(\chi_{1},\chi_{2})\longmapsto\chi_{1}\oplus\chi_{2} (χi\chi_{i} are considered as characters of the Weil-Deligne group via the Artin map). The Steinberg representation maps to the special representation sp(2)sp(2) of the Weil-Deligne group. A supercuspidal representation BC(K1/K,χ)BC(K_{1}/K,\chi) is mapped to the irreducible Weil-Deligne representation which is obtained by induction of χ\chi from WK1W_{K_{1}} to WKW_{K}.

Now given an anabelomorphism α:LK\alpha:L\leftrightsquigarrow K and a Weil-Deligne representation ρ:WKGL(V)\rho:W_{K}^{\prime}\to{\rm GL}(V), one can associate to it the Weil-Deligne representation ρα:WLGL(V)\rho\circ\alpha:W_{L}^{\prime}\to{\rm GL}(V). 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 pp be an odd prime and let LKL\leftrightsquigarrow K be anabelomorphic pp-adic fields. Then the local Langlands correspondence for GL2(K){\rm GL_{2}}(K) is compatible with the automorphic synchronization provided by Theorem 15.3.1. LL-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 p=2p=2, but their proofs will be a little more involved as there are many more representations to deal with. \bullet

Remark 15.3.4.

Let KK be a pp-adic field and let KLK\leftrightsquigarrow L be an anabelomorphism of pp-adic fields. Then by [Hoshi, 2021] the Brauer group Br(K)Br(K) is amphoric and hence given a division algebra DKD_{K} over KK, there exists a division algebra DLD_{L} which corresponds to DKD_{K}. It seems reasonable to expect that, at least for the case where DKD_{K} (and hence DLD_{L}) is a quaternion division algebra, there exists synchronization of admissible representations of DKD_{K}^{*} and DLD_{L}^{*} which is compatible with the above constructions. \bullet

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

U=1{0,1,},U={\mathbb{P}}^{1}-\{0,1,\infty\},

then for any field LL, U(L)=L{1}U(L)=L^{*}-\{1\} (see Theorem 16.3.3 for a general result). If we have an anabelomorphism LKL\leftrightsquigarrow K then one has an isomorphism LKL^{*}\to K^{*} of topological groups and hence an isomorphism topological spaces (with the respective pp-adic topologies)

U(L)=L{1}U(K)=K{1}.U(L)=L^{*}-\{1\}\simeq U(K)=K^{*}-\{1\}.
Theorem 16.1.1 (Anabelomorphic Density Theorem).

Let U=1{0,1,}U={\mathbb{P}}^{1}-\{0,1,\infty\}. Let KK be a number field. Let (K,{v1,,vn})(K,{w1,,wn})\left({K},\{{v}_{1},\ldots,{v}_{n}\}\right)\leftrightsquigarrow\left({K^{\prime}},\{{w}_{1},\ldots,{w}_{n}\}\right) be an anabelomorphically connected number field. Then the inclusion

U(K)iU(Kwi)iU(Kvi)U(K^{\prime})\subset\prod_{i}U(K^{\prime}_{w_{i}})\simeq\prod_{i}U(K_{v_{i}})

is dense for the pp-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 1{\mathbb{P}}^{1} 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

U=1{0,1,}1{0,1728,}.U={\mathbb{P}}^{1}-\{0,1,\infty\}\simeq{\mathbb{P}}^{1}-\{0,1728,\infty\}.

Then for any field LL, U(L)=L{1}U(L)=L^{*}-\{1\} and composite mapping

L{1}=U(L)1{0,1,}1{0,1728,}L^{*}-\{1\}=U(L)\to{\mathbb{P}}^{1}-\{0,1,\infty\}\simeq{\mathbb{P}}^{1}-\{0,1728,\infty\}

allows to view the open subset U(L)U(L) as jj-invariants of elliptic curves over LL except for j=0,1728j=0,1728. If we have an anabelomorphism LKL\leftrightsquigarrow K then one has an isomorphism of topological spaces (with the respective pp-adic topologies)

U(L)=L{1}U(K)=K{1}.U(L)=L^{*}-\{1\}\simeq U(K)=K^{*}-\{1\}.
Theorem 16.2.1 (Anabelomorphically Connectivity Theorem for Elliptic Curves).

Let

(K,{v1,,vn})(K,{w1,,wn})\left({K},\{{v}_{1},\ldots,{v}_{n}\}\right)\leftrightsquigarrow\left({K^{\prime}},\{{w}_{1},\ldots,{w}_{n}\}\right)

be an anabelomorphically connected pair of number fields. Let E/KE/K be an elliptic curve over a number field KK with jE0,1728j_{E}\neq 0,1728. Then there exists an elliptic curve E/KE^{\prime}/K^{\prime} such that

  1. (1)

    For all ii one has ordvi(jE)=ordwi(jE)\mathop{\rm ord}\nolimits_{v_{i}}(j_{E})=\mathop{\rm ord}\nolimits_{w_{i}}(j_{E^{\prime}}).

  2. (2)

    The jj-invariant jEj_{E^{\prime}} of EE^{\prime} is integral at all non-archimedean places of KK^{\prime} except w1,,wnw_{1},\cdots,w_{n}.

  3. (3)

    In particular, if EE has semi-stable reduction at viv_{i} then EE^{\prime} has semistable reduction at wiw_{i} and one has v(qE,vi)=v(qE,wi)v(q_{E,v_{i}})=v(q_{E^{\prime},w_{i}}) for the Tate parameters of EE at viv_{i} (resp. EE^{\prime} at wiw_{i}).

  4. (4)

    E/KE^{\prime}/K^{\prime} has potential good reduction at all non-archimedean primes of KK^{\prime} except at w1,,wnw_{1},\ldots,w_{n}.

Proof.

Let j=jEj=j_{E} be the jj-invariant of E/KE/K. At any place vv of semi-stable reduction one has v(j)<0v(j)<0. Let αi:KviKwi\alpha_{i}:K_{v_{i}}\leftrightsquigarrow K^{\prime}_{w_{i}} be the given anabelomorphisms. Let ji=αi(j)Kwij_{i}=\alpha_{i}(j)\in K_{w_{i}}^{{}^{\prime}*}. Then by the Theorem 16.1.1 one sees that

U(K)iU(Kvi)=iKvi{1}iU(Kwi)=iKwi{1}U(K^{\prime})\hookrightarrow\prod_{i}U(K_{v_{i}})=\prod_{i}K_{v_{i}}^{*}-\{1\}\simeq\prod_{i}U(K^{\prime}_{w_{i}})=\prod_{i}K_{w_{i}}^{{}^{\prime}*}-\{1\}

is dense. Hence there exists a jKj^{\prime}\in K^{\prime} which is sufficiently close to each of the jij_{i} and is ww-integral for all other non-archimedean valuations ww of KK^{\prime}.

By the well-known theorem of Tate [Silverman, 1985] there exists an elliptic curve E/KE^{\prime}/K^{\prime} with jj-invariant jj^{\prime}. By construction jE=jj_{E^{\prime}}=j^{\prime} is sufficiently close to jij_{i} for each ii and as E/KE/K has semi-stable reduction at each viv_{i} the valuation of jEj_{E} at each viv_{i} is negative. Moreover for other non-archimedean valuations ww of KK^{\prime}, jj^{\prime} is ww-integral by construction and so EE^{\prime} has potential good reduction at such ww.

As jj^{\prime} is sufficiently close to jij_{i} and the anabelomorphism KviKwiK_{v_{i}}\leftrightsquigarrow K^{\prime}_{w_{i}} preserves valuations on both the sides, the other assertions follow from the relationship between jj-invariants and Tate parameters at primes of semi-stable reduction.

A particularly useful consequence of this is the following:

Corollary 16.2.2.

Let E/FE/F 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 (K,{v1,,vn})(K,{v1,,vn})\left({K},\{{v}_{1},\ldots,{v}_{n}\}\right)\leftrightsquigarrow\left({K^{\prime}},\{{v^{\prime}}_{1},\ldots,{v^{\prime}}_{n}\}\right) such that

  1. (1)

    FKF\subseteq K is a finite extension

  2. (2)

    and EK=E×FKE_{K}=E\times_{F}K has semi-stable reduction,

  3. (3)

    v1,,vn{v}_{1},\ldots,{v}_{n} is the set of primes of semi-stable reduction of E/KE/K.

§ 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 X/KX/K I will mean that X(K)Sect(GK,π1(X/K))X(K)\hookrightarrow{\rm Sect}(G_{K},\pi_{1}(X/K)), and that there is some characterization of the image of this set with some reasonable functoriality in X/KX/K, and which depends only on the anabelomorphism class of X/KX/K. I will simply write Hom(GK,π1(X/K))Hom(G_{K},\pi_{1}(X/K)) to means the subset of sections Sect(GK,π1(X/K)){\rm Sect}(G_{K},\pi_{1}(X/K)) which are characterized as arising from X(K)X(K). 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 X/KX/K is an hyperbolic curve, then X(K)X(K) injects into the set of sections of π1(X/K)\pi_{1}(X/K) (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

(K,{v1,,vn})(K,{v1,1,,v1,r1;;vn,1,,vn,rn})\left({K},\{{v}_{1},\ldots,{v}_{n}\}\right)\leftrightsquigarrow\left({K^{\prime}},\{{v^{\prime}}_{1,1},\ldots,{v^{\prime}}_{1,r_{1}};\ldots;{v^{\prime}}_{{n},1},\ldots,{v^{\prime}}_{{n},r_{n}}\}\right)

and say that K,KK,K^{\prime} are anabelomorphically connected along non-archimedean places v1,,vn{v}_{1},\ldots,{v}_{n} of KK and non-archimedean places v1,1,,v1,r1;;vn,1,,vn,rn{v^{\prime}}_{1,1},\ldots,{v^{\prime}}_{1,r_{1}};\ldots;{v^{\prime}}_{{n},1},\ldots,{v^{\prime}}_{{n},r_{n}} of KK^{\prime} if

 for each i, one has KviKvi,j for all 1jri.\text{ for each }i,\text{ one has }K_{v_{i}}\leftrightsquigarrow K^{\prime}_{v^{\prime}_{i,j}}\text{ for all }1\leq j\leq r_{i}.

Clearly this extends the notion introduced previously by allowing several primes of KK^{\prime} lying over a place of KK.

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 X/KX/K and Y/LY/L are two geometrically connected, smooth, quasi-projective anabelomorphic varieties over pp-adic fields K,LK,L (i.e. π1(X/K)π1(Y/L)\pi_{1}(X/K)\simeq\pi_{1}(Y/L) is an isomorphism of topological groups and in particular, one has an anabelomorphism KLK\leftrightsquigarrow L). Assume that Grothendieck’s Section Conjecture holds for X/KX/K and Y/LY/L. Then one has a natural bijection of sets

X(K)Y(L),X(K)\simeq Y(L),

and in particular, if X(K)X(K)\neq\emptyset then Y(L)Y(L)\neq\emptyset.

Remark 16.3.2.

Note that in the context of the usual Moret-Bailly Theorem, the pp-adic fields K,LK,L are isomorphic so one may take Y=XY=X 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]. \bullet

Proof of Lemma 16.3.1.

Let me remark that if X/KX/K and Y/LY/L are two varieties over anabelomorphic fields KLK\leftrightsquigarrow L such that

π1(X/K)π1(Y/L) i.e. X/K,Y/L are anabelomorphic varieties\pi_{1}(X/K)\simeq\pi_{1}(Y/L)\text{ i.e. }X/K,Y/L\text{ are anabelomorphic varieties}

then Grothendieck’s section conjecture, which asserts that

X(K)Hom(GK,π(X/K))X(K)\to{\rm Hom}(G_{K},\pi(X/K))

is a bijection of sets, implies that there is a natural bijection of sets

X(K)Hom(GK,π1(X/K))Hom(GL,π1(Y/L))Y(L),X(K)\simeq{\rm Hom}(G_{K},\pi_{1}(X/K)){\lx@xy@svg{\hbox{\raise 0.0pt\hbox{\kern 3.0pt\hbox{\ignorespaces\ignorespaces\ignorespaces\hbox{\vtop{\kern 0.0pt\offinterlineskip\halign{\entry@#!@&&\entry@@#!@\cr&\crcr}}}\ignorespaces{\hbox{\kern-3.0pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise 0.0pt\hbox{$\textstyle{{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern 9.27777pt\raise 4.62312pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.62312pt\hbox{$\scriptstyle{\simeq}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern 27.0pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}{\hbox{\kern 27.0pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise 0.0pt\hbox{$\textstyle{}$}}}}}}}\ignorespaces}}}}\ignorespaces}{\rm Hom}(G_{L},\pi_{1}(Y/L))\simeq Y(L),

and now the last assertion is obvious.

Theorem 16.3.3.

Let KK be a number field and let v1,,vnv_{1},\ldots,v_{n} be a finite set of non-archimedean places of KK. Let (K,{v1,,vn})(K,{v1,,vn})\left({K},\{{v}_{1},\ldots,{v}_{n}\}\right)\leftrightsquigarrow\left({K^{\prime}},\{{v^{\prime}}_{1},\ldots,{v^{\prime}}_{n}\}\right) be anabelomorphically connected number field. Let X/KX/K (resp. Y/KY/K^{\prime}) be a geometrically connected, smooth, quasi-projective variety over KK (resp. KK^{\prime}). Suppose the following conditions are met:

  1. (1)

    X/KviX/K_{v_{i}} and Y/KviY/K^{\prime}_{v^{\prime}_{i}} are anabelomorphic varieties for 1in1\leq i\leq n, and

  2. (2)

    X(Kvi)X(K_{v_{i}})\neq\emptyset for all 1in1\leq i\leq n, and

  3. (3)

    Grothendieck’s section conjecture holds for each X/KviX/K_{v_{i}} and Y/KviY/K^{\prime}_{v^{\prime}_{i}}, and

  4. (4)

    suppose that one is given a non-empty open subset (in the viv_{i}-adic topology) UiX(Kvi)U_{i}\subseteq X(K_{v_{i}}).

Then there exists a finite extension K′′/KK^{\prime\prime}/K^{\prime} and places v′′1,1,,v′′1,r1;;v′′n,1,,v′′n,rn{v^{\prime\prime}}_{1,1},\ldots,{v^{\prime\prime}}_{1,r_{1}};\ldots;{v^{\prime\prime}}_{{n},1},\ldots,{v^{\prime\prime}}_{{n},r_{n}} of K′′K^{\prime\prime}

  1. (1)

    such that one has the anabelomorphic connectivity chain

    (K,{v1,,vn})(K,{v1,,vn})(K′′,{v′′1,1,,v′′1,r1;;v′′n,1,,v′′n,rn})\left({K},\{{v}_{1},\ldots,{v}_{n}\}\right)\leftrightsquigarrow\left({K^{\prime}},\{{v^{\prime}}_{1},\ldots,{v^{\prime}}_{n}\}\right)\leftrightsquigarrow({K^{\prime\prime}},\{{v^{\prime\prime}}_{1,1},\ldots,{v^{\prime\prime}}_{1,r_{1}};\ldots;{v^{\prime\prime}}_{{n},1},\ldots,{v^{\prime\prime}}_{{n},r_{n}}\})
  2. (2)

    and, for all corresponding primes in the above connectivity chain, bijections

    Y(Kvi,j′′′′)Y(Kvi)X(Kvi)Y(K^{\prime\prime}_{v^{\prime\prime}_{i,j}})\simeq Y(K^{\prime}_{v^{\prime}_{i}})\simeq X(K_{v_{i}})
  3. (3)

    and a point yY(K′′)y\in Y(K^{\prime\prime}) whose image in Y(Kvi,j′′)Y(Kvi)X(Kvi)Y(K^{\prime\prime}_{v_{i,j}})\simeq Y(K^{\prime}_{v_{i}})\simeq X(K_{v_{i}}) (for all i,ji,j) is contained in UiU_{i}.

Corollary 16.3.4.

Let K,KK,K^{\prime} 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. (1)

    X=n/KX={\mathbb{P}}^{n}/K and Y=n/KY={\mathbb{P}}^{n}/K^{\prime}, or

  2. (2)

    X=𝔸n/KX=\mathbb{A}^{n}/K and Y=𝔸n/KY=\mathbb{A}^{n}/K^{\prime}.

Proof of Corollary 16.3.4.

This is immediate from the fact that by Theorem 12.1.3 (for the case X=n/KX={\mathbb{P}}^{n}/K and Y=n/KY={\mathbb{P}}^{n}/K^{\prime}) and by Theorem 12.1.1 (for X=𝔸n/KX=\mathbb{A}^{n}/K and Y=𝔸n/KY=\mathbb{A}^{n}/K^{\prime}), 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 X/Kvi,Y/KviX/K_{v_{i}},Y/K^{\prime}_{v^{\prime}_{i}} are anabelomorphic, one has by Lemma 16.3.1, that for each ii, there is a natural bijection of sets

X(Kvi)Y(Kvi),X(K_{v_{i}})\simeq Y(K^{\prime}_{v^{\prime}_{i}}),

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 Y/KY/K^{\prime} with S={v1,,vn}S=\{v_{1}^{\prime},\ldots,v^{\prime}_{n}\} so there exists a finite extension K′′/KK^{\prime\prime}/K^{\prime} which is totally split at all the primes viv_{i}^{\prime} into primes vi,j′′v_{i,j}^{\prime\prime} with j=1,,ri=[K′′:K]j=1,\ldots,r_{i}=[K^{\prime\prime}:K^{\prime}] and hence for each ii one has isomorphisms KviKvi,j′′K^{\prime}_{v^{\prime}_{i}}\simeq K^{\prime\prime}_{v_{i,j}} (for all jj) and hence for each ii one has KviKvi,j′′K^{\prime}_{v^{\prime}_{i}}\leftrightsquigarrow K^{\prime\prime}_{v_{i,j}} (for all jj) 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 FF be a pp-adic field and let X/FX/F be a geometrically connected, smooth, quasi-projective variety over FF. Let KLK\leftrightsquigarrow L be two anabelomorphic pp-adic fields containing FF. Let XK=X×FKX_{K}=X\times_{F}K (resp. XL=X×FLX_{L}=X\times_{F}L). Then

  1. (1)

    There exists a finite extension K/KK^{\prime}/K and L/LL^{\prime}/L and an anabelomorphism KLK^{\prime}\leftrightsquigarrow L^{\prime} such that there is a natural bijection of sets XK(K)XL(L)X_{K^{\prime}}(K^{\prime})\to X_{L^{\prime}}(L^{\prime}).

  2. (2)

    There is a Zariski dense open subset UX/FU\subset X/F such that the induced mapping UK(K)UL(L)U_{K^{\prime}}(K^{\prime})\to U_{L^{\prime}}(L^{\prime}) 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 FF be a pp-adic field. Let X/FX/F be a geometrically connected, smooth, quasi-projective variety over FF. For any field extension F/FF^{\prime}/F, write XF=X×FFX_{F^{\prime}}=X\times_{F}{F^{\prime}} for the base change of XX to FF^{\prime}. Consider the set

[X,F]:={XF:[F:F]<},[X,F]:=\{X_{F^{\prime}}:[F^{\prime}:F]<\infty\},

of all possible base change of X/FX/F to finite extensions F/FF^{\prime}/F. I define an equivalence relation on the set [X,F][X,F] as follows.

Definition 17.1.1.

Let XK,XL[X,F]X_{K},X_{L}\in[X,F], then I will say that XK,XLX_{K},X_{L} are weakly anabelomorphic or basally anabelomorphic if and only if KLK\leftrightsquigarrow L.

The following is fundamental in understanding this:

Proposition 17.1.2.

Let X/FX/F be a geometrically connected, smooth, quasi-projective variety. Let XK,XL[X,F]X_{K},X_{L}\in[X,F].

  1. (1)

    Basal anabelomorphy is an equivalence relation \sim on [X,F][X,F].

  2. (2)

    If XKX_{K} and XLX_{L} are anabelomorphic then they are also basally anabelomorphic.

Proof.

The first assertion is immediate from the properties of anabelomorphic of pp-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. \bullet

Definition 17.1.4.

Let X/FX/F be a geometrically connected, smooth, quasi-projective variety over a pp-adic field FF. Let XK[X,F]X_{K}\in[X,F]. Then a quantity QXKQ_{X_{K}} or an algebraic structure AXKA_{X_{K}} or a property 𝒫\mathscr{P} associated to XKX_{K} 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 XKX_{K} in [X,F][X,F]. More precisely: if, XKXLX_{K}\sim\ {X_{L}} for a pair XK,XL[X,F]X_{K},X_{L}\in[X,F], then one has QXK=QXLQ_{X_{K}}=Q_{X_{L}} (resp. algebraic structure AXKAXLA_{X_{K}}\simeq A_{X_{L}}, and the property 𝒫\mathscr{P} holds for XKX_{K} if and only if 𝒫\mathscr{P} holds for XLX_{L}. If a quantity (resp. alg. structure, property) of X/KX/K 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 E/FE/F be an elliptic curve over a pp-adic field FF. Let EK,EL[E,F]E_{K},E_{L}\in[E,F] be basally anabelomorphic. Then

  1. (1)

    EKE_{K} has potential good reduction if and only if ELE_{L} has potential good reduction.

  2. (2)

    EKE_{K} has multiplicative reduction if and only if ELE_{L} has multiplicative reduction.

  3. (3)

    In general, the following quantities are weakly unamphoric.

    1. (a)

      The valuation of the discriminant of EKE_{K},

    2. (b)

      the exponent of conductor of EKE_{K}.

    3. (c)

      The Kodaira Symbol of EKE_{K}, and

    4. (d)

      the Tamagawa number of EKE_{K}.

  4. (4)

    In particular, the number of irreducible components of the special fiber of EKE_{K} is weakly unamphoric.

  5. (5)

    In particular, among all ELE_{L} with LKL\leftrightsquigarrow K, there is one LL for which ordL(ΔEL)\mathop{\rm ord}\nolimits_{L}(\Delta_{E_{L}}) 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 EKE_{K}, the Kodaira Symbol of EKE_{K}, and the Tamagawa number of EKE_{K} are all weakly amphoric. But I do not know how to prove this at the moment. \bullet

Remark 17.2.3.

The first two assertions of Theorem 17.2.1 are similar to [Mochizuki, 2012, Theorem 2.14(ii)]. \bullet

The following elementary consequence of Theorem 17.2.1 above and Theorem 2.4.7 is important:

Corollary 17.2.4.

Let E/FE/F be an elliptic curve over a pp-adic field FF. Let K/FK/F be a finite extension of FF. Let ΔK=ΔEK\Delta_{K}=\Delta_{E_{K}} be the minimal discriminant of E/KE/K. If E/KE/K has semi-stable reduction then let qKKq_{K}\in K^{*} be its Tate parameter. Then

  1. (1)

    {vL(ΔL):LK}\left\{v_{L}(\Delta_{L}):L\leftrightsquigarrow K\right\} is a finite set.

  2. (2)

    If EKE_{K} and ELE_{L} both have semi-stable reduction then {vL(log(qL)):LK}\left\{v_{L}(\log(q_{L})):L\leftrightsquigarrow K\right\} is a finite set.

In particular, under the above respective hypotheses, vK(ΔK),vK(log(qK))v_{K}(\Delta_{K}),v_{K}(\log(q_{K})) are bounded in the anabelomorphism class of KK.

Proof of Theorem 17.2.1.

Let jEj_{E} be the jj-invariant of EE. Then jE=jEK=jELj_{E}=j_{E_{K}}=j_{E_{L}} so write jj for this quantity. The important point in the proof is the determination of the order of jj in KK and LL 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] EKE_{K} has potential good reduction if and only if ordK(j)0\mathop{\rm ord}\nolimits_{K}(j)\geq 0. If j=0j=0 then jj-invariant is integral in both KK and LL (because it is already so in FF). So assume j0j\neq 0. Then ordF(j)0\mathop{\rm ord}\nolimits_{F}(j)\geq 0 if and only if ordK(j)0\mathop{\rm ord}\nolimits_{K}(j)\geq 0 and ordF(j)0\mathop{\rm ord}\nolimits_{F}(j)\geq 0 if and only if ordL(j)0\mathop{\rm ord}\nolimits_{L}(j)\geq 0. This proves the first assertion.

Using [Silverman, 1985, Chap VII, Prop. 5.1] one sees that EKE_{K} has multiplicative reduction if and only if vK(j)<0v_{K}(j)<0 and as vK(j)<0v_{K}(j)<0 if and only if vF(j)<0v_{F}(j)<0 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 EKE_{K} also encodes the number of irreducible components of the special fiber.

Let F=3(ζ9)F={\mathbb{Q}}_{3}(\zeta_{9}), let K=F(39)K=F(\sqrt[9]{3}) and L=F(29)L=F(\sqrt[9]{2}). Then KLK\leftrightsquigarrow L as it can be easily checked using [Viviani, 2004]. Both of these field have degree

[K:3]=[L:3]=54.[K:{\mathbb{Q}}_{3}]=[L:{\mathbb{Q}}_{3}]=54.

Let E:y2=x3+3x2+9E:y^{2}=x^{3}+3x^{2}+9 and EKE_{K} and ELE_{L} be as above. Let Δ\Delta be the minimal discriminant (over the relevant field), ff 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 EKE_{K} and ELE_{L}.

Curve v(Δ)v(\Delta) ff Kodaira Symbol Tamagawa Number
EKE_{K} 66 44 IVIV 11
ELE_{L} 66 2 I0I_{0}^{*} 44

Here is another example let E:y2=x3+3x2+3E:y^{2}=x^{3}+3x^{2}+3 and let K,L,EK,ELK,L,E_{K},E_{L} be as above. Then one has

Curve v(Δ)v(\Delta) ff Kodaira Symbol Tamagawa Number
EKE_{K} 1212 66 IVIV^{*} 33
ELE_{L} 1212 10 IVIV 11

§ 17.3  Additional numerical examples

Here are two more random examples where all the four quantities are simultaneously different..

Let

F=3(ζ9)K=F(39)L=F(49),F={\mathbb{Q}}_{3}(\zeta_{9})\quad K=F(\sqrt[9]{3})\quad L=F(\sqrt[9]{4}),

and let

E:y2=x3+(ζ95+8ζ94ζ93+ζ922ζ911)x+(408ζ956ζ94+201ζ93+37ζ9238ζ9+1348).E:y^{2}=x^{3}+(-\zeta_{9}^{5}+8\zeta_{9}^{4}-\zeta_{9}^{3}+\zeta_{9}^{2}-2\zeta_{9}-11)x+(-408\zeta_{9}^{5}-6\zeta_{9}^{4}+201\zeta_{9}^{3}+37\zeta_{9}^{2}-38\zeta_{9}+1348).
Curve v(Δ)v(\Delta) ff Kodaira Symbol Tamagawa Number
EKE_{K} 1515 1515 IIII 11
ELE_{L} 3939 3737 IVIV 33

For the same fields F,K,LF,K,L as in the previous example and for the curve

E:y2=x3+(2ζ95+ζ94+ζ93ζ92+2ζ9+5)x+(869ζ95+159ζ9447ζ93125ζ92+354ζ9+713).E:y^{2}=x^{3}+(-2\zeta_{9}^{5}+\zeta_{9}^{4}+\zeta_{9}^{3}-\zeta_{9}^{2}+2\zeta_{9}+5)x+(869\zeta_{9}^{5}+159\zeta_{9}^{4}-47\zeta_{9}^{3}-125\zeta_{9}^{2}+354\zeta_{9}+713).
Curve v(Δ)v(\Delta) ff Kodaira Symbol Tamagawa Number
EKE_{K} 1515 99 IVIV^{*} 33
ELE_{L} 2727 1919 IIII^{*} 11

Now let me provide two examples for p=2p=2. Again these are examples (taken from my data) where all the four quantities are simultaneously different. Let F=2(ζ16)F={\mathbb{Q}}_{2}(\zeta_{16}), K=F(ζ81,ζ831)K=F(\sqrt{\zeta_{8}-1},\sqrt{\zeta_{8}^{3}-1}), L=F(ζ414)L=F(\sqrt[4]{\zeta_{4}-1}) (these fields are considered in [Jarden and Ritter, 1979]). By loc. cit. KK and LL are anabelomorphic of degree n=32n=32 and totally ramified extensions of 2{\mathbb{Q}}_{2}.

E:y2=x3+(2ζ167+2ζ1662ζ165+2ζ1642ζ163+4ζ162+6ζ16+30)x+(32ζ16776ζ1668ζ165+32ζ16424ζ16320ζ162+16ζ1628).E:y^{2}=x^{3}+(-2\zeta_{16}^{7}+2\zeta_{16}^{6}-2\zeta_{16}^{5}+2\zeta_{16}^{4}-2\zeta_{16}^{3}+4\zeta_{16}^{2}+6\zeta_{16}+30)x\\ \qquad\qquad\qquad+(32\zeta_{16}^{7}-76\zeta_{16}^{6}-8\zeta_{16}^{5}+32\zeta_{16}^{4}-24\zeta_{16}^{3}-20\zeta_{16}^{2}+16\zeta_{16}-28).

Then

Curve v(Δ)v(\Delta) ff Kodaira Symbol Tamagawa Number
EKE_{K} 6464 6060 I0I_{0}^{*} 22
ELE_{L} 5252 5252 IIII 11
E:y2=x3+(2ζ1662ζ164+4ζ162+2)x+(28ζ16640ζ16524ζ164+8ζ163+16ζ16240ζ16+60).E:y^{2}=x^{3}+(-2\zeta_{16}^{6}-2\zeta_{16}^{4}+4\zeta_{16}^{2}+2)x\\ \qquad\qquad\qquad+(28\zeta_{16}^{6}-40\zeta_{16}^{5}-24\zeta_{16}^{4}+8\zeta_{16}^{3}+16\zeta_{16}^{2}-40\zeta_{16}+60).

Then

Curve v(Δ)v(\Delta) ff Kodaira Symbol Tamagawa Number
EKE_{K} 6868 6060 IIII^{*} 11
ELE_{L} 5656 5252 I0I_{0}^{*} 22

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 pp-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 EE has semistable reduction, then the four quantities considered above are weakly amphoric.

Table 17.3: Fragment of data on weak unamphoricity of numerical invariants of elliptic curves
E/(ζ9)E/{\mathbb{Q}}(\zeta_{9}) E/(ζ9,39)E/{\mathbb{Q}}(\zeta_{9},\sqrt[9]{3}) E/(ζ9,49)E/{\mathbb{Q}}(\zeta_{9},\sqrt[9]{4})
[a1,a2,a3,a4,a6][a_{1},a_{2},a_{3},a_{4},a_{6}] [vK(Δ),f, K. Sym,T. num.][v_{K}(\Delta),f,\text{ K. Sym},\text{T. num.}] [vL(Δ),f, K. Sym,T. num.][v_{L}(\Delta),f,\text{ K. Sym},\text{T. num.}]
[0,ζ95+ζ946ζ93ζ92+3ζ911,0,3ζ94ζ92+2ζ9418,ζ953ζ94ζ92ζ9+22][0,-\zeta_{9}^{5}+\zeta_{9}^{4}-6\zeta_{9}^{3}-\zeta_{9}^{2}+3\zeta_{9}-11,0,-3\zeta_{9}^{4}-\zeta_{9}^{2}+2\zeta_{9}-418,\zeta_{9}^{5}-3\zeta_{9}^{4}-\zeta_{9}^{2}-\zeta_{9}+22] [6,6,II,1][6,6,II,1] [18,10,II,1][18,10,II^{*},1]
[0,2ζ954ζ94+ζ93+8ζ92+2ζ9+204,0,4ζ95ζ944ζ93ζ92+ζ9+7,54ζ95+ζ94+ζ93ζ92106][0,2\zeta_{9}^{5}-4\zeta_{9}^{4}+\zeta_{9}^{3}+8\zeta_{9}^{2}+2\zeta_{9}+204,0,4\zeta_{9}^{5}-\zeta_{9}^{4}-4\zeta_{9}^{3}-\zeta_{9}^{2}+\zeta_{9}+7,-54\zeta_{9}^{5}+\zeta_{9}^{4}+\zeta_{9}^{3}-\zeta_{9}^{2}-106] [15,7,II,1][15,7,II^{*},1] [15,13,IV,1][15,13,IV,1]
[0,ζ95ζ93ζ92+ζ9+47,0,ζ954ζ9411ζ934ζ930,62ζ95ζ92+3ζ9+131][0,-\zeta_{9}^{5}-\zeta_{9}^{3}-\zeta_{9}^{2}+\zeta_{9}+47,0,\zeta_{9}^{5}-4\zeta_{9}^{4}-11\zeta_{9}^{3}-4\zeta_{9}-30,62\zeta_{9}^{5}-\zeta_{9}^{2}+3\zeta_{9}+131] [6,6,II,1][6,6,II,1] [18,10,II,1][18,10,II^{*},1]
[0,2ζ94ζ923ζ97,0,2ζ95ζ94ζ93ζ92+ζ911,ζ954ζ94+ζ932ζ922ζ912][0,2\zeta_{9}^{4}-\zeta_{9}^{2}-3\zeta_{9}-7,0,-2\zeta_{9}^{5}-\zeta_{9}^{4}-\zeta_{9}^{3}-\zeta_{9}^{2}+\zeta_{9}-11,\zeta_{9}^{5}-4\zeta_{9}^{4}+\zeta_{9}^{3}-2\zeta_{9}^{2}-2\zeta_{9}-12] [15,7,II,1][15,7,II^{*},1] [15,13,IV,3][15,13,IV,3]
[0,9ζ958ζ94ζ93+5ζ92+ζ921,0,2ζ954ζ936ζ92+23ζ9+33,2ζ95ζ93+28ζ92+3ζ9+53][0,-9\zeta_{9}^{5}-8\zeta_{9}^{4}-\zeta_{9}^{3}+5\zeta_{9}^{2}+\zeta_{9}-21,0,2\zeta_{9}^{5}-4\zeta_{9}^{3}-6\zeta_{9}^{2}+23\zeta_{9}+33,-2\zeta_{9}^{5}-\zeta_{9}^{3}+28\zeta_{9}^{2}+3\zeta_{9}+53] [6,6,II,1][6,6,II,1] [18,10,II,1][18,10,II^{*},1]
[0,ζ95+ζ94+ζ9311ζ9212ζ947,0,78ζ95ζ94ζ93+ζ92ζ9160,2ζ95ζ94ζ932ζ9210][0,-\zeta_{9}^{5}+\zeta_{9}^{4}+\zeta_{9}^{3}-11\zeta_{9}^{2}-12\zeta_{9}-47,0,-78\zeta_{9}^{5}-\zeta_{9}^{4}-\zeta_{9}^{3}+\zeta_{9}^{2}-\zeta_{9}-160,2\zeta_{9}^{5}-\zeta_{9}^{4}-\zeta_{9}^{3}-2\zeta_{9}^{2}-10] [12,4,II,1][12,4,II^{*},1] [0,0,I0,1][0,0,I_{0},1]
[0,ζ95+2ζ94+8ζ93ζ92+22,0,ζ947ζ93+ζ92ζ919,12ζ95+ζ942ζ932ζ92ζ9+31][0,-\zeta_{9}^{5}+2\zeta_{9}^{4}+8\zeta_{9}^{3}-\zeta_{9}^{2}+22,0,-\zeta_{9}^{4}-7\zeta_{9}^{3}+\zeta_{9}^{2}-\zeta_{9}-19,12\zeta_{9}^{5}+\zeta_{9}^{4}-2\zeta_{9}^{3}-2\zeta_{9}^{2}-\zeta_{9}+31] [12,4,II,1][12,4,II^{*},1] [0,0,I0,1][0,0,I_{0},1]
[0,62ζ952ζ94+2ζ93+4ζ92+4ζ996,0,7ζ94+ζ93+ζ923,ζ95ζ944ζ93+ζ92+ζ94][0,-62\zeta_{9}^{5}-2\zeta_{9}^{4}+2\zeta_{9}^{3}+4\zeta_{9}^{2}+4\zeta_{9}-96,0,7\zeta_{9}^{4}+\zeta_{9}^{3}+\zeta_{9}^{2}-3,\zeta_{9}^{5}-\zeta_{9}^{4}-4\zeta_{9}^{3}+\zeta_{9}^{2}+\zeta_{9}-4] [6,6,II,1][6,6,II,1] [18,10,II,1][18,10,II^{*},1]
[0,ζ9539ζ93ζ9281,0,ζ95+ζ94ζ93+ζ92ζ92,35ζ95+102ζ9419ζ9324ζ928ζ9+80][0,\zeta_{9}^{5}-39\zeta_{9}^{3}-\zeta_{9}^{2}-81,0,-\zeta_{9}^{5}+\zeta_{9}^{4}-\zeta_{9}^{3}+\zeta_{9}^{2}-\zeta_{9}-2,-35\zeta_{9}^{5}+102\zeta_{9}^{4}-19\zeta_{9}^{3}-24\zeta_{9}^{2}-8\zeta_{9}+80] [9,7,IV,3][9,7,IV,3] [21,13,II,1][21,13,II^{*},1]
[0,ζ95+3ζ94ζ926,0,ζ95+85ζ9434ζ92+2ζ9+108,6ζ9584ζ94+103ζ93+22ζ92119ζ9+63][0,\zeta_{9}^{5}+3\zeta_{9}^{4}-\zeta_{9}^{2}-6,0,\zeta_{9}^{5}+85\zeta_{9}^{4}-34\zeta_{9}^{2}+2\zeta_{9}+108,6\zeta_{9}^{5}-84\zeta_{9}^{4}+103\zeta_{9}^{3}+22\zeta_{9}^{2}-119\zeta_{9}+63] [9,7,IV,3][9,7,IV,3] [21,13,II,1][21,13,II^{*},1]
[0,3ζ95ζ94+ζ93ζ9287ζ9179,0,ζ95+ζ94+ζ93ζ92+3,225ζ95+39ζ94+276ζ93+1222ζ92+238ζ9+2215][0,3\zeta_{9}^{5}-\zeta_{9}^{4}+\zeta_{9}^{3}-\zeta_{9}^{2}-87\zeta_{9}-179,0,-\zeta_{9}^{5}+\zeta_{9}^{4}+\zeta_{9}^{3}-\zeta_{9}^{2}+3,225\zeta_{9}^{5}+39\zeta_{9}^{4}+276\zeta_{9}^{3}+1222\zeta_{9}^{2}+238\zeta_{9}+2215] [6,4,IV,3][6,4,IV,3] [6,4,IV,1][6,4,IV,1]
[0,ζ95+4ζ93+5ζ92+ζ9+24,0,14ζ94ζ93+5ζ92+3ζ9+54,48ζ95661ζ94+572ζ93+229ζ92721ζ9+122][0,-\zeta_{9}^{5}+4\zeta_{9}^{3}+5\zeta_{9}^{2}+\zeta_{9}+24,0,14\zeta_{9}^{4}-\zeta_{9}^{3}+5\zeta_{9}^{2}+3\zeta_{9}+54,48\zeta_{9}^{5}-661\zeta_{9}^{4}+572\zeta_{9}^{3}+229\zeta_{9}^{2}-721\zeta_{9}+122] [6,4,IV,3][6,4,IV,3] [6,2,I0,1][6,2,I_{0}^{*},1]
[0,ζ94+3ζ93ζ92+6ζ9+14,0,7ζ95+6ζ94+5ζ93+2ζ9218ζ9+1,13ζ95+6ζ945ζ935ζ92+6ζ91][0,-\zeta_{9}^{4}+3\zeta_{9}^{3}-\zeta_{9}^{2}+6\zeta_{9}+14,0,7\zeta_{9}^{5}+6\zeta_{9}^{4}+5\zeta_{9}^{3}+2\zeta_{9}^{2}-18\zeta_{9}+1,-13\zeta_{9}^{5}+6\zeta_{9}^{4}-5\zeta_{9}^{3}-5\zeta_{9}^{2}+6\zeta_{9}-1] [6,4,IV,1][6,4,IV,1] [6,2,I0,1][6,2,I_{0}^{*},1]
[0,2ζ95ζ946ζ93+2ζ92+ζ912,0,2ζ9518ζ94+5ζ93+ζ926ζ935,185ζ957ζ94+79ζ9379ζ92+86ζ9+198][0,-2\zeta_{9}^{5}-\zeta_{9}^{4}-6\zeta_{9}^{3}+2\zeta_{9}^{2}+\zeta_{9}-12,0,2\zeta_{9}^{5}-18\zeta_{9}^{4}+5\zeta_{9}^{3}+\zeta_{9}^{2}-6\zeta_{9}-35,185\zeta_{9}^{5}-7\zeta_{9}^{4}+79\zeta_{9}^{3}-79\zeta_{9}^{2}+86\zeta_{9}+198] [9,7,IV,3][9,7,IV,3] [21,13,II,1][21,13,II^{*},1]
[0,ζ944ζ9310ζ92297,0,ζ95ζ94ζ93+2ζ92+ζ9+10,3ζ95+174ζ948ζ92+58ζ9+841][0,-\zeta_{9}^{4}-4\zeta_{9}^{3}-10\zeta_{9}^{2}-297,0,\zeta_{9}^{5}-\zeta_{9}^{4}-\zeta_{9}^{3}+2\zeta_{9}^{2}+\zeta_{9}+10,-3\zeta_{9}^{5}+174\zeta_{9}^{4}-8\zeta_{9}^{2}+58\zeta_{9}+841] [12,6,IV,1][12,6,IV^{*},1] [12,10,IV,1][12,10,IV,1]
[0,2ζ95ζ94+ζ9329,0,2ζ95ζ93ζ929ζ920,631ζ95+260ζ94+52ζ9321ζ92+65ζ9+858][0,2\zeta_{9}^{5}-\zeta_{9}^{4}+\zeta_{9}^{3}-29,0,-2\zeta_{9}^{5}-\zeta_{9}^{3}-\zeta_{9}^{2}-9\zeta_{9}-20,631\zeta_{9}^{5}+260\zeta_{9}^{4}+52\zeta_{9}^{3}-21\zeta_{9}^{2}+65\zeta_{9}+858] [12,6,IV,1][12,6,IV^{*},1] [12,10,IV,1][12,10,IV,1]
[0,ζ954ζ94+ζ93+2ζ9+3,0,ζ959ζ94ζ93ζ924,14ζ9521ζ94+75ζ9321ζ92+10ζ9+28][0,\zeta_{9}^{5}-4\zeta_{9}^{4}+\zeta_{9}^{3}+2\zeta_{9}+3,0,-\zeta_{9}^{5}-9\zeta_{9}^{4}-\zeta_{9}^{3}-\zeta_{9}-24,-14\zeta_{9}^{5}-21\zeta_{9}^{4}+75\zeta_{9}^{3}-21\zeta_{9}^{2}+10\zeta_{9}+28] [6,4,IV,3][6,4,IV,3] [6,2,I0,1][6,2,I_{0}^{*},1]
[0,ζ95ζ943ζ92+6ζ9+2,0,3ζ95+ζ93+14ζ924ζ9+19,31ζ95+20ζ94+126ζ93+8ζ9243ζ9+304][0,-\zeta_{9}^{5}-\zeta_{9}^{4}-3\zeta_{9}^{2}+6\zeta_{9}+2,0,-3\zeta_{9}^{5}+\zeta_{9}^{3}+14\zeta_{9}^{2}-4\zeta_{9}+19,-31\zeta_{9}^{5}+20\zeta_{9}^{4}+126\zeta_{9}^{3}+8\zeta_{9}^{2}-43\zeta_{9}+304] [6,4,IV,3][6,4,IV,3] [6,2,I0,1][6,2,I_{0}^{*},1]
[0,2ζ9513ζ94ζ925ζ945,0,ζ942ζ93ζ923ζ911,837ζ95100ζ94123ζ9353ζ92+194ζ944][0,-2\zeta_{9}^{5}-13\zeta_{9}^{4}-\zeta_{9}^{2}-5\zeta_{9}-45,0,-\zeta_{9}^{4}-2\zeta_{9}^{3}-\zeta_{9}^{2}-3\zeta_{9}-11,-837\zeta_{9}^{5}-100\zeta_{9}^{4}-123\zeta_{9}^{3}-53\zeta_{9}^{2}+194\zeta_{9}-44] [6,4,IV,3][6,4,IV,3] [6,2,I0,4][6,2,I_{0}^{*},4]
Table 17.5: Fragment of data on weak amphoricity of invariants of semistable elliptic curves
E/(ζ9)E/{\mathbb{Q}}(\zeta_{9}) E/(ζ9,39)E/{\mathbb{Q}}(\zeta_{9},\sqrt[9]{3}) E/(ζ9,49)E/{\mathbb{Q}}(\zeta_{9},\sqrt[9]{4})
[a1,a2,a3,a4,a6][a_{1},a_{2},a_{3},a_{4},a_{6}] [vK(Δ),f, K. Sym,T. num.][v_{K}(\Delta),f,\text{ K. Sym},\text{T. num.}] [vL(Δ),f, K. Sym,T. num.][v_{L}(\Delta),f,\text{ K. Sym},\text{T. num.}]
[0,ζ95+ζ946ζ93ζ99,0,ζ95ζ94+8ζ92ζ9+12,ζ95+ζ92+1][0,\zeta_{9}^{5}+\zeta_{9}^{4}-6\zeta_{9}^{3}-\zeta_{9}-9,0,\zeta_{9}^{5}-\zeta_{9}^{4}+8\zeta_{9}^{2}-\zeta_{9}+12,\zeta_{9}^{5}+\zeta_{9}^{2}+1] [9,1,I9,9][9,1,I_{9},9] [9,1,I9,9][9,1,I_{9},9]
[0,2ζ952ζ94ζ93+ζ95,0,ζ94+ζ933ζ92+8ζ9+11,ζ95+ζ942ζ93+3ζ92ζ9+1][0,2\zeta_{9}^{5}-2\zeta_{9}^{4}-\zeta_{9}^{3}+\zeta_{9}-5,0,-\zeta_{9}^{4}+\zeta_{9}^{3}-3\zeta_{9}^{2}+8\zeta_{9}+11,\zeta_{9}^{5}+\zeta_{9}^{4}-2\zeta_{9}^{3}+3\zeta_{9}^{2}-\zeta_{9}+1] [18,1,I18,18][18,1,I_{18},18] [18,1,I18,18][18,1,I_{18},18]
[0,ζ95+ζ94+24ζ93+11ζ92+75,0,ζ95+3ζ94ζ92+ζ9+8,ζ953ζ94+ζ93+ζ922ζ91][0,\zeta_{9}^{5}+\zeta_{9}^{4}+24\zeta_{9}^{3}+11\zeta_{9}^{2}+75,0,-\zeta_{9}^{5}+3\zeta_{9}^{4}-\zeta_{9}^{2}+\zeta_{9}+8,\zeta_{9}^{5}-3\zeta_{9}^{4}+\zeta_{9}^{3}+\zeta_{9}^{2}-2\zeta_{9}-1] [18,1,I18,18][18,1,I_{18},18] [18,1,I18,18][18,1,I_{18},18]
[0,ζ95+2ζ94+ζ93+10ζ92+ζ9+31,0,ζ95+3ζ94ζ92ζ92,ζ954ζ937ζ923][0,\zeta_{9}^{5}+2\zeta_{9}^{4}+\zeta_{9}^{3}+10\zeta_{9}^{2}+\zeta_{9}+31,0,-\zeta_{9}^{5}+3\zeta_{9}^{4}-\zeta_{9}^{2}-\zeta_{9}-2,\zeta_{9}^{5}-4\zeta_{9}^{3}-7\zeta_{9}-23] [18,1,I18,18][18,1,I_{18},18] [18,1,I18,18][18,1,I_{18},18]
[0,8ζ95+8ζ94ζ92+ζ9+4,0,2ζ95+ζ935ζ922ζ910,3ζ95+ζ94ζ93ζ92+5ζ922][0,-8\zeta_{9}^{5}+8\zeta_{9}^{4}-\zeta_{9}^{2}+\zeta_{9}+4,0,2\zeta_{9}^{5}+\zeta_{9}^{3}-5\zeta_{9}^{2}-2\zeta_{9}-10,-3\zeta_{9}^{5}+\zeta_{9}^{4}-\zeta_{9}^{3}-\zeta_{9}^{2}+5\zeta_{9}-22] [9,1,I9,9][9,1,I_{9},9] [9,1,I9,9][9,1,I_{9},9]
[0,3ζ94+7ζ924ζ9+16,0,2ζ95+ζ94+8ζ93ζ92+21,ζ95+3ζ92ζ9+3][0,3\zeta_{9}^{4}+7\zeta_{9}^{2}-4\zeta_{9}+16,0,2\zeta_{9}^{5}+\zeta_{9}^{4}+8\zeta_{9}^{3}-\zeta_{9}^{2}+21,\zeta_{9}^{5}+3\zeta_{9}^{2}-\zeta_{9}+3] [9,1,I9,9][9,1,I_{9},9] [9,1,I9,9][9,1,I_{9},9]
[0,ζ957ζ94+2ζ922ζ912,0,ζ95ζ94+ζ93ζ9+4,ζ943ζ92+ζ9+3][0,-\zeta_{9}^{5}-7\zeta_{9}^{4}+2\zeta_{9}^{2}-2\zeta_{9}-12,0,\zeta_{9}^{5}-\zeta_{9}^{4}+\zeta_{9}^{3}-\zeta_{9}+4,-\zeta_{9}^{4}-3\zeta_{9}^{2}+\zeta_{9}+3] [9,1,I9,9][9,1,I_{9},9] [9,1,I9,9][9,1,I_{9},9]
[0,ζ95ζ946ζ93ζ92+17,0,3ζ94+ζ93+ζ92+11,2ζ95+ζ93ζ92+3ζ9+1][0,\zeta_{9}^{5}-\zeta_{9}^{4}-6\zeta_{9}^{3}-\zeta_{9}^{2}+17,0,3\zeta_{9}^{4}+\zeta_{9}^{3}+\zeta_{9}^{2}+11,2\zeta_{9}^{5}+\zeta_{9}^{3}-\zeta_{9}^{2}+3\zeta_{9}+1] [18,1,I18,18][18,1,I_{18},18] [18,1,I18,18][18,1,I_{18},18]
[0,ζ94+2ζ93ζ9210ζ99,0,ζ94+2ζ92+4,ζ9517ζ94ζ93+ζ92+2ζ934][0,\zeta_{9}^{4}+2\zeta_{9}^{3}-\zeta_{9}^{2}-10\zeta_{9}-9,0,\zeta_{9}^{4}+2\zeta_{9}^{2}+4,\zeta_{9}^{5}-17\zeta_{9}^{4}-\zeta_{9}^{3}+\zeta_{9}^{2}+2\zeta_{9}-34] [9,1,I9,9][9,1,I_{9},9] [9,1,I9,9][9,1,I_{9},9]
[0,ζ95+9ζ946ζ93+3ζ92+ζ9+17,0,ζ95274ζ94+ζ93+ζ92+2ζ9553,2ζ95+ζ94+6ζ934ζ92+22][0,\zeta_{9}^{5}+9\zeta_{9}^{4}-6\zeta_{9}^{3}+3\zeta_{9}^{2}+\zeta_{9}+17,0,-\zeta_{9}^{5}-274\zeta_{9}^{4}+\zeta_{9}^{3}+\zeta_{9}^{2}+2\zeta_{9}-553,2\zeta_{9}^{5}+\zeta_{9}^{4}+6\zeta_{9}^{3}-4\zeta_{9}^{2}+22] [9,1,I9,9][9,1,I_{9},9] [9,1,I9,9][9,1,I_{9},9]
[0,2ζ95+ζ93+2ζ9+45,0,3ζ95ζ94+3ζ9+11,2ζ95ζ942ζ938ζ92+8ζ9+4][0,-2\zeta_{9}^{5}+\zeta_{9}^{3}+2\zeta_{9}+45,0,3\zeta_{9}^{5}-\zeta_{9}^{4}+3\zeta_{9}+11,2\zeta_{9}^{5}-\zeta_{9}^{4}-2\zeta_{9}^{3}-8\zeta_{9}^{2}+8\zeta_{9}+4] [9,1,I9,9][9,1,I_{9},9] [9,1,I9,9][9,1,I_{9},9]
[0,2ζ95+7ζ93+ζ92+27,0,ζ95ζ936ζ9+1,11ζ95+2ζ94+2ζ938ζ92+17][0,2\zeta_{9}^{5}+7\zeta_{9}^{3}+\zeta_{9}^{2}+27,0,\zeta_{9}^{5}-\zeta_{9}^{3}-6\zeta_{9}+1,11\zeta_{9}^{5}+2\zeta_{9}^{4}+2\zeta_{9}^{3}-8\zeta_{9}^{2}+17] [9,1,I9,9][9,1,I_{9},9] [9,1,I9,9][9,1,I_{9},9]
[0,ζ95ζ94ζ932ζ92ζ914,0,ζ95ζ94+ζ93+7ζ92ζ9+6,2ζ95+ζ94+2ζ9211ζ9][0,-\zeta_{9}^{5}-\zeta_{9}^{4}-\zeta_{9}^{3}-2\zeta_{9}^{2}-\zeta_{9}-14,0,\zeta_{9}^{5}-\zeta_{9}^{4}+\zeta_{9}^{3}+7\zeta_{9}^{2}-\zeta_{9}+6,2\zeta_{9}^{5}+\zeta_{9}^{4}+2\zeta_{9}^{2}-11\zeta_{9}] [9,1,I9,9][9,1,I_{9},9] [9,1,I9,9][9,1,I_{9},9]
[0,ζ95ζ94ζ93+ζ923,0,ζ942ζ933ζ92ζ916,31ζ953ζ94ζ93+ζ9+53][0,-\zeta_{9}^{5}-\zeta_{9}^{4}-\zeta_{9}^{3}+\zeta_{9}^{2}-3,0,-\zeta_{9}^{4}-2\zeta_{9}^{3}-3\zeta_{9}^{2}-\zeta_{9}-16,31\zeta_{9}^{5}-3\zeta_{9}^{4}-\zeta_{9}^{3}+\zeta_{9}+53] [27,1,I27,27][27,1,I_{27},27] [27,1,I27,27][27,1,I_{27},27]
[0,4ζ952ζ94+ζ93+ζ92ζ93,0,3ζ9310ζ92ζ912,ζ95+ζ94+2ζ93ζ9210ζ914][0,-4\zeta_{9}^{5}-2\zeta_{9}^{4}+\zeta_{9}^{3}+\zeta_{9}^{2}-\zeta_{9}-3,0,3\zeta_{9}^{3}-10\zeta_{9}^{2}-\zeta_{9}-12,\zeta_{9}^{5}+\zeta_{9}^{4}+2\zeta_{9}^{3}-\zeta_{9}^{2}-10\zeta_{9}-14] [18,1,I18,18][18,1,I_{18},18] [18,1,I18,18][18,1,I_{18},18]
[0,ζ94+2ζ93ζ92+2ζ9+12,0,ζ95ζ9470ζ92+ζ9129,ζ953ζ943ζ9313][0,\zeta_{9}^{4}+2\zeta_{9}^{3}-\zeta_{9}^{2}+2\zeta_{9}+12,0,-\zeta_{9}^{5}-\zeta_{9}^{4}-70\zeta_{9}^{2}+\zeta_{9}-129,\zeta_{9}^{5}-3\zeta_{9}^{4}-3\zeta_{9}^{3}-13] [9,1,I9,9][9,1,I_{9},9] [9,1,I9,9][9,1,I_{9},9]
[0,ζ952ζ93ζ92+ζ9+8,0,ζ94+4ζ93+ζ92+ζ9+8,11ζ95ζ94+84ζ934ζ92+183][0,\zeta_{9}^{5}-2\zeta_{9}^{3}-\zeta_{9}^{2}+\zeta_{9}+8,0,-\zeta_{9}^{4}+4\zeta_{9}^{3}+\zeta_{9}^{2}+\zeta_{9}+8,11\zeta_{9}^{5}-\zeta_{9}^{4}+84\zeta_{9}^{3}-4\zeta_{9}^{2}+183] [9,1,I9,9][9,1,I_{9},9] [9,1,I9,9][9,1,I_{9},9]
[0,4ζ95+10ζ948ζ934ζ923,0,9ζ95+ζ94ζ93+ζ92ζ920,ζ95+ζ94ζ93ζ927][0,-4\zeta_{9}^{5}+10\zeta_{9}^{4}-8\zeta_{9}^{3}-4\zeta_{9}-23,0,-9\zeta_{9}^{5}+\zeta_{9}^{4}-\zeta_{9}^{3}+\zeta_{9}^{2}-\zeta_{9}-20,-\zeta_{9}^{5}+\zeta_{9}^{4}-\zeta_{9}^{3}-\zeta_{9}^{2}-7] [27,1,I27,27][27,1,I_{27},27] [27,1,I27,27][27,1,I_{27},27]
[0,4ζ95+3ζ942ζ92+10ζ9+40,0,ζ95ζ94+41ζ93+86,ζ92+ζ9+10][0,4\zeta_{9}^{5}+3\zeta_{9}^{4}-2\zeta_{9}^{2}+10\zeta_{9}+40,0,\zeta_{9}^{5}-\zeta_{9}^{4}+41\zeta_{9}^{3}+86,\zeta_{9}^{2}+\zeta_{9}+10] [27,1,I27,27][27,1,I_{27},27] [27,1,I27,27][27,1,I_{27},27]
[0,ζ95+4ζ943ζ93+3ζ92+ζ9+7,0,191ζ953ζ94+ζ93+ζ92ζ9379,ζ95+7ζ94+ζ93+21][0,\zeta_{9}^{5}+4\zeta_{9}^{4}-3\zeta_{9}^{3}+3\zeta_{9}^{2}+\zeta_{9}+7,0,-191\zeta_{9}^{5}-3\zeta_{9}^{4}+\zeta_{9}^{3}+\zeta_{9}^{2}-\zeta_{9}-379,\zeta_{9}^{5}+7\zeta_{9}^{4}+\zeta_{9}^{3}+21] [9,1,I9,9][9,1,I_{9},9] [9,1,I9,9][9,1,I_{9},9]
[0,ζ94141ζ93ζ92+ζ9283,0,6ζ94ζ934ζ92+ζ916,ζ95ζ94+ζ92ζ9+11][0,-\zeta_{9}^{4}-141\zeta_{9}^{3}-\zeta_{9}^{2}+\zeta_{9}-283,0,-6\zeta_{9}^{4}-\zeta_{9}^{3}-4\zeta_{9}^{2}+\zeta_{9}-16,-\zeta_{9}^{5}-\zeta_{9}^{4}+\zeta_{9}^{2}-\zeta_{9}+11] [9,1,I9,9][9,1,I_{9},9] [9,1,I9,9][9,1,I_{9},9]
[0,6ζ95ζ944ζ93+ζ9213,0,403ζ95+ζ9311ζ92+778,3ζ95ζ94ζ92ζ975][0,-6\zeta_{9}^{5}-\zeta_{9}^{4}-4\zeta_{9}^{3}+\zeta_{9}^{2}-13,0,403\zeta_{9}^{5}+\zeta_{9}^{3}-11\zeta_{9}^{2}+778,3\zeta_{9}^{5}-\zeta_{9}^{4}-\zeta_{9}^{2}-\zeta_{9}-75] [9,1,I9,9][9,1,I_{9},9] [9,1,I9,9][9,1,I_{9},9]
[0,6ζ95+83ζ94+8ζ93ζ92ζ9+194,0,9ζ94+2ζ93+ζ92+ζ96,ζ95+ζ94+2ζ932ζ924ζ95][0,6\zeta_{9}^{5}+83\zeta_{9}^{4}+8\zeta_{9}^{3}-\zeta_{9}^{2}-\zeta_{9}+194,0,-9\zeta_{9}^{4}+2\zeta_{9}^{3}+\zeta_{9}^{2}+\zeta_{9}-6,-\zeta_{9}^{5}+\zeta_{9}^{4}+2\zeta_{9}^{3}-2\zeta_{9}^{2}-4\zeta_{9}-5] [9,1,I9,9][9,1,I_{9},9] [9,1,I9,9][9,1,I_{9},9]
[0,24ζ95+ζ9414ζ93ζ92+ζ9+17,0,2ζ952ζ94+ζ93+2ζ92+ζ9+1,ζ95+2ζ94+2ζ93ζ9+4][0,24\zeta_{9}^{5}+\zeta_{9}^{4}-14\zeta_{9}^{3}-\zeta_{9}^{2}+\zeta_{9}+17,0,-2\zeta_{9}^{5}-2\zeta_{9}^{4}+\zeta_{9}^{3}+2\zeta_{9}^{2}+\zeta_{9}+1,-\zeta_{9}^{5}+2\zeta_{9}^{4}+2\zeta_{9}^{3}-\zeta_{9}+4] [9,1,I9,9][9,1,I_{9},9] [9,1,I9,9][9,1,I_{9},9]
[0,ζ95ζ935ζ927,0,2ζ95+ζ94ζ9254ζ9114,3ζ954ζ94ζ921][0,-\zeta_{9}^{5}-\zeta_{9}^{3}-5\zeta_{9}^{2}-7,0,-2\zeta_{9}^{5}+\zeta_{9}^{4}-\zeta_{9}^{2}-54\zeta_{9}-114,3\zeta_{9}^{5}-4\zeta_{9}^{4}-\zeta_{9}^{2}-1] [9,1,I9,9][9,1,I_{9},9] [9,1,I9,9][9,1,I_{9},9]

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 FF be a pp-adic field and let X/FX/F be a geometrically connected, smooth quasi-projective variety over FF. Let KLK\leftrightsquigarrow L be anabelomorphic pp-adic fields containing FF. Write XK=X×FKX_{K}=X\times_{F}K and XL=X×FLX_{L}=X\times_{F}L.

Lemma 17.4.1.

Let KLK\leftrightsquigarrow L be an anabelomorphism of pp-adic fields. Let KnrK^{\rm nr} (resp. LnrL^{\rm nr}) be the maximal unramified extension of KK (resp. LL). Then

KnrLnr.K^{\rm nr}\leftrightsquigarrow L^{\rm nr}.

Proof.

Since the inertia subgroup IKI_{K} is amphoric by Theorem 2.4.2 and by the fact that KnrK^{\rm nr} is the fixed field of IKI_{K}, 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 KnrK^{\rm nr}. By the above lemma, KnrLnrK^{\rm nr}\leftrightsquigarrow L^{\rm nr} and hence one can affect the passage to a strictly Henselian ring without affecting anabelomorphic data.

If X/KX/K is a geometrically connected, smooth, proper variety and Xη¯X_{\bar{\eta}} (resp. XsX_{s}) is the geometric generic fiber (resp. special fiber) of a regular, proper model then one has a discriminant ΔX/K\Delta_{X/K} defined as in [Saito, 1988]. This coincides with the usual discriminant if X/KX/K is an elliptic curve. The main theorem of loc. cit. asserts that if X/KX/K is a curve then by loc. cit. one has

ordK(ΔX/K)=Artin(X/K)=χét(Xη¯)χét(Xs)+Swan(Hét1(XK×K¯,)).-\mathop{\rm ord}\nolimits_{K}(\Delta_{X/K})={\rm Artin}(X/K)=\chi_{\text{\'{e}t}}(X_{\bar{\eta}})-\chi_{\text{\'{e}t}}(X_{s})+\mathop{\rm Swan}(H^{1}_{\text{\'{e}t}}(X_{K}\times\bar{K},{\mathbb{Q}}_{\ell})).

Let

Swan(XK)=i0(1)iSwan(Héti(XK,))\mathop{\rm Swan}(X_{K})=\sum_{i\geq 0}(-1)^{i}\mathop{\rm Swan}(H^{i}_{\text{\'{e}t}}(X_{K},{\mathbb{Q}}_{\ell}))

be the Swan conductor of XKX_{K}.

Theorem 17.4.2.

Let FF be a pp-adic field and let X/FX/F be a geometrically connected, smooth proper variety over FF. Let p\ell\neq p be a prime.

  1. (1)

    Swan(XK)\mathop{\rm Swan}(X_{K}) is weakly unamphoric.

  2. (2)

    Suppose X/KX/K is one dimensional i.e. a curve. Then ordK(ΔX/K)\mathop{\rm ord}\nolimits_{K}(\Delta_{X/K}) is weakly unamphoric.

  3. (3)

    In particular, if X/KX/K is an elliptic curve then ordK(ΔX/K)\mathop{\rm ord}\nolimits_{K}(\Delta_{X/K}) is weakly unamphoric.

Proof.

Let KLK\leftrightsquigarrow L be anabelomorphic pp-adic fields containing FF. Write XK=X×FKX_{K}=X\times_{F}K and XL=X×FLX_{L}=X\times_{F}L. 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 ρ:GKGL(V)\rho:G_{K}\to{\rm GL}(V) be a GKG_{K}-representation in a finite dimension {\mathbb{Q}}_{\ell}-vector space (with p\ell\neq p a prime) such that the image of the wild inertia subgroup PKP_{K} is finite.

I claim, in fact, that the breaks in the break-decomposition of VV (see [Katz, 1988, Lemma 1.5]) are unamphoric. If KLK\leftrightsquigarrow L is a strict anabelomorphism then the GKG_{K} and GLG_{L} 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 KK be a pp-adic field and let ρ:GKGL(V)\rho:G_{K}\to{\rm GL}(V) be a continuous representation of GKG_{K} in a {\mathbb{Q}}_{\ell}-vector space VV such that the wild inertia subgroup PKP_{K} operates through a finite quotient. Then the break-decomposition of VV 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. \bullet

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 KK be a complete perfectoid field of characteristic zero (see [Scholze, 2012, Section 3]). Let KK^{\flat} 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 pp-adic completions K,LK,L respectively of

K=p(ζp,ζp2,)^pK=\widehat{{\mathbb{Q}}_{p}(\zeta_{p},\zeta_{p^{2}},\cdots)}\subset{\mathbb{C}}_{p}

and

L=p(pp,pp2,)^p.L=\widehat{{\mathbb{Q}}_{p}(\sqrt[p]{p},\sqrt[p^{2}]{p},\cdots)}\subset{\mathbb{C}}_{p}.

Then K,LK,L are both perfectoid fields. Let K,LK^{\flat},L^{\flat} be the tilts [Scholze, 2012] of K,LK,L respectively with an isometry

K𝔽p((t1/p))L.K^{\flat}\simeq{\mathbb{F}}_{p}((t^{1/p^{\infty}}))\simeq L^{\flat}.

The following is a formulation of [Scholze, 2012, Theorem 3.7] from the point of view of anabelomorphy:

Theorem 18.1.2.

Let K,LK,L be perfectoid fields with an isometry KLK^{\flat}\simeq L^{\flat} between their respective tilts. Then one has anabelomorphisms of perfectoid fields

KKLL.K\leftrightsquigarrow K^{\flat}\leftrightsquigarrow L^{\flat}\leftrightsquigarrow L.

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 (GK,GK)(G_{K},G_{K}^{\small{\bullet}}) does not identify the perfectoid field KK uniquely.

Proof.

Let GKG_{K} (resp. GKG_{K^{\flat}}) be the absolute Galois group of KK (resp. KK^{\flat}). Then by [Scholze, 2012, Theorem 3.7] one has an isomorphism

GKGKG_{K}\simeq G_{K^{\flat}}

and also the similar isomorphism for LL

GLGL.G_{L}\simeq G_{L^{\flat}}.

Since KLK^{\flat}\simeq L^{\flat}, one has an isomorphism GKGLG_{K^{\flat}}\simeq G_{L^{\flat}}. Putting these together one obtains

GKGKGLGL.G_{K}\simeq G_{K^{\flat}}\simeq G_{L^{\flat}}\simeq G_{L}.

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. \bullet

§ 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 KK is a perfectoid field. Let X/KX/K be a perfectoid space over KK [Scholze, 2012, Definition 6.15], which I will assume to be reasonable, to avoid inane pathologies. Let X/KX^{\flat}/K^{\flat} be its tilt (see [Scholze, 2012, Definition 6.16]). Let π1(X/K)\pi_{1}(X/K) 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 K,LK,L be perfectoid fields with isometric tilts. Let X/KX/K be a perfectoid space and suppose that Y/LY/L is another perfectoid space with isomorphism of the tilts

X/KY/L.X^{\flat}/K^{\flat}\simeq Y^{\flat}/L^{\flat}.

Then one has anabelomorphisms of perfectoid spaces

X/KX/KY/LY/L.X/K\leftrightsquigarrow X^{\flat}/K^{\flat}\leftrightsquigarrow Y^{\flat}/L^{\flat}\leftrightsquigarrow Y/L.

Proof.

This is a consequence of the stronger assertion [Scholze, 2012, Theorem 7.12] which implies that the categories of finite étale covers of X/KX/K and X/KX^{\flat}/K^{\flat} are equivalent.

Other examples of this phenomenon arise in the theory of Diamonds [Scholze, 2017]:

Theorem 18.2.2.

Let KLK\leftrightsquigarrow L be anabelomorphic pp-adic fields (i.e. GKGLG_{K}\simeq G_{L}), there exist geometric spaces, more precisely there exist diamonds, ZKZ_{K} and ZLZ_{L} such that

π1(ZK)GKGLπ1(ZL).\pi_{1}(Z_{K})\simeq G_{K}\simeq G_{L}\simeq\pi_{1}(Z_{L}).

Remark 18.2.3.

The formation of ZKZ_{K} (resp. ZLZ_{L}) requires K¯^\hat{\bar{K}} (resp. L¯^\hat{\bar{L}}). By [Mochizuki, 1997], if K,LK,L are strictly anabelomorphic, then the fields K¯^\hat{\bar{K}}, resp. L¯^\hat{\bar{L}}, are not isomorphic if equipped with the actions of GKG_{K} (resp. GLG_{L}). Let me also remark that the construction of ZKZ_{K} (resp. ZLZ_{L}) 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. \bullet

19 Anabelomorphy for pp-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 pp-adic differential equations in the sense of [André, 2003, Chap. III, Section 3]. Let X/KX/K be a geometrically connected, smooth, quasi-projective variety over a pp-adic field KK. Let Xan/KX^{{\rm an}}/K denote the strictly analytic Berkovitch space associated to X/KX/K. By the Riemann-Hilbert Correspondence, I mean [André, 2003, Chapter III, Theorem 3.4.6].

Theorem 19.1 (Synchronization of pp-adic differential equations).

Let X/KX/K and Y/LY/L be two geometrically connected, smooth, quasi-projective varieties over pp-adic fields KK and LL. Assume that Xan/KX^{{\rm an}}/K and Yan/LY^{{\rm an}}/L are anabelomorphic strictly analytic spaces (i.e. α:π1(Xan/K)π1(Yan/L)\alpha:\pi_{1}(X^{{\rm an}}/K)\simeq\pi_{1}(Y^{{\rm an}}/L) (where the fundamental groups with respect to a KK-rational (resp. an LL-rational) base point)). Then there exists a natural bijection α\alpha between pp-adic differentials on Xan/KX^{{\rm an}}/K and Yan/LY^{{\rm an}}/L which associates to a pp-adic differential equation (V,)(V,\nabla) on Xan/KX^{{\rm an}}/K, a pp-adic differential equation Yan/LY^{{\rm an}}/L such that the associated (discrete) monodromy representation of π1(Yan/L)\pi_{1}(Y^{{\rm an}}/L) is given composing with α1:π1(Yan/L)π1(Xan/K)\alpha^{-1}:\pi_{1}(Y^{{\rm an}}/L){\lx@xy@svg{\hbox{\raise 0.0pt\hbox{\kern 3.0pt\hbox{\ignorespaces\ignorespaces\ignorespaces\hbox{\vtop{\kern 0.0pt\offinterlineskip\halign{\entry@#!@&&\entry@@#!@\cr&\crcr}}}\ignorespaces{\hbox{\kern-3.0pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise 0.0pt\hbox{$\textstyle{{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern 9.27777pt\raise 4.62312pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.62312pt\hbox{$\scriptstyle{\simeq}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern 27.0pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}{\hbox{\kern 27.0pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise 0.0pt\hbox{$\textstyle{}$}}}}}}}\ignorespaces}}}}\ignorespaces}\pi_{1}(X^{{\rm an}}/K).

Let X/FX/F be a geometrically connected, smooth, quasi-projective variety over a pp-adic field FF. Let KLK\leftrightsquigarrow L be anabelomorphic pp-adic fields containing FF. Then given any α:KL\alpha:K\to L. Then one can consider our pp-adic differential equation as a pp-adic differential equation on Xan/KX^{{\rm an}}/K and Xan/LX^{{\rm an}}/L. In particular, it is possible to ask if there are quantities, properties algebraic structures associated to a differential equation on X/KX/K which are weakly unamphoric (i.e. with respect to anabelomorphisms KLK\leftrightsquigarrow L). When I speak of a weakly amphoric quantity (resp. property, alg. structure) associated to a pp-adic differential equation, I mean weak amphoricity (resp. weak unamphoricity) with respect to anabelomorphisms KLK\leftrightsquigarrow L.

An important invariant of interest is the index of irregularity of a pp-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 X/FX/F is a curve (i.e. dim(X)=1\dim(X)=1) and let KFK\supseteq F be a finite extension. Then the index of irregularity of a pp-adic differential equation (V,)(V,\nabla) on X/KX/K is weakly unamphoric. More generally, the irregularity module of the differential equation (V,)(V,\nabla) over X/KX/K is weakly unamphoric (XX 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. \bullet

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 {\mathbb{Q}}-Hodge structure is semi-simple, on the other hand there are no one dimensional {\mathbb{Q}}-Hodge structures of weight one, and so the Hodge structure of an elliptic curve is indecomposable as a {\mathbb{Q}}-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 H1(GK,p(1))H^{1}(G_{K},{\mathbb{Q}}_{p}(1)) corresponding to Θ\Theta-functions on an elliptic curve.

For the Diophantine applications which Mochizuki considers in [Mochizuki, 2021a, b, c, d], let KK be a number field which one typically assumes to have no real embeddings. Let E/KE/K be an elliptic curve and assume that the Faltings height h(E)h(E) of EE is large. By the known facts about Faltings height, h(E)0h(E)\gg 0 corresponds to h(jE)0h(j_{E})\gg 0 and equivalently this means that the Schottky (uniformization) parameter qE=e2πiτEq_{E}=e^{2\pi i\tau_{E}} of EE is small.

Schottky uniformization of elliptic curves says that one has an isomorphism of complex abelian manifolds

/qEE(){\mathbb{C}}^{*}/q_{E}^{\mathbb{Z}}{\lx@xy@svg{\hbox{\raise 0.0pt\hbox{\kern 3.0pt\hbox{\ignorespaces\ignorespaces\ignorespaces\hbox{\vtop{\kern 0.0pt\offinterlineskip\halign{\entry@#!@&&\entry@@#!@\cr&\crcr}}}\ignorespaces{\hbox{\kern-3.0pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise 0.0pt\hbox{$\textstyle{{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern 9.27777pt\raise 4.62312pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.62312pt\hbox{$\scriptstyle{\simeq}$}}}\kern 3.0pt}}}}}}\ignorespaces{\hbox{\kern 27.0pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}{\hbox{\kern 27.0pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise 0.0pt\hbox{$\textstyle{}$}}}}}}}\ignorespaces}}}}\ignorespaces}E({\mathbb{C}})

at infinity (let me remind the readers that Tate’s Theory of pp-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:

ExtMHS1((0),(1))=.{\rm Ext}\,^{1}_{MHS}({\mathbb{Z}}(0),{\mathbb{Z}}(1))={\mathbb{C}}^{*}.

In particular, the Schottky parameter qEq_{E}\in{\mathbb{C}}^{*} provides a unique mixed Hodge structure

H=H(E)ExtMHS1((0),(1))=H=H(E)\in{\rm Ext}\,^{1}_{MHS}({\mathbb{Z}}(0),{\mathbb{Z}}(1))={\mathbb{C}}^{*}

(not to be confused with the usual Hodge structure H1(E,)H^{1}(E,{\mathbb{Z}}) which is of weight one. The mixed Hodge structure H(E)H(E) comes equipped with a weight filtration and unipotent monodromy (see [Deligne, 1997]). In particular, let me recall the formula from [Deligne, 1997]:

(20.2) H\displaystyle H_{\mathbb{C}} =\displaystyle= e0e1,\displaystyle{\mathbb{C}}e_{0}\oplus{\mathbb{C}}e_{1},
(20.3) W2H\displaystyle W_{-2}\subset H =\displaystyle= e1,\displaystyle{\mathbb{C}}e_{1},
(20.4) F0H\displaystyle F^{0}\subset H =\displaystyle= e0,\displaystyle{\mathbb{C}}e_{0},
(20.5) H\displaystyle H_{\mathbb{Z}} =\displaystyle= 2πie0(e0+log(q)e1)H.\displaystyle 2\pi i{\mathbb{Z}}e_{0}\oplus{\mathbb{Z}}(e_{0}+\log(q)e_{1})\subset H_{\mathbb{C}}.

The mapping (1)H{\mathbb{Z}}(1)\to H_{\mathbb{Z}} is given by 2πi2πie12\pi i\longmapsto 2\pi ie_{1} and H(0)H_{\mathbb{Z}}\to{\mathbb{Z}}(0) is given by e01e_{0}\longmapsto 1. Then one has an exact sequence of mixed Hodge structures

0(1)H(0)0,0\to{\mathbb{Z}}(1)\to H\to{\mathbb{Z}}(0)\to 0,

whose class in ExtMHS1((0),(1)){\rm Ext}\,^{1}_{MHS}({\mathbb{Z}}(0),{\mathbb{Z}}(1)) is given by qq\in{\mathbb{C}}^{*}.

Now let u=e2πizu=e^{2\pi iz} with zz\in{\mathbb{C}} and let ΘE=Θ(q,0)\Theta_{E}=\Theta(q,0) where Θ(q,z)=1+O(q)\Theta(q,z)=1+O(q) is a suitable Jacobi Theta function on E/E/{\mathbb{C}}. For 0<|q|10<|q|\ll 1, ΘE\Theta_{E}\in{\mathbb{C}}^{*} and hence provides us a mixed Hodge structure HE,ΘExtMHS1((0),(1))H_{E,\Theta}\in{\rm Ext}\,^{1}_{MHS}({\mathbb{Z}}(0),{\mathbb{Z}}(1)) given by ΘE\Theta_{E}\in{\mathbb{C}}^{*}.

Thus I have proved the following:

Theorem 20.6.

Let E/E/{\mathbb{C}} be an elliptic curve with Schottky parameter q=qEq=q_{E} such that 0<|q|10<|q|\ll 1. Then

  1. (1)

    there is mixed Hodge structure H=H(E)Ext1((0),(1))H=H(E)\in{\rm Ext}\,^{1}({\mathbb{Z}}(0),{\mathbb{Z}}(1))\simeq{\mathbb{C}}^{*} whose extension class corresponds to qq\in{\mathbb{C}}^{*}, and

  2. (2)

    there is a mixed Hodge structure HΘ=H(E,Θ)Ext1((0),(1))H_{\Theta}=H(E,\Theta)\in{\rm Ext}\,^{1}({\mathbb{Z}}(0),{\mathbb{Z}}(1)) whose extension class corresponds to the θ\theta-value ΘE=Θ(q,0)\Theta_{E}=\Theta(q,0)\in{\mathbb{C}}^{*}.

Remark 20.7.

The mixed Hodge structures H(E),H(E,Θ)H(E),H(E,\Theta) correspond, at a prime vv of semi-stable reduction, to the GvG_{v}-modules H1(E,p)H^{1}(E,{\mathbb{Q}}_{p}) and the Θ\Theta-value class constructed by Mochizuki in [Mochizuki, 2009], [Mochizuki, 2015]. \bullet

Remark 20.8.

Comparing the definition above of HH and with the formula of Fontaine for 𝔏\mathfrak{L}-invariant, I define the 𝔏\mathfrak{L}-invariant 𝔏(H)=log(q)2πi\mathfrak{L}_{\infty}(H)=\frac{\log(q)}{2\pi i}. If q=e2πiτq=e^{2\pi i\tau} then 𝔏(H)=τ\mathfrak{L}_{\infty}(H)=\tau! So τ\tau is the 𝔏\mathfrak{L}-invariant of the elliptic curve at archimedean primes and anabelomorphy changes the 𝔏\mathfrak{L}-invariant at all the places. \bullet

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 E/E/{\mathbb{C}} be an elliptic curve and let X=E{O}X=E-\{O\}. Let f𝒪Xf\in{\mathscr{O}}_{X}^{*} be a meromorphic function on EE which is an invertible function on XX. More generally, one can consider any open subset UU of EE and consider f𝒪Uf\in{\mathscr{O}}_{U}^{*} i.e. an invertible function on UU. Then there exists a variation of mixed Hodge structures (over UU) H(E,f)ExtVMHS1((0),(1))H(E,f)\in{\rm Ext}\,^{1}_{V-MHS}({\mathbb{Z}}(0),{\mathbb{Z}}(1)) such that under the natural identification

ExtVMHS1((0),(1))=𝒪U{\rm Ext}\,^{1}_{V-MHS}({\mathbb{Z}}(0),{\mathbb{Z}}(1))={\mathscr{O}}_{U}^{*}

the extension class corresponding to H(E,f)H(E,f) is equal to f𝒪Uf\in{\mathscr{O}}_{U}^{*}. The mixed Hodge structure H(E,f)H(E,f) is constructed as follows (see [Deligne, 1997]). Let V=𝒪Ue1+𝒪Ue2V={\mathscr{O}}_{U}e_{1}+{\mathscr{O}}_{U}e_{2} be a locally free 𝒪U{\mathscr{O}}_{U} module with basis e1,e2e_{1},e_{2}. The connection \nabla (with log-poles at OO) on VV is defined by

=d+(00dff0).\nabla=d+\begin{pmatrix}0&0\\ -\frac{df}{f}&0\end{pmatrix}.

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 (V,,Fil(V))(V,\nabla,Fil(V)) consisting of the bundle VV together with the connection \nabla and the Hodge filtration is the data of an indigenous bundle (equivalently a rank two oper) on UU.

So one can apply this consideration to a chosen ff such as a theta function on EE which does not vanish on the open set X=E{O}X=E-\{O\}. By the theory of theta functions, up to scaling by a constant, there is a unique function with this property, denoted by Θ(q,z)\Theta(q,z). 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 {1,τ}\{1,\tau\} satisfies

(20.9) θ(q,z+1)θ(q,z+1)\displaystyle\frac{\theta(q,z+1)^{\prime}}{\theta(q,z+1)} =\displaystyle= θ(q,z)θ(q,z)\displaystyle\frac{\theta(q,z)^{\prime}}{\theta(q,z)}
(20.10) θ(q,z+τ)θ(q,z+τ)\displaystyle\frac{\theta(q,z+\tau)^{\prime}}{\theta(q,z+\tau)} =\displaystyle= 2πi+θ(q,z)θ(q,z).\displaystyle-2\pi i+\frac{\theta(q,z)^{\prime}}{\theta(q,z)}.

More precisely, there is a vector bundle on EE of rank two and a connection on EE, with log-poles at OO, which on the universal cover {\mathbb{C}} of EE is given by the connection matrix as above with f=Θ(q,z)f=\Theta(q,z). At any rate, the connection defined by the above formula on {\mathbb{C}} descends to EE (with log-poles at OO). Hence one has proved that

Theorem 20.11.

Let E/E/{\mathbb{C}} be an elliptic curve with Schottky parameter q=qEq=q_{E} such that 0<|q|10<|q|\ll 1 and let X=E{O}X=E-\{O\}. Let Θ(q,z)\Theta(q,z) be a Theta function on EE which does not vanish on XX and normalized so that Θ(q,z)=1+O(q)\Theta(q,z)=1+O(q). Then there is a variation of mixed Hodge structures over XX, denoted

H=H(E,Θ(q,z))ExtVMHS1((0),(1))𝒪XH=H(E,\Theta(q,z))\in{\rm Ext}\,^{1}_{V-MHS}({\mathbb{Z}}(0),{\mathbb{Z}}(1))\simeq{\mathscr{O}}_{X}^{*}

such that the extension class of H(E,f)H(E,f) corresponds to Θ(q,z)𝒪X\Theta(q,z)\in{\mathscr{O}}_{X}^{*} (here 𝒪X{\mathscr{O}}_{X}^{*} is the group of holomorphic functions which are invertible on XX). 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 XX be a non-proper hyperbolic Riemann surface, π1top(X)\pi_{1}^{top}(X) its topological fundamental group. Let [π1top(X)]{\mathbb{Q}}[\pi_{1}^{top}(X)] be the group ring and J[π1top(X)]J\subset{\mathbb{Q}}[\pi_{1}^{top}(X)] be the augmentation ideal. By well-known results for each r1r\geq 1, [π1top(X)]/Jr+1{\mathbb{Q}}[\pi_{1}^{top}(X)]/J^{r+1} carries a mixed Hodge structure and good unipotent variations of mixed Hodge structures on XX of nilpotence 2\leq 2 with values in {\mathbb{Q}} (or a real field) arise precisely from finite dimensional representations VV of π1top(X)\pi_{1}^{top}(X) such that the natural map [π1top(X)]/J3End(V){\mathbb{Q}}[\pi_{1}^{top}(X)]/J^{3}\to\rm{End}(V) 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 XX, denoted ExtVMHS1((0),(1)){\rm Ext}\,^{1}_{V-MHS}({\mathbb{Q}}(0),{\mathbb{Q}}(1)) is also described, by [Carlson and Hain, 1989, Theorem 12.1] in an essentially anabelomorphic way, as follows:

H1(X,(1))H1(π1top(X),(1))ExtVMHS1((0),(1))𝒪X.H^{1}_{\mathscr{H}}(X,{\mathbb{Q}}(1))\simeq H^{1}_{\mathscr{H}}(\pi^{top}_{1}(X),{\mathbb{Q}}(1))\simeq{\rm Ext}\,^{1}_{V-MHS}({\mathbb{Q}}(0),{\mathbb{Q}}(1))\simeq{\mathscr{O}}_{X}^{*}\otimes{\mathbb{Q}}.

The cohomology H1H^{1}_{\mathscr{H}} 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 XX). \bullet

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