• Aucun résultat trouvé

ON THE NON-VANISHING OF p-ADIC HEIGHTS ON CM ABELIAN VARIETIES, AND THE ARITHMETIC

N/A
N/A
Protected

Academic year: 2022

Partager "ON THE NON-VANISHING OF p-ADIC HEIGHTS ON CM ABELIAN VARIETIES, AND THE ARITHMETIC"

Copied!
26
0
0

Texte intégral

(1)

ANNALES DE

L’INSTITUT FOURIER

LesAnnales de l’institut Fouriersont membres du

Ashay A. Burungale & Daniel Disegni

On the non-vanishing ofp-adic heights on CM abelian varieties, and the arithmetic of Katzp-adicL-functions Tome 70, no5 (2020), p. 2077-2101.

<http://aif.centre-mersenne.org/item/AIF_2020__70_5_2077_0>

© Association des Annales de l’institut Fourier, 2020, Certains droits réservés.

Cet article est mis à disposition selon les termes de la licence Creative Commons attribution – pas de modification 3.0 France.

http://creativecommons.org/licenses/by-nd/3.0/fr/

(2)

ON THE NON-VANISHING OF p-ADIC HEIGHTS ON CM ABELIAN VARIETIES, AND THE ARITHMETIC

OF KATZ p-ADIC L-FUNCTIONS

by Ashay A. BURUNGALE & Daniel DISEGNI

Abstract. —LetBbe a simple CM abelian variety over a CM field E,pa rational prime. Suppose that B has potentially ordinary reduction abovep and is self-dual with root number −1. Under some further conditions, we prove the generic non-vanishing of (cyclotomic)p-adic heights onBalong anticyclotomicZp- extensions ofE. This provides evidence towards Schneider’s conjecture on the non- vanishing ofp-adic heights. For CM elliptic curves overQ, the result was previously known as a consequence of works of Bertrand, Gross–Zagier and Rohrlich in the 1980s. Our proof is based on non-vanishing results for Katzp-adicL-functions and a Gross–Zagier formula relating the latter to families of rational points onB.

Résumé. —SoientBune variété abélienne CM simple sur un corps CME,p un premier rationnel. On suppose que B a une réduction potentiellement ordi- naire au dessus de pet est auto-duale avec signe−1. Sous quelques hypothèses supplementaires, on montre la non-annulation générique des hauteurs p-adiques (cyclotomiques) surBle long deZp-extensions anticyclotomiques deE. Cela con- firme partiellement la conjecture de Schneider sur la non-annulation des hauteurs p-adiques. Pour les courbes elliptiques CM sur Q, le résultat était déjà connu comme conséquence de travaux de Bertrand, Gross–Zagier et Rohrlich dans les années 80. Notre preuve est basée sur des résultats de non-annulation pour les fonctionsL p-adiques de Katz, et sur une formule de Gross–Zagier qui les relie à des familles de points rationnels surB.

1. Introduction and statements of the main results LetBbe an abelian variety over a number fieldE, and letBbe its dual.

Letp be a prime and letL be a finite extension of Qp. The Néron–Tate height pairing onB(E0)Q×B(E0)Q, whereE0 is a finite extension ofE, admits ap-adic analogue (see e.g. [34])

(1.1) B(E0)Q×B(E0)QL

Keywords:Keywords:p-adic heights, Katzp-adicL-functions, CM abelian varieties.

2020Mathematics Subject Classification:11G50, 11G10, 11G40.

(3)

depending on the choices of a homomorphism `:E×\E×AL (“p-adic logarithm”) and on splittings of the Hodge filtration on HdR1 (B/Ev) at the primesv|p; in the potentially ordinary case under consideration in this paper, there are canonical choices (the “unit root” subspaces) for the Hodge splittings.

While it is a classical result that the Néron–Tate height pairing is non- degenerate, the pairing (1.1) can vanish for some choices of `. Suppose however that` =`QNE/Q with `Q a p-adic logarithm of Q such that

`Q|1+pZp is nontrivial (we call such ` a cyclotomic logarithm). Then it is conjectured [39] that (1.1) is non-vanishing. This long-standing conjecture is only known in a few special cases: for CM elliptic curves, thanks to Bertrand [6], and also for elliptic curves overQat supersingular primes.(1) The stronger statement that (1.1) is non-degenerate is also conjectured to be true; this is not known in any cases of rank higher than 1. The non- degeneracy conjecture has arithmetic consequences: it allows to formally deduce thep-adic Birch and Swinnerton-Dyer conjecture from the Iwasawa main conjecture forB.(2)

The pairing (1.1) is equivariant for the actions of Gal(E0/E) and of K := End0(B) on both sides; for our purposes we can then assume that B is simple, that the coefficient field L is sufficiently large and has the structure of aK⊗Qp-algebra, and then decompose the pairing into isotypic components

(1.2) B(χ)LB χ−1

L

for the Gal(E0/E)-action. Here and in the rest of the paper, if R is a KQp-algebra andχis anR×-valued character of Gal(Eab/E), we define

B(χ) := B(Eab)⊗K⊗QpR(χ)Gal(Eab/E) , whereR(χ) is a rank-1 R-module with Galois action byχ.

The most significant result of this paper is the proof that, under some assumptions, the non-vanishing conjecture for (1.2) is true “generically”

whenB is ap-ordinary CM abelian variety over a CM fieldEandχvaries among anticyclotomic characters ofE unramified outside p.

The method of proof, different from that of previous results on this topic, is automorphic. (In particular, the approach does not involve transcendence arguments.) It combines two ingredients. The first is a pair of nonvanishing

(1)This was observed in [4]; see [31, Section 4.5] for the comparison between the definition of the height pairing used in [4] and the “standard” definition of Zarhin and Nekovář [34].

(2)See [39]. For further applications to theclassicalBirch and Swinnerton–Dyer formula, see [20, 31, 37].

(4)

results for Katzp-adicL-functions due to Hida, Hsieh, and the first author (in turn relying on Chai’s results on Hecke-stable subvarieties of a mod pShimura variety [15, 16, 17]). The second ingredient is a Gross–Zagier formula relating derivatives of Katz p-adic L-functions to families of ra- tional points on CM abelian varieties. We deduce this formula from work of the second author, by an argument employed by Bertolini–Darmon–

Prasanna [5] in a different context.

In the rest of this section we describe the main results in more detail.

1.1. Non–vanishing of p-adic heights

Let B/E be a simple CM abelian variety over a CM field E, i.e.

K := End0(B) is a CM field of degree [K : Q] = 2 dimB. Let F be the maximal totally real subfield ofE, and letη=ηE/F be the associated character ofF×\FA×.

1.1.1. Assumptions

The abelian variety B is associated with a Hecke character λ= (λτ):K,→C): E×\EA×→(K⊗C)× ([42, Section 19]). Suppose thatλsatisfies the condition

(1.3) λ|F×

A

=η| · |−1A ;

this holds in particular whenever B arises as the base-change of a real- multiplication abelian varietyA/F [42, Theorem 20.15]. It implies that the for eachτ there is a functional equation with signw(λ) :=ε(1, λτ)∈ {±1}

(independent ofτ) relatingL(s, λτ) toL(2s, λτ). We will assume that

(1.4) w(λ) =−1.

Finally, we assume that

(1.5) B has potentiallyordinary reduction at every prime ofEabove p.

1.1.2. Anticyclotomic regulators

Let E (respectively E+) be the anticyclotomic Z[F:Q]p -extension (re- spectively cyclotomic Zp-extension) of E and, for a prime of F above p, let E℘,∞E be the ℘-anticyclotomic subextension, i.e. the maxi- mal subextension unramified outside the primes abovein E; finally, let

(5)

E:=EE+ andE℘,∞=E℘,∞ E+. If•is any combination of subscripts

∅,and superscripts∅, +,−(we convene that ‘∅’ denotes no symbol), the corresponding infinite Galois group is

Γ:= Gal(E•,∞/E).

Let Lbe a finite extension of a p-adic completion Kw ofK. If• is any set of sub- and superscripts as above, we let

Λ:=OL[[Γ]]⊗L, Y:= Spec Λ.

When we want to emphasise the role of a specific choice ofL, we will write Λ•, L,Y•, L.

For◦=℘,∅we let

χuniv,◦: Γ →Λ−, × be the tautological anticyclotomic character.

We then have a Λ-module

B(χuniv,◦) := B(E)⊗Λuniv,◦)Gal(E/E) ,

whose specialisation at any finite order character χ ∈ Y is B(χ), and height pairings ([36, Section 2.3], see also [35, Section 11])

(1.6) B(χuniv,◦)⊗ΛB χ−1univ,◦

→Λ

associated with choices of ap-adic logarithm`and of Hodge splittings. We suppose that`: Gal(Eab/E)Lis the cyclotomic logarithm and that the Hodge splittings are given by the unit root subspaces.

Theorem 1.1. — LetB be a simple CM abelian variety over the CM fieldEwith associated Hecke characterλsatisfying (1.3),(1.4), and(1.5);

suppose that the extensionE/F is ramified. Letpbe a rational prime, and suppose thatp-2DFhE, where hE =hE/hF is the relative class number ofE/F and DF is the absolute discriminant of F. Letbe a prime of F abovep, and letLKwKbe as above.

Then for almost all finite-order characters χofΓ, the pairing(1.2) B(χ)LB χ−1

L

is non-vanishing. Equivalently, the paring (1.6) for◦ = (hence also for

◦=∅) is nonzero.

Here “almost all” means that the set of finite-order characters χ∈Y

which fail to satisfy the conclusion of the theorem is not Zariski dense in Y. When dimY = 1 (e.g. F = Q), this is equivalent to such set of exceptions being finite.

(6)

1.2. Gross–Zagier formula for the Katz p-adic L-function

As recalled in Section 2.4, under our conditions and assuming that the extension LKw splits E, the character λ (more precisely, its w-adic avatar) has ap-adic CM type ΣE⊂Hom(E, L) ofE. We also identify ΣE

with (i) a choice, for each prime℘|pofF, of one among the two primes of E above ℘, and (ii) an element of Z[Hom(E, L)]. To the CM type ΣE is attached the Katzp-adicL-function

LΣE∈Λ.

It interpolates the values L(0, λ0−1) for characters λ0 whose infinity type lies in a certain region ofZ[Hom(E,Cp)]; this region is uniquely determined by ΣE and contains in particular the infinity type ΣE.

Let λ(x) := λ(xc), where c denotes the complex conjugation of E/F. The root number assumption (1.4) implies that LΣE(λ) = LΣEc)

= L(0, λ∗−1) = L(0, λ−1) = L(1, λ) = L(B,1) = 0, and more generally that the functionLΣEc, λ:χ07→LΣEcχ0) vanishes alongY⊂Y. We may then consider the cyclotomic derivative

L0ΣEc, λ:χ7→ d

dsLΣEc λχ·χscyc s=0,

forχ∈Y. (Hereχcycis thep-adic cyclotomic character ofEA×).

For◦=∅, ℘, letKbe the field of fractions of Λ and letB(χuniv,◦)K

:=Buniv,◦)⊗Λ

K; similarly forB−1univ)K

.

Theorem 1.2. — Let◦=∅or◦=℘. Under the assumptions of Theo- rem 1.1, there is a ‘pair of points’

P⊗PB χ−1univ,◦

K

B(χuniv,◦)K

satisfying

hP,Pi=L0ΣEc, λ|Y

in K, where h,i is the height pairing (1.6), and we identify Γ+ ∼=Zp

via the cyclotomic logarithm.

The construction of the points depends on some choices, analogously to how the construction of rational points on an elliptic curve over Q of analytic rank one depends on the choice of an auxiliary imaginary quadratic field. Like in that situation, it comes from Heegner points and relies on a non-vanishing result forL-functions – in this case, the results of Hida and Hsieh [25, 28] for anticyclotomic Katzp-adicL-functions. Nevertheless the auxiliary setup does not seem to be explored in regard to the cyclotomic derivative.

(7)

The following Conjecture 1.3, which can be regarded as analogous to the results of Kolyvagin, would imply that the ambiguity is rather mild.

Conjecture 1.3. — Let ◦ = ∅ or ◦ = for a prime p of F. The K-vector spacesB χ−1univ,◦

K

,Buniv,◦)K

have dimension one.

WhenE is an imaginary quadratic field andB is the base-change of an elliptic curve overQ, the conjecture is part of the main result of Agboola and Howard in [2].

Remark 1.4. — It is natural to wonder about the arithmetic significance of the values

(1.7) LΣ0E)

for CM types Σ0E such that

δ(Σ0E) :=|Σ0E∩ΣE|>1.

We would like to suggest that ifδ(Σ0E) 6 r := ords=1L(B, s), the cyclo- tomic order of vanishing ofLΣ0

E atλ(that is, the smallestksuch that the cyclotomic derivativeL(k)Σ0

E

)6= 0) should be

(1.8) ordcycLΣ0

E, λ

=? rδ(ΣE0) and that there should be an explicit formula relating

L(r−δ(ΣΣ0 E0)) E

)

to ap-adic regulator. When [E:Q] is a quadratic field andλcomes from an elliptic curve, (1.8) was conjectured by Rubin [38] together with a precise formula, and proved by himself whenr61.

Theorem 1.2 provides evidence for the general case of (1.8) in one of the cases withr61, whereas the other such case is treated, when [E:Q] = 2, by Rubin’s formula as generalised by Bertolini–Darmon–Prasanna [5].(3) The particular interest of the case of [E : Q] > 2 lies of course in the possibility of havingδ(Σ0E)>2: our speculation is also inspired from the recent work of Darmon–Rotger [19] onp-adicL-functions related to certain Mordell–Weil groups of rank 2.

(3)We hope to present a generalisation of this formula in a sequel to the present paper.

(8)

1.3. An arithmetic application

For an elliptic curve E/Q and a primep, let us refer to the implication corankZpSelp(E/Q) = 1 =⇒ ords=1L(s, E/Q) = 1

as the “p-converse theorem” (to the one of Gross–Zagier, Kolyvagin and Rubin). In [13], the authors establish thep-converse theorem in the case of p-ordinary CM elliptic curves (complementing the earlier works [43, 46]).

The approach crucially relies on the auxiliary setup introduced in the proof of the main results here, and also on the main results themselves (Theo- rem 1.1 and Theorem 1.2).

1.4. Context and strategy of proof

When E is an imaginary quadratic field and B = AE for a CM elliptic curve A/Q, Theorem 1.1 is a consequence (see Rubin [3]) of the aforementioned result of Bertrand together with Mazur’s conjecture on the generic non-vanishing of Heegner points along anticyclotomic extensions (which in that case is proved, via the Gross–Zagier formula, by the generic non-vanishing of derivatives of L-functions established by Rohrlich). Our method is rather different (although not distant in spirit): we first deduce the formula of Theorem 1.2 from the p-adic Gross–Zagier formula of the second author [21]. Theorem 1.1, or rather its more precise version Theo- rem 2.11 below, is then a consequence of Theorem 1.2 and non-vanishing results of the first author [7] (or their refinement in [11]) for the derivatives of Katzp-adicL-functions. As a corollary we recover Mazur’s conjecture, which in our case was proved by Aflalo–Nekovář [1] as a generalisation of work of Cornut and Vatsal. Note further that our method would readily adapt to cover the case of (generalised) Heegner cycles upon availability of a suitably general p-adic Gross–Zagier formula for them. The second author expects to present such a formula as part of a forthcoming version of [22].(4)

A parallel approach is followed by the first author in a series of works [9], [10] establishing, without assumptions of complex multiplication, the gene- ric non-vanishing of Heegner points and cycles, or more precisely of (the reduction modulopof) their images under the Abel–Jacobi map (also see [8]

(4)Note added in proof: this formula has now been proven.

(9)

and [12]).(5) The strategy to prove Theorem 1.2 is inspired from the proof of Rubin’s formula in [5]. As in [5], we can remark that we have established a result for a motive attached to the group U(1) by making use ofp-adic L-functions for U(1)×U(2). Readers with a generous attitude towards mathematical induction might find in this a good omen for future progress.

Acknowledgments

We would like to thank D. Bertrand, K. Büyükboduk, F. Castella, M. Chida, H. Darmon, H. Hida, B. Howard, M.-L. Hsieh, M. Kakde, J. Lin, J. Nekovář, D. Prasad, D. Rohrlich, K. Rubin, C. Skinner and Y. Tian for useful conversations, correspondence or suggestions. We are grateful to the referee for thorough comments and suggestions. During part of the writing of this paper, the second author was funded by a public grant from the Fondation Mathématique Jacques Hadamard.

2. Proofs 2.1. CM theory

We start by reviewing some basic results in the theory of Complex Mul- tiplication. The classical reference is [42] (see especially Sections 18-20); see also [18, Section 2.5].

Let B be an abelian variety of dimension d over a field E, such that End0(B) =K is a CM field of degree 2d. Denote byMK the maximal totally real subfield. The action of K on LieB gives, after base-change from E to an extension ι: E ,C which splits K, a CM type (K,Σ) over C, namely Σ = Σ(B, ι) is a set of representatives for the action of Gal(K/M) on Hom(K, C). Finally, to the CM type (K,Σ) we can associate its reflex CM type (K,Σ); the reflex field K =K(ι) (which depends onι) comes as a subfieldKE. The set ΣE := InfE/KΣ⊂Hom(E, C), consisting of those embeddings whose restriction toK belongs to Σ, is a CM type ofE. Finally, the CM type Σ(ι) gives rise to a homomorphism NΣ(ι): K(ι)×K× called thereflex norm. The homomorphism (2.1) NΣE :=NΣ(ι)NE/K(ι):E×K×

(5)Note that, asp-adic heights factor through thep-adic Abel–Jacobi map, their non- vanishing is a finer statement.

(10)

is independent of choices.

A CM type Σ0 of K0 with values in an extension C of Qp splitting E is said to be ap-adic CM type(6) if its elements induce pairwise distinct p-adic places ofK0. This condition can only be satisfied if all primesp0+ of K0+(the maximal totally real subfield ofK0) abovepsplit inK0. We may and will identify ap-adic CM type with a set of primesp0 ofK0 containing exactly one prime above eachp0+|pofK0+.

Lemma 2.1. — Suppose that B has potentially ordinary reduction at all primes ofEabove p. Then:

(1) for each embeddingιp:E ,Qp, the setΣ(B, ιp)is a p-adic CM type ofK;

(2) the primepis totally split inK;

(3) for each ιp:E ,Qp, the setΣp) := Σ(B, ιp) is a p-adic CM type ofK.

Proof. — Part (1), which is in fact equivalent to the hypothesis of the lemma, can be checked after base-change fromE to a finite extension over whichB acquires good reduction. There it becomes a well-known immedi- ate consequence of the Shimura–Taniyama formula [18, (2.1.4.1)]. Part (1) implies part (2) by [29, Proposition 7.1]. Part (3) is implied by part (2).

The main theorem of Complex Multiplication attaches toB a character λ:EA×K×

such that (2.2)

for allτ:E ,C, λτ :=τλ· NΣτ

E,∞

−1

:EA×C× satisfiesλτ|E× = 1, (2.3) λ(x)λ(x)ρ=|x|−1A for all xEA×.

Hereρis the complex conjugation inKandNΣτ

E,: E×K×Kτ× is the continuous extension ofNΣE. We say thatλτ is an an algebraic Hecke character of infinity type ΣτE, where ΣτE⊂Hom(E,C) is defined by

NΣτE,(x) = Y

ιΣτE

ι(x) for all xE×. TheL-function ofB is

(2.4) L(B, s) =L(s, λ) := (L(s, λτ))τ∈Hom(K,C)KC∼=CHom(K,C); it satisfies a functional equation with centre ats= 1.

(6)In some of the literature this is called ap-ordinary CM type.

(11)

Suppose now that B = AE for an abelian variety A/F with End0(A)

=M (the maximal totally real subfield of K). Then E =KF [42, Re- mark 20.5].

Suppose conversely that λis a Hecke character ofE satisfying the con- ditions (2.2), (2.3) for a CM type (K,Σ). Then by a theorem of Casselman (e.g. [18, Theorem 2.5.2]), there is an abelian varietyB=Bλ/E, unique up toE-isogeny, satisfying (2.4). The abelian variety B is simple if and only if the CM type (K,Σ) is not induced from a CM type of a subfield of K.

2.2. Theta lifts of Hecke characters

LetQdenote an algebraic closure ofK, letχ0:E×\EA×Q× be finite order character, and letψ be a Hecke character ofE with the same CM type as the characterλfrom the Introduction. We suppose that

(2.5) χ0|F×

A

=ω:=η·ψ|F×

A

· | |AF.

LetK0Qbe a CM extension ofKcontaining the values ofχ0andψ|E×

A. 2.2.1. The abelian variety associated withψ

By construction, ψsatisfies conditions (2.2), (2.3) for the CM type (K0, InfK0/KΣ), and in particular it is associated with an abelian varietyBψ, K0 /Eof dimension [K0 :Q]/2, which is uniquely determined up toE-isogeny, has CM by K0, and is K-linearly isogenous to a sum of copies of a sim- ple CM abelian variety. (Note that Bψ, K0 depends on the choice of K0: ifK0K00 is a finite extension of CM fields of degreed0, then Bψ, K00Bψ, K⊕d0 0.) We denote byBψ\ any one of the simpleE-isogeny factors ofBψ, K0. On the other hand, the theta correspondence attaches toψa Gal(M/Q)- conjugacy class (for some totally real fieldMK0) of cuspidal automor- phic representations σ= (στM)MHom(M,C)) of ResF /QGL2 of parallel weight 2; namelyστM =θ(ψτ0) ifτ0:K0 ,C satisfiesτ0|M =τM.(7)

LetA:=Aσ/F be the simple abelian variety associated withσ=θ(ψ), which is determined uniquely up toF-isogeny. Suppose that

(2.6) ε 1/2, σEχ−10

=−1

As discussed in the introductions to [45] or [21], the condition (2.6) guaran- tees thatAcan be found as an isogeny factor of the Jacobian of a Shimura

(7)In the terminology of [21, 45],σis anM-rationalrepresentation.

(12)

curve over F; its endomorphism algebra End0A is a totally real field of dimensiond= dimA, which can be identified withM.

For any embedding τM: M ,C, we have L(s, στM) = L(s, ψτ0) for τ0: K ,C such that τ0|M = τM. The following consequences of this identity are proved in [23] (note that the CM type ofψτ0 is ΣE):

(1) Aacquires complex multiplication byKover some finite extension ofF, and in fact, as remarked before, a minimal such extension is KF =E;

(2) AEis isogenous to a sum of copies of the abelian varietyBψ\ defined above.

As M is contained in the maximal real subfield of K0, the dimension [M : Q] of AE divides the dimension [K0 :Q]/2 of Bψ, K0; hence in fact Bψ, K0 isK-linearly isogenous to a sum of copies ofAE, i.e. for somer>1,

(2.7) Bψ, K0A⊕rE .

2.3. Rankin–Selberg p-adicL-function

Moving to a more general context for this subsection only, let F be a totally real field,E a CM quadratic extension of F. LetM be a number field and letσbe anM-rational automorphic representation of ResF /QGL2

of parallel weight 2, with central characterω. LetMvbe ap-adic completion ofM, letL be a finite extension ofMv, and let

χ0: E×\EA×L× be a finite-order character satisfyingχ0|F×

A

=ω. (We will later specialise to the situationσ=θ(ψ) considered in Section 2.2). We recall the definition of ap-adic Rankin–SelbergL-function on YL attached to the base-change σE ofσto Etwisted byχ−10 .

Given a place ℘|p of F, we say that σ is nearly ordinary at with unit characters α if, after possibly enlarging L, there exist characters α:F×→OL×, such thatσ⊗Lis either specialα·St with characterα, or irreducible principal series Ind(|·|α, β) (un-normalised induction) for some other characterβ.

Theorem 2.2. — Suppose that for all℘|p, σ is nearly ordinary at ℘.

Then there is a function

Lp σEχ−10

∈Λ

(13)

characterised by the interpolation property Lp σEχ−10

0) =ep σιE⊗(χ0χ0)ι,−1

·L(p) 1/2, σEι ⊗(χ0χ0)ι,−1ισ

for all sufficiently p-ramified(8) finite order characters χ0: Γ → Q× and ι: Q,C. Here

ισ :=L(1, σι,ad) and ep σιE⊗(χ0χ0)ι,−1

=Y

℘|p

e σEι ⊗(χ0χ0)ι,−1 with

(2.8) e σEι ⊗(χ0χ0)ι,−1

=ε 0, ι(α−1χ0,pχ0p)

·ε 0, ι(α−1 χ0,pcχ0pc) . Proof. — This is essentially [21, Theorem A]. OurLpEχ−10 ) differs from the one of loc. cit. by the involution χ0 7→ χ0−1, the shiftχ−10 , and some algebraic constants. Regarding the interpolation factors, note that if χ0p,χ0pc are sufficiently ramified then all localL-values in the interpolation formula from [21] are equal to 1. The relation between the Gauß sums used in [21] and our epsilon factors (2.8) follows from e.g. [14, (23.6.2)].

2.4. Katz p-adic L-function

From now until the end of this paper, letK,E, ΣEbe as in Section 2.1.

Fix a p-adic place w of K, and denote byv be the induced place of the maximal real subfieldMK. We letQQpKw be algebraic closures ofK and of Kw, and letCp be the completion ofQp. We also letL be a sufficiently large finite extension ofKw insideQp as in the introduction.

2.4.1. p-adic CM type associated withw Let NΣ(w)

E,p: Ep×Kp×Kw× be the continuous extension of NΣE. We let

Σ(w)E :=

p|pprime of E:| ·

wNΣ(w)

E, p

E×p

is a non-trivial norm onEp×

,

which, by Lemma 2.1 and the construction ofNΣE, has the property that Σ(w)E(w)E cis the set of all primespofEabove p. Hence Σ(w)E is ap-adic CM type ofE, identified with a set of embeddingsE ,Qp.

(8)See the proof for the precise meaning.

(14)

Lemma 2.3. — Every prime ofF abovepsplits inE, and the CM type Σ(w)E is a p-adic CM type ofE.

Proof. — The first assertion is Lemma 2.1 part (2). The second assertion follows from Lemma 2.1 part (3), after noting that Σ(w)E = InfE/KΣp) for anyιp:E ,Qp inducing a prime in ΣE.

2.4.2. p-adic Hecke characters Assume thatLsplits E, and let

χ:E×\EA×L×

be a locally algebraicp-adic character. We say thatχis a Hecke character ofp-adic infinity typekZ[Hom(E, L)] if there exists an open subgroup UEA× such that

χ(t) = Y

σHom(E, L)

t−kσ σ

for tU. Note that this definition differs from the one in some of the literature (e.g. [27] and [25]) by a sign in the exponents; it agrees with [5].

If χis a locally algebraic character of p-adic infinity typek andι:LC is an embedding, we can define the ι-avatar χι: EA×C× similarly to [32, Definition 1.5]. The embeddingιinduces an isomorphism Hom(E, L)

→ Hom(E,C) by σ 7→ ισ; the infinity type kιZ[Hom(E,C)] of χι corresponds to k under this bijection. The association χχι defines a bijection between locally algebraic Hecke characters overE with values in Land arithmetic Hecke characters overE in the usual sense.

For example, if λis as in Section 2.1, the character λ(w)(x) :=λ(x)NΣ(w)

E, p(xp)−1:E×\EA×Kw×

is a Hecke character ofp-adic infinity type Σ(w)E .(9) The placewbeing fixed, in the rest of this paper we will often abuse notation by simply writingλ in place ofλ(w).

2.4.3. p-adicL-function

Let now L be an extension of Kw splitting E, and let ΣE be a p-adic CM type ofE over someL. LetE] be a finite extension of Econtained inEab, and let Γ]:= Gal(E] /E). Let Λ]:=Zp[[Γ]]]L,Y]:= Spec Λ].

(9)Strictly speaking this assertion holds after consideringλ(w)as valued in some exten- sionLKwsplittingE.

(15)

By [27, 30] and the first assertion of Lemma 2.3, there is an element LΣE ∈Λ]

uniquely characterised by the interpolation property that we now describe.

The domain of interpolation consists of locally algebraicp-adic Hecke char- actersλ0: Γ]Q×p with infinity type

(w)E +κ(1c) forkZ, κZ[Σ(w)E ] such that

(i) k>1, or

(ii) k61 and(w)E +κZ>0(w)E ].

The interpolation property is then the following. There exist explicitp-adic periods

ΣE = (ΩΣE,p)pΣEZ¯×pΣE

and, for each complex CM type ΣE,∞ofE, complex periodsΣE, = (ΩΣE,)τΣE,C×ΣE,∞

(both defined in [27, (4.4)]) such that for any characterλ0: Γ→Q×p in the domain of interpolation, and anyι:L(λ0),C, we have(10)

ι LΣE0) Ωk+2κΣ

E

!

=ep0)−1ι

· L(p) 0,((λ0)−1)ιk+2κΣ

E, ι,

·πκΓΣ(kΣE, ι+κ)

(=ϑ)κ · [OE×:OF×] p|DF| In the interpolation formula, ΣE,ιis the complex CM type induced from Σ(w)E viaι, and we then identifyκwithκιZ>0E,ι]; whenkZappears in the exponent of one of the periods ΩΣit is considered as k·P

τΣιEτ. Ifχ= (λ0)−1is ramified at all p|p, thep-Euler factor is given by

epι) = Y

pΣ(w)E

e(χιp)

for (dropping all superscriptsι)

(2.9) e(χp) = L(0, χp)

ε(0, χp)L 1, χ−1p

(10)Note that we are ignoring interpolation factors at places away fromp appearing elsewhere in the literature, since those, while non-integral, can be interpolated by poly- nomial functions onY].

(16)

Finally, ΓΣ(kΣE,ι+κ) =Q

τΣE, ιΓ(k+κτ) for the usual Γ-function, and ϑE as in [28, Section 3.1]. All local epsilon factors in this paper are understood with respect to some uniform choice of additive characters of Ep of level one for allp|p.

For a later consideration, we fix a sufficiently large extensionE]as above and consider the restriction ofLΣE to certain open subsets ofY]: ifλ0 is ap-adic Hecke character factoring through Γ] with values inL, and ΣE is ap-adic CM type, we define

LΣE, λ0 ∈Λ by

LΣE, λ00) :=LΣE0χ0).

We will henceforth drop the superscript w from the notation for the characterλ(w).

2.5. Factorisation of the Rankin–Selberg p-adic L-function

Letσ:=θ(ψ) as in Section 2.2. There is a factorisation (2.10) L s−1/2, σE⊗(χ0χ0)−1

=L s, ψ(χ0χ0)−1

L s, ψ0χ0)−1 of complex (more preciselyKC-valued)L-functions, valid for algebraic Hecke charactersχ0 overE. It implies the following factorisation of p-adic L-functions.

Lemma 2.4. — Let LpEχ−10 ) be thep-adicL-function associated withσ =θ(ψ) and the embeddingMMvKw, where wis the place ofKfixed above andv its restriction toM. LetLbe a finite extension of Kw splittingE. We have

(2.11) Lp σEχ−10 .

= LΣ

E, ψχ∗−10

p,ΣE

·LΣ

Ec, ψχ∗−10

p,ΣEc

inΛ = ΛL, where we use the symbol .

=to signify an equality which holds up to multiplication by a constant inQ×.

Proof. — We evaluate both sides of the proposed equality at finite order characters χ0 of Γ which are sufficiently ramified in the sense that, for all primes p|p of E, χp has conductor larger than the conductors of ψp

and χ0,p. This is sufficient as such characters are dense in Y (cf. [21, Lemma 10.2.1]).

(17)

Note first the self-duality relation

(2.12) λ0∗=λ0−1| · |−1A

E

(where| · |=| · |AE), valid for bothλ0 =ψχ−10 andλ0 =ψχ∗−10 (this follows from (2.5)). Evaluating (2.10) ats= 1, we find

L 1/2, σE⊗(χ0χ0)−1

=L 0, ψ| · |(χ0χ0)−1

L 0, ψ| · |(χ0χ0)−1

=L 0,(ψχ∗−10 χ0)−1

L(0, ψχ∗−10 χ0)−1 . Therefore the L-values agree with the ones being interpolated by the p-adicL-functions in (2.11). We now compare the local Euler-like interpo- lation factors and the complex periods.

Recall from e.g. [26, p. 119] that, for OE =ppc, we have σ'π(ψp, ψpc)

By the construction of Σ(w)E and the Shimura–Taniyama formula for Hecke characters (see [18, Proposition A.4.7.4 (ii)], cf. also the paragraph after Example A 4.8.3 ibid.), the characterψp has values inw-adic units if and only ifp∈/ Σ(w)E , equivalentlyp∈Σ(w)E c.

Denoting by a fixed prime ofF abovepand byp the unique prime in Σ(w)E above℘, it follows thatα=ψpc under the identificationEpc =F. Then, under our assumption on the ramification ofχ0, we have

(2.13) e σEχ−10 , χ0

=ε 0, ψp−1c χ0,pχ0p

·ε 0, ψ−1pcχ0,pcχ0pc

whereas the Katz interpolation factors aboveare ε 0, ψ−1p χ0,pcχ0p−1−1

·ε 0, ψ−1p χ0,pχ0pc−1−1

. By the functional equation

ε(s, χ)−1=ε(1s, χ−1)χ(−1)

valid for any character χ of a local field (e.g. [14, (23.4.2)]) and the self- dualities (2.12), these equal

ε 0,| · |ψpχ−10,pcχ0p

·ε 0,| · |ψpχ−10,pχ0pc

=ε 0, ψp−1cχ0,pχ0p

·ε 0, ψ−1pc χ0,pcχ0pc

matching (2.13).

In regard to periods, we first note that the periods in the asserted equality are independent ofχ0. As

Ad(σ)'η⊕IndFE ψ(ψ)−1 ,

(18)

we have

L(1, σι,ad) =L(1, η)L 1, ψ(ψ)−1

=L(1, η)L 0,(ψ(ψ)−1)D The infinity type ofι(ψ(ψ)−1)Dis 2ΣιE. From the algebraicity of Hecke L-values due to Shimura, we have

L 0,(ψ(ψ)−1)D .

= Ω2Σι E

(see [40] and [27, Section 4], especially [27, pp. 215–16]). Moreover, we have a period relation

1Σι E

= Ω. 1Σι E◦c

(see [41] and [42, Theorem. 32.5]).

It follows that

ισ .

= Ω2Σι E

= Ω. Σι

EΣι

E◦c.

2.6. Construction of an auxiliary character

We will now look for a characterχ0 suitable for our purposes. If a Hecke character λ0 of E×A satisfies (2.12), then its functional equation relates L(s, λ0) with L(1s, λ0−1) = L(2s, λ0∗) = L(2s, λ0); the sign of this functional equation is the root number

w(λ0) :=ε(1, λ0)∈ {±1}.

We say that finite-order character χ:E×\EA×Q× isanticyclotomic if it satisfies the following two conditions, which are equivalent by [24, Lemma 5.31]:

(1) χ=χ−1;

(2) there exists a finite-order characterχ0:E×\EA×Q× such that

(2.14) χ=χ00.

Lemma 2.5. — Let λ be a Hecke character satisfying (2.12). Suppose that the extension E/F is ramified. Then there exist an anticyclotomic finite-order characterχ=χ00: E×\EA×Q× such that the root num- ber

w(λχ) = +1.

(19)

Proof. — Suppose first thatλsatisfies the following condition. (We will later reduce to this case.)

(∗) there is a primeofE, ramified overF, such that ord(C) is odd, where C is the conductor of λ. In particular, the norm idealNE/F(C) is not a square. For a quadratic characterχ0 overF, letχ0E=χ0NE/F be the corresponding Hecke character overE. By definition,χ0E is a quadratic Hecke character overE and also anticyclotomic. For the latter, note that

χ0E(a)χ0∗E(a) =χ0 NE/F(a)

χ0 NE/F(c(a))

=χ0 NE/F(a)2

= 1.

We consider twists ofλby characters of the form χ0E with the conductor of χ0E prime to C. Recall that the twist of a self-dual character by an anticyclotomic character is again self-dual. To prove existence of twist with change in the root number, it thus suffices to show thatχ0 can be chosen so thatχ0(NE/F(C)) takes value 1 or−1. The sufficiency follows from the explicit root number formula for the twistλχ0Ein [44, (3.4.6)]. As the norm idealNE/F(C) is not a square, the existence of desiredχ0 follows readily.

To reduce to condition (∗), it suffices, given λ, to find λ0 = λχ11 satisfying (∗). Letbe a prime ofE ramified inE/F and letδ:= ord(2).

Letr be an odd integer greater thanδ+ 2 and the exponent of in the conductor ofλ. Letχ1 be a finite order character ofEA×/E×such that the exponent of in the conductor of χ1 is exactly rδ. As (1 +℘t−δOE)2

= 1 +tOE for all t>δ+ 1, the conductor of χ21,℘ is exactly r. Letting χ =χ11, and denoting by$ a uniformiser at ℘, for anyt > δ+ 1 we have for anyt>(r−δ)/2:

χ 1 +$ta

=χ1,℘ 1 +$ta

χ1,℘ 1−$ta−1

=χ1, ℘ 1 +$ta2 . It follows that the conductor of χ is the same as the conductor of χ21, that is,r; by our choice ofrthe same is true ofλχ, and in particular λ0

satisfies (∗).

Remark 2.6. — Let χ = χ0χ∗−10 be as in the Lemma 2.5 and let ψ :=λχ0, whereλis as fixed in the Introduction. Thenψsatisfies (2.5); by the analogous formula to (2.10), σ := θ(ψ) has root number −1 (i.e., it satisfies (2.6)).

2.7. p-adic Gross–Zagier formula

We recall a formula relating Rankin–Selbergp-adicL-functions to points on abelian varieties; we will later deduce from it an analogous formula for

Références

Documents relatifs

On the other hand, an approach based on the Weil restriction process [17, 14, 2, 20] produced important results: taking as input a discrete logarithm problem in an elliptic

In the case of a power of the multiplicative group G = G d m , the transcendence result yields lower bounds for the p–adic rank of the units of an algebraic number field (namely

p-adic Eisenstein-Kronecker numbers We next give the definition of p-adic Eisenstein-Kronecker numbers, when the lattice Γ is the period lattice of an elliptic curve with

The polar quotient corresponding to branches of ri and the multiplicity of ri can be explicitly computed in terms of the minimal set of generators of the

In the case of a function field, however, this method does not work very well when the coefficient field is so large that the.. Mordell-Weil group of each fiber is no

Relational structures, ages, counting functions, oligomorphic groups, age algebra, Ramsey theorem, integral domain.. ∗ Research done under the auspices of Intas programme

Parmi tous ces patrons, quels sont ceux qui permettent de construire le prisme ci-contre :.. E XERCICE

The aim of this paper is to give a precise bound for the degree of the maximal torsion cosets (translates of abelian subvarieties by torsion points) that appear in Raynaud’s