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2. METODOLOGÍA

2.1. Componentes del robot

2.1.1. Placa base

integers of the division fields of F in the “Kummer” case, that is, considering

K(F[πm+r]) as an extension ofK(F[πr]) for integersr m 1. Use the notation

M = K(F[πr]) and N = K(F[πm+r]), so that N/M is a Galois extension with group isomorphic to F[πm]. Specifically, we fix a primitive πm+r-torsion point α and define ψ : Γ = Gal(N/M) → F[πm] by ψ(γ) = γ(α)

F α. This map is an

isomorphism known as the Kummer isomorphism. In [CNT, Ch. X], the authors consider the ring of integersON as an additive Γ-module. They determine that the associated order of this module inside MΓ is

AN/M =OM + qm2

X

i=0

where σi = π1m

P

γ∈Γψ(γ)

i(γ1).

We would like to make a comparison between their associated order and the elements of AF(N) described in Theorems 10.1 and 10.2. An obstacle to this com-

parison is that while the Galois module OM can use ON as its ring of scalars, a Lubin-Tate formal group only admits scalar multiplication by OK. Therefore we will compute the intersection of AN/M with KΓ.

Proposition 10.3. The intersection of AN/M with KΓ is generated as an OKΓ- module by τi = πm1−i

P

γ∈Hiγ for i= 0, . . . , m−1, where Hi = Gal(N/K([π

i+r])).

Proof. It is clear that τi ∈ KΓ for all i. Next we show that τi ∈ AN/M. Let

Mi =NHi, so thatM =M0 ⊂M1 ⊂ · · · ⊂Mm =N. Then we have AN/M ∩KΓ =

AN/M0 ∩KΓ ⊇ AN/M1 ∩KΓ ⊇ · · · ⊇AN/Mm ∩KΓ = OK. By Cassou-Nogu`es and

Taylor’s result, τi is an element of AN/Mm−i (it is the σ0 generator).

To finish the proof, we show that if φ is any element of AN/M ∩KΓ then the coefficients of the elements of Hi−Hi+1 ⊂Γ agree up to an element ofOK.

Ifθ ∈ Gal(M/K) then it restricts to an automorphism of F[πm]. Let θ

∗ be the

automorphism of Γ such that θ ◦ψ = ψ ◦θ∗. Using the correspondence between

θ and θ∗, the Galois group of M/K can act on φ ∈ MΓ in two ways—write θ·φ

for θ acting on the coefficients of φ and φθ for the action on elements of Γ via

θ−1

∗ . One checks that these two actions agree on σi for all i. Now if we act on

φ ∈AN/M∩KΓ we are guaranteed to have invariance under the left action because

θ fixes K. If we let φ =a+Pqm−2

i, we have φθφ=φθθ·φ=aθ(a)∈ O

M, that is, φθ−φ∈ OM∩KΓ =OK. This proves the above claim, for we note that, since Gal(M/K) acts transitively on the set of primitive πi-torsion points, the θ

∗ act transitively on Hi −Hi+1 for i= 0, . . . , m−1.

The π2-torsion field, the subject of Theorem 10.1, is an instance of a Kummer

tower withr=m= 1. WithN =K(F[π2]) andM =K(F[π]), the proposition says thatAN/M∩KΓ is generated overOKΓ byτ0 =π−1

P

γ∈Γγ. This means that, if the

same eigenspace decomposition from Section 7.1 is applied to the additive Galois module ON, this τ0 will lie in the associated order of every eigenspace. However, for the points of F in ON, we have seen in the previous two sections that while τ0

does indeed lie in the associated order of F(m)(r) for r = 2, . . . , q2, the same is

not true for r = q. We have found by computation of examples that τ0 may fail to be in the associated order of F(m)(q−1), but as yet we do not have a proof of a

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