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Let p be a prime number, F a finite extension of Qp, and GF the Galois group of Qp over F. We suppose that we are given a continuous p-adic representation (12) ρ: GFGL(V),

where V is a Qp-vector space of finite dimension d. As before, we write GV=ρ(GF). If we are to successfully apply the Lie algebra criteria of §2 to study the GV-cohomology of V, we must be able to construct elements in the Lie algebra

L(GV)Q

p=L(GV)

Qp

Qp.

The aim of this section is to take an important first step in this direction when V is a semistable Galois representation in the sense of Fontaine [14].

Let F0 denote the maximal unramified extension ofQp contained in F. We recall that V is said to be semistable if

D(V)=(Bst

QpV)GF

has dimension d over F0, where d=dimQ

p(V); here Bst is Fontaine’s ring for semistable representations (see [14]). Assume from now on that V is semistable. Then D(V) is a filtered (ϕ, N)-module in the sense of [13], [14]. We recall briefly the main properties of D(V). Firstly, D(V) is endowed with an F0-linear endomorphism N, called the monodromy operator. Recall that the representation is said to be crystalline if N=0. Secondly, D(V) is endowed with an isomorphism of additive groups ϕ : D(V) D(V), which is σ-linear in the sense that ϕ(av)=σ(a)ϕ(v) for a in F0 and v in D(V); here σ denotes the arithmetic Frobenius in the Galois group of F0

over Qp (i.e. σ operates on the residue field of F0 by raising to the p-th power). Let kF denote the residue field of F, and suppose that kF has cardinality q=pf. Hence

(13) Φ=ϕf

will be an F0-linear automorphism of D(V), and we shall refer to it as the Frobenius endomorphism associated to the filtered module. Recall that we have

NΦ=qΦN.

By definition, Φ is an automorphism of a vector space on which GF acts trivially. It is therefore somewhat surprising that we shall show, using the Tannakian formalism of [9] and an elementary fact about Fontaine’s theory for unramified representations, that Φ gives rise to interesting elements in the Lie algebra L(GV)Q

p of GV=ρ(GF) of our original Galois representation.

We recall the extension of the p-adic logarithm to the multiplicative group of Qp. Let O denote the ring of integers of Qp, O× the group of units of O, and m the maximal ideal of O. The usual series for logz converges on 1 +m. Let µ denote the group of all roots of unity of Qp of order prime to p. Then O ×=µ×(1 +m). We extend logz to O× by specifying that log(µ)=0. Now fix any non-zero element π of Qp whose absolute value is less than one. If x is any element of Qp×, we can write x=πay, where a Q and y O×. We then define logπ(x)= log( y). Note that this is well-defined as the ratio of any two such y must be a root of unity.

Theorem 3.1. — Assume that V is a semistable Galois representation, and let D(V) be the associated filtered (ϕ,N)-module. Let λ1, ...,λd denote the roots in Qp of the characteristic polynomial of the automorphism Φ=ϕf of D(V). Then there exists X in the Lie algebra L(GV)Q

p

ofGV=ρ(GF) such that the characteristic polynomial of X on VQ

p has roots logπ(λ1), ..., logπ(λd).

We will also need an analogue of this result for the Lie algebra L(HV)Q

p, where, as before, HV=GVSL(V). We recall from [13], [14] that the F-vector space D(V)F=F

F0D(V) is endowed with a canonical decreasing filtration FiliD(V)F (i Z) of F-subspaces such that FiliD(V)F=D(V)F for i sufficiently small and FiliD(V)F=0 for i sufficiently large. This filtration enables us to define the so called Hodge-Tate weights of D(V). These are a family of integers

(14) i16i26...6id,

which are defined as follows. Any integer h occurs in (14) if FilhD(V)F=| Filh+1D(V)F, and when h does occur its multiplicity in (14) is the F-dimension of the quotient FilhD(V)F/Filh+1D(V)F. We define

(15) t=

Xd

h= 1

ih.

Let det : GF Z×p denote the character of GF obtained by composing the representation ρ with the determinant map. We write ξ: GFZ×p for the cyclotomic character of GF, i.e. the character giving the action of GF on Tp(µ). As V is a semistable GF-module, it is known (see [14, Prop. 5.4.1]) that the restriction of det to the inertial subgroup IF is equal to the restriction of ξt to IF, where t is given by (15). Further,

thep-adic valuation of the determinant of Φ is equal to that of qt. If we set detΦ=qtu, with u F0 a unit, then det : GF Z×p is ηξt with η an unramified character and, moreover, η is of finite order if and only if u is a root of unity.

Theorem3.2. — Assume that Vis a semistable Galois representation, and that its determinant character det: GF Z×p coincides on an open subgroup of GF with ξt where ξ is the cyclotomic character, and t is given by (15). Let λ1, ...,λd denote the roots in Qp of the characteristic polynomial of the automorphism Φ=ϕf of D(V). Then there exists X in the Lie algebra L(HV)Q

p of HV=ρ(GF)SL(V) such that, for a suitable ordering of λ1, ...,λd, the roots of the characteristic polynomial of X on VQ

p are given by logπ(λ1qi1), ..., logπ(λdqid), where q=pf, and i1, ...,id

denote the Hodge-Tate weights (14).

Before embarking on the proof of these two theorems, we recall some basic definitions about algebraic groups, and the p-adic logarithms of their points. Let W be any finite dimensional vector space over some finite extension K of Qp. We write GLW for the general linear group of W, considered as an algebraic group over K.

Thus, for each finite extension M of K contained in Qp, the group GLW(M) of M-points of W is the group of M-automorphisms of W

KM. If J denotes any algebraic subgroup of GLW, we write L( J) for its Lie algebra, which coincides with the Lie algebra L( J(K) ) of the p-adic Lie subgroup J(K). Now take θ to be any element of GLW(K). We can write θ=su, where s is semisimple, u is unipotent, and s and u commute. As u is unipotent, some power of u−1 is zero, and so we can define log(u) by the usual series log(u)=Pn= 1(1)n1 (un1)n. We define logπ(s) as follows. We can write QpKW= Wi, where Wi is some subspace on which the semisimple element s acts via some eigenvalue αi. We then define logπ(s) to be the endomorphism of QpKW, which operates on Wi by logπ(αi). In fact, it is clear that if π belongs to K, logπ(s) belongs to the endomorphism ring of W over the original base field K. We finally define

logπ(θ)=logπ(s) + log(u).

The automorphism θ topologically generates a compact subgroup of GLW(K) if and only if its eigenvalues αi are units. If this is the case, then logπ(αi), and therefore logπ(θ), do not depend of the choice of the αi. In fact, we can define log(θ) in a more natural manner. Let r denote the cardinality of GLm(k), where m is the dimension of W over K, and k is the residue field of K, and put β=θr. Our hypothesis on θ shows that θ must stabilize a lattice in W, and so it is clear that the matrix A of β relative to a K-basis of W coming from this lattice must satisfy A 1 modπK, where πK is any

local parameter of K. We can then define log(θ)=1

r

X n= 1

(−1)n1(A1)n

n .

The following lemma is well-known (cf. [3, Chap. III, §7.6, Propositions 10 and 13]).

Lemma 3.3. — Let W be a finite dimensional vector space over K, where K is a finite extension of Qp, and let θ be any element of GLW(K). If θ topologically generates a compact subgroup of GLW(K), then logπ(θ)= log(θ). If J is any algebraic subgroup of GLW, and θ belongs to J(K), then logπ(θ) belongs to the Lie algebra L( J) of J.

Proof of Theorem 3.1. If H is any subgroup of GLV(Qp), we define Halg to be the Zariski closure of H in GLV i.e. the intersection of all algebraic subgroups J of GLV such that J is defined over Qp and J(Qp) contains H. As earlier, let IF denote the inertial subgroup of the Galois group GF. We put

GV=ρ(GF), IV=ρ(IF).

We then have the algebraic groups GalgV and IalgV in GLV, and we can consider the four Lie algebras L(GV), L(IV), L(GalgV ), L(IalgV ). By a basic result of Serre and Sen, [23], we have

(16) L(IV)=L(IalgV).

Hence we have the inclusions

(17) L(IalgV ) L(GV)L(GalgV ).

By definition, the image of the Galois representation ρ of GF is contained in GalgV (Qp).

Thus, for each representation α of the algebraic group GalgV in a finite dimensional Qp-vector space Vα, we obtain a new Galois representation:

(18) ρα: GF GalgV (Qp)GLVα(Qp)=GL(Vα).

The main idea of the proof of Theorem 3.1 is to work with this new Galois representation ρα for a suitable choice of α. We first note that, for every such α, the Galois representation ρα is also semistable. Indeed, it is known [9, Proposition 2.20] that the representation α of GalgV is a subquotient of a finite direct sum of copies of tensor products of the tautological representation of GalgV and its dual. But it is also known that the category of semistable representations of GF is stable under the Tannakian operations in the category of finite dimensional p-adic representations of GF and so ρα must be semistable, because ρ is semistable. For simplicity, we write Dα

for the filtered (ϕ, N)-module associated with ρα. In general, we write a subscript α on each object associated with the original representation ρ to denote the corresponding object attached to ρα.

We put GVα=ρα(GF). The algebraic groups IalgV , GalgV clearly act on Vα, and we denote the images of these groups in GLVα by IalgVα, GalgVα, respectively.

For the rest of the proof, we fix the following representation of GalgV . As IalgV is clearly normal in GalgV , there exists a representation α0 of GalgV in GLVα0 whose kernel is precisely IalgV . For simplicity, we write V0 instead of Vα0, ρ0 instead of ρα0, and so on for all objects attached to the representation ρα0. We write Fr for the arithmetic Frobenius in GF/IF. Thus ρ0(Fr) topologically generates GV0=ρ0(GF). Hence the Lie algebra L(GV0) of GV0 is the one dimensional Qp-subspace of End (V0) generated by log(ρ0(Fr) ); note that log(ρ0(Fr) ) is defined as explained earlier because ρ0(Fr) generates a compact group. Clearly GalgV0 is the smallest algebraic subgroup of GLV0 containing ρ0(Fr), and is abelian. Let π : L(GalgV ) L(GalgV0) denote the natural surjection. Since L(IalgV )=L(IV), we evidently have

(19) L(GV)=π1(L(GV0) ).

There are two basic steps in the proof of Theorem 3.1. The first uses all the representations α of GalgV to construct, via the Tannakian formalism, an element in the Lie algebra L(GalgV )Q

p having the same eigenvalues as the endomorphism logπ(Φ) of D(V). The second step exploits the unramified Galois representation ρ0 arising from α0 to show, using Fontaine’s theory in the modest case of unramified Galois representations, together with the key fact (19), the existence of the desired element X in L(GV)Q

p.

We now give the first step. Denote by Rep(GalgV ) (respectively, Rep(GalgVα) ) the category of all finite dimensional Qp-representations of the algebraic group GalgV (respectively, GalgVα). Since α gives rise to a homomorphism from GalgV to GalgVα, we can identify Rep(GalgVα) with a sub-category of Rep(GalgV ). We refer to [9] for the following basic facts about Tannakian categories and their associated formalism. We note that Rep(GalgV ) is a Tannakian category, and that Rep(GalgVα) is a sub-Tannakian category. Let VecF

0 denote the category of all finite dimensional vector spaces over the field F0. We have two fibre functors over F0,

ωG: Rep(GalgV )VecF

0, ωD: Rep(GalgV )VecF

0

which are defined by ωG(α)=Vα

QpF0, ωD(α)=Dα;

we recall that Dα is the filtered (ϕ, N)-module attached by Fontaine’s theory to the semistable Galois representation ρα. It is proven in [9, Proposition 2.8] that we can identify GalgVα over F0 with the group of ⊗-automorphisms of ωG restricted to the sub-category Rep(GalgVα) of Rep(GalgV ). We define GalgD to be the algebraic group of

⊗-automorphisms of the fibre functor ωD. Let GalgDα denote the algebraic group of

⊗-automorphisms of ωD restricted to the sub-category Rep(GalgVα). Both GalgD and GalgDα are defined over F0, and GalgDα is the image of GalgD in GLDα.

Write =s for the affine algebraic variety of ⊗-isomorphisms from ωD to ωG, and

=sα for the variety of ⊗-isomorphisms from ωD and ωG restricted to Rep(GalgVα). The variety =sα is a right torsor under GalgDα, and a left torsor under GalgVα. Now the choice of a point i in =s(Qp) gives, for each α, a point iα in =sα(Qp). This point iα gives rise to an isomorphism

(20) ηiα : Dα

F0Qp'(Vα)Q

p=Vα

QpQp which induces an isomorphism of algebraic groups

GalgDα×

F0Qp' GalgVα×

QpQp and an isomorphism of Lie algebras

L(GalgDα)

F0Qp'L(GalgVα)Q

p.

Moreover, a different choice of the point i has the effect of changing these two isomorphisms by an inner automorphism of GalgDα(Qp) or an inner automorphism of GalgVα(Qp).

For each α in Rep(GalgV ), we recall that the associated Galois representation ρα

is semistable, and that the filtered (ϕ, N)-module Dα attached to ρα has the F0 -auto-morphism Φα=ϕαf. Thus the family of all Φα define an automorphism of the functor ωD, and so we obtain a canonical element of GalgD(F0), which we again denote by Φ. Recalling the definition of logπ(Φ) given earlier, it follows that it belongs to the Lie algebra L(GalgD) of the algebraic group GalgD. Now fix any point i in =s(Qp), and let ηi

denote the isomorphism (20) for the tautological representation of GalgV in GLV. We define the endomorphism Xi of VQ

p by

(21) Xi=ηilogπ(Φ)ηi 1.

As logπ(Φ) belongs to L(GalgD), it follows that Xi belongs to L(GalgD)Q

p. Moreover, if λ1, ...,λd denote the eigenvalues of Φ with multiplicities, it is clear that the eigenvalues

of Xi with multiplicities are logπ(λ1), ..., logπ(λd). This construction of Xi completes the first basic step in the proof of Theorem 3.1.

To finish the proof of Theorem 3.1, we must show that Xi belongs to the Lie subalgebra L(GV)Q

p of L(GalgV )Q

p. Here we make use of the representation α0 of GalgV . Let L(α0) be the map from L(GalgV )Q

p to L(GLV0)Q

p induced by α0. In view of (19), it suffices to show that

(22) L(α0)(Xi)L(GV0)Q

p.

Let i0 denote the point in =sα0(Qp) arising from i. We have (23) L(α0)(Xi)=ηi0 logπ(Φ0)ηi01,

whereΦ0=ϕ0f comes from the filtered (ϕ, N)-module D0. Since the representation ρ0 of GF is unramified, it is well-known that Φ0 fixes a lattice (see [13]). Hence Φ0 generates a compact subgroup of GLD0(F0). Thus logπ(Φ0)= log(Φ0) is independent of the choice of π. Moreover, GV0 is topologically generated byρ0(Fr), and so GalgV0 is abelian, whence GalgD0×

F0Qp is also abelian. In view of the remark made earlier, we see that the right hand side of (23) does not depend on the choice of i in =s(Qp) nor on the choice of π. In fact, we see that the right hand side of (23) is the same for any choice of i0

in =sα0(M), where M is any extension field of F0. We now make a suitable choice of M and i0, which will enable us to compute explicitly the right hand side of (23).

We will use the following lemma about Fontaine’s theory for arbitrary unramified Galois representations ψ : GF GL(W), where W is a Qp-vector space of finite dimension. Let K denote the maximal unramified extension of Qp, and write K forb the completion of K. In the following, GF acts on Kb

QpW by τ(a⊗w)=τ(a)τ(w) for a in K andb w in W.

Lemma 3.4. — Assume that the Galois representation ψ is unramified. Consider the F0 -subspace of Kb

QpW given by U=(Kb

QpW)GF. Then W is crystalline in the sense of Fontaine [13], [14] and the associated filtered (ϕ,N)-module is D(W)=U. Moreover, the F0-automorphism ΦW=ϕWf of D(W) is given by

(24) βΦWβ1=ψ(Fr1),

where Fr is the arithmetic Frobenius in GF/IF, and β : Kb

F0U' Kb

QpW is the isomorphism obtained by extending scalars on the F0-subspace U of W.

Proof. The fact that β is an isomorphism is, of course, not obvious, and we refer to the Appendix of Chapter 3 of [25] for a proof. Also, K is naturally includedb in Fontaine’s ring Bcris, and so U is an F0-subspace of D(W) (see [13], [14]). But the fact that β is an isomorphism shows that the F0-dimension of U must be equal to the Qp-dimension of W, and hence D(W)=U. Let ϕB denote the action of Frobenius on the Fontaine ring Bcris (see [13], [14]). We write σ for the arithmetic Frobenius in the Galois group of K over Qp. The restriction of ϕB to K is the arithmetic Frobeniusb σ. Let 1W denote the identity map of W. By definition, ϕW is the restriction to U of the map σ

Qp1W. Hence the σ-linear extension σ

QpϕW of ϕW to Kb

F0U satisfies β(σ

F0ϕW)β1=σ

Qp1W.

Raising both sides to the power f and extending ΦW linearly to the whole of Kb

F0U, we conclude that

(25) β(σf

F01U)ΦWβ1=σf

Qp1W.

As the restriction to K of the action of Gb F on Bcris is the usual action, U is the F0-subspace of Kb

QpW fixed by the σf-linear extension of ψ(Fr) to Kb

QpW. Extending ψ(Fr) linearly to Kb

QpW, it follows that (26) β(σf

F01U)β1=(σf

Qp1W)ψ(Fr).

The equation (24) follows on comparing (25) and (26). This completes the proof of Lemma 3.4.

We can at last complete the proof of Theorem 3.1. We apply Lemma 3.4 to the unramified Galois representation ρ0 of GF in V0. We have the isomorphism

(27) β0:Kb

F0D0 'Kb

QpV0,

and the analogous isomorphisms for all the unramified Galois representations in the Tannakian category generated by ρ0. Thus these isomorphisms define a point i0 in

=s0(K). On applying log to both sides of (24), we deduce from (23) thatb (28) L(α0)(Xi)=logρ0(Fr1).

As the right hand side of (28) is clearly an element of L(GV0), the proof of Theorem 3.1 now follows from (19).

We shall need the following lemma for the proof of Theorem 3.2. Recall that ξ : GF Z×p is the cyclotomic character.

Lemma 3.5. — Assume that V is a semistable representation, and let det : GF Z×p be its determinant character. Then the following statements are equivalent:

(i) The map det coincides on an open subgroup of GF with ξt, where t is given by (15).

(ii) If δ=δ(Φ) denotes the determinant of the endomorphism Φ=ϕf of D(V), then (29) logπ(δ)=logπ(qt), where q=pf.

In particular, when t=|0, these equivalent assertions imply that the image of det is infinite.

Proof. Recall that d is the Qp-dimension of V, and put W=(ΛdV)(t). As the restriction of the determinant character of GF to IF is equal to ξt, we see that W is an unramified representation of GF of dimension 1 over Qp. Let ψ : GF Q×p denote the character giving the action of GF on W. We can compute ΦW in terms of δ as follows. We have that D(W)=Z[−t], where Z=ΛdD(V), and Z[−t] means that the automorphism ΦZ of Z is replaced by the automorphism qtΦZ. Hence ΦW is multiplication by δ.qt, and we recall that δ.qt is a p-adic unit. Now assertion (i) is equivalent to saying that GF/IF acts on W via a finite quotient. Hence the arithmetic Frobenius Fr in GF/IF must act on W via a root of unity, and therefore we have ψ(Fr)n=1 for some integer n. Applying Lemma 3.4 to W, we conclude that ΦnW=1.

Hence (i) is equivalent to δ.qt=ζ,

for some n-th root of unity ζ. The lemma is now obvious as logπ(ζ)=0.

Proof of Theorem 3.2. Assume now that the hypotheses of Theorem 3.2 hold for V. Thenλ1, ...,λd=δ, where δis the determinant ofΦ. By Theorem 3.1, there exists an element X in L(GV)Q

p, whose characteristic polynomial has roots logπ(λ1), ..., logπ(λd).

Recall that HV=GV SL(V), so that L(HV)Q

p consists of the elements of L(GV)Q

p of trace zero. But, by Lemma 3.5,

(30) tr(X)= Σd

i= 1

logπ(λi)= logπ(qt).

Hence, ast= Σd

i= 1

ij, it suffices to find another element Y in L(GV)Q

p, whose characteristic polynomial has roots

(31) logπ(λ1qi1), ..., logπ(λdqid),

for a suitable ordering of λ1, ...,λd. Since V is semistable, it is of Hodge-Tate type (see [28,§2]), and we now exploit this fact. Let C denote the completion ofQp. We consider VC=CQpV, endowed with the semilinear action of GF given byτ(c⊗v)=τ(c)τ(v) for all τ in GF, c in C, and v in V. For each m in Z, we write VC{m} for the F-subspace of VC consisting of all v such that τ(v)=ξm(τ)v for τ in GF. Put VC(m)=CFVC{m}, again endowed with the semilinear action of GF. To say that V is of Hodge-Tate type means that we have a direct sum decomposition

(32) VC=

mJVC(m),

where J is some finite set of integers. It is well-known [13], [14, Theorem 3.8] that the integers in J are the negatives of the distinct integers occuring in the sequence of Hodge-Tate weights (14), and that the C-dimension of VC(m) is equal to the F-dimension of FilmD(V)F/Film+1D(V)F. Moreover, the direct sum decomposition (32) allows us to define a homomorphism

(33) µ : Gm IalgV ×

QpC

of algebraic groups over C, where, for c C×, µ(c) is the automorphism of VC given by the formula

µ(c)(x)=cmx for all x in VC(m) (mJ).

As is explained in [28, §1.5], the image of µ is contained in IalgV ×QpC.

As in the proof of Theorem 3.1, let =s denote the affine algebraic variety of

⊗-isomorphisms from the fibre functor ωD to the fibre functor ωG. Again, we fix a point i in =s(Qp), and we write ηi for the isomorphism (20), when α is taken to be the tautological representation of GalgV in GLV. Put

(34) =ηiΦηi 1,

where Φ is given by (13). Thus belongs to GalgV (Qp). Now it is well-known [2, Theorem 4.4] that there then exist commuting elements s and u in GalgV (Qp) such that s is semisimple, u is unipotent, and

(35) =su=us.

Let Θ be the smallest algebraic subgroup (over Qp) which contains s. As s is semisimple, Θ is a multiplicative group (see [10, Chap. IV, §3]). Let Θ0 be the connected component of Θ so that Θ=Θ0×P, where P is a finite group. Suppose that F0 is a finite extension of F such that the residue field extension has degree a multiple of #P. Passing to the extension F0 and working with the Φ and s associated to F0, we may clearly assume that the multiplicative group Θ is a torus.

Let T denote a maximal torus in GalgV ×QpQp containing the torus Θ. Returning to our homomorphism µ coming from p-adic Hodge theory, we choose a maximal torus in GalgV ×Qp C containing the image of µ. But all maximal tori in GalgV ×Qp C are conjugate [B, Prop. 11.3], and so there exists g in GalgV (C) such that µ0=gµg1 has image in T. Moreover, the induced map µ0 : Gm T is necessarily defined over Qp (see [2, Proposition 8.11]). Hence µ0(q) belongs to T(Qp).

We recall that we are seeking to construct an element in the Lie algebra L(GV)Q

p, whose characteristic polynomial has the roots (31). To complete the proof, we use once more the representation α0 of GalgV in GLV0, whose kernel is precisely IalgV. The torus T acts on GalgV ×Qp Qp and its normal subgroup IalgV ×QpQp by inner automorphisms, and so also on the quotient GalgV0×QpQp. As GalgV0×QpQp is abelian, T acts trivially on it by inner automorphisms. Given an algebraic group M over Qp, let MQ

p=M×QpQp denote its extension to Qp. For an algebraic group H defined over Qp we write Hu for its unipotent radical [2, §11.21] and L(H)u for the corresponding Lie algebra. Now we have the exact sequence of Lie algebras over Qp

0L( (IalgV )Q

p)uL( (GalgV )Q

p)uL( (GalgV0)Q

p)u0

[2, Cor. 14.11]. The action of T on the algebraic groups induces the adjoint action of T on the Lie algebras. We denote with the superscript T the maximal Lie subalgebras on which T acts trivially. Then, since representations of a torus are semisimple, we have the exact sequence

(36) 0L( (IalgV )Q

p)Tu L( (GalgV )Q

p)Tu L( (GalgV0)Q

p)u0.

Here we have used the fact that T acts trivially on the Lie algebra L( (GalgV0)Q

p)u, as GV0 is abelian. Let u0 be the image of u in (GalgV0)Q

p and let n0 be an element in L( (GalgV )Q

p)Tu which is a lift of log(u0). Consider the element u0=exp(n0); clearly u0 commutes with elements of T. In particular, we have now arranged that the elements µ0(q), s and u0 commute. It is plain that the roots of the characteristic polynomial of

Y= logπ(s.µ0(q).u0)

are as in (31). As X and Y have the same image in L(GalgV0)Q

p, by Theorem 3.1 and

p, by Theorem 3.1 and

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