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Hilbert's Theorem 90

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cohomology

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Idea

A theorem in Galois cohomology due to David Hilbert.

Statement

There are actually two versions of Hilbert’s theorem 90, one multiplicative and the other additive. We begin with the multiplicative version.

Theorem

(Hilbert) Suppose K be a finite Galois extension of a field k, with a cyclic Galois group G=g of order n. Regard the multiplicative group K * as a G-module. Then the group cohomology of G with coefficients in K * – the Galois cohomology – satisfies

H 1(G,K *)=0.H^1(G, K^\ast) = 0 \,.

Before embarking on the proof, we recall from the article projective resolution that if G=C n is a finite cyclic group of order n, then there is a projective resolution of as trivial G-module:

NGDGNGDG0\ldots \stackrel{N}{\to} \mathbb{Z}G \stackrel{D}{\to} \mathbb{Z}G \stackrel{N}{\to} \mathbb{Z}G \stackrel{D}{\to} \mathbb{Z}G \to \mathbb{Z} \to 0

where the map G is induced from the trivial group homomorphism G1 (hence is the map that forms the sum of all coefficients of all group elements), and where D, N are multiplication by special elements in G, also denoted D, N:

Dg1,D \coloneqq g - 1,
\,
N1+g+g 2++g k1N \coloneqq 1 + g + g^2 + \ldots + g^{k-1}

The calculations in the proof that follows implicitly refer to this resolution as a means to defining H n(G,A) (in the case A=K *), by taking cohomology of the induced cochain complex

0hom G(,A)hom G(G,A)hom G(G,A)0 \to \hom_{\mathbb{Z}G}(\mathbb{Z}, A) \to \hom_{\mathbb{Z}G}(\mathbb{Z}G, A) \to \hom_{\mathbb{Z}G}(\mathbb{Z}G, A) \to \ldots
Proof

Let σG be an element of the group algebra, and denote the action of σ on an element βK by exponential notation β σ. The action of the element NG is

β N=β 1+g++g n1=ββ gβ g n1\beta^N = \beta^{1 + g + \ldots + g^{n-1}} = \beta \cdot \beta^g \cdot \ldots \beta^{g^{n-1}}

which is precisely the norm N(β). We are to show that if N(β)=1, then there exists αK such that β=α/g(α).

By lemma 1 below, the homomorphisms 1,g,,g n1:K *K * are, when considered as elements in a vector space of K-valued functions, K-linearly independent. It follows in particular that

1+βg+β 1+gg 2++β 1+g++g n2g n11 + \beta g + \beta^{1+g}g^2 + \ldots + \beta^{1 + g + \ldots + g^{n-2}}g^{n-1}

is not identically zero, and therefore there exists θK * such that the element

α=θ+βθ g+β 1+gθ g 2++β 1+g++g n2θ g n1\alpha = \theta + \beta \theta^g + \beta^{1+g}\theta^{g^2} + \ldots + \beta^{1 + g + \ldots + g^{n-2}}\theta^{g^{n-1}}

is non-zero. Using the fact that N(β)=1, one may easily calculate that βα g=α, as was to be shown.

Now we give the additive version of Hilbert’s theorem 90:

Theorem

Under the same hypotheses given in 1, and regarding the additive group K as a G-module, we have

H 1(G,K)=0.H^1(G, K) = 0 \,.

The trace of an element αK is defined by

Tr(α)Nα=α+g(α)++g n1(α).Tr(\alpha) \coloneqq N \cdot \alpha = \alpha + g(\alpha) + \ldots + g^{n-1}(\alpha).

We want to show that if Tr(β)=0, then there exists αK such that β=αg(α). By the theorem on linear independence of characters (following section), there exists θ such that Tr(θ)0; notice Tr(θ) belongs to the ground field k since gN=N. Put

α1Tr(θ)(βg(θ)+(β+g(β))g 2(θ)++(β+g(β)++g n2(β))g n1(θ).\alpha \coloneqq \frac1{Tr(\theta)}(\beta g(\theta) + (\beta + g(\beta))g^2(\theta) + \ldots + (\beta + g(\beta) + \ldots + g^{n-2}(\beta))g^{n-1}(\theta).

One may then calculate that

αg(α) = 1Tr(θ)(βg(θ)+βg 2(θ)++βg n1(θ)(g(β)++g n1(β))θ = 1Tr(θ)(βg(θ)+βg 2(θ)++βg n1(θ)+βθ) = β\array{ \alpha - g(\alpha) & = & \frac1{Tr(\theta)}(\beta g(\theta) + \beta g^2(\theta) + \ldots + \beta g^{n-1}(\theta) - (g(\beta) + \ldots + g^{n-1}(\beta))\theta \\ & = & \frac1{Tr(\theta)}(\beta g(\theta) + \beta g^2(\theta) + \ldots + \beta g^{n-1}(\theta) + \beta \theta) \\ & = & \beta }

where in the second line we used Tr(β)=0.

Independence of characters

The next result may be thought of as establishing “independence of characters” (where “characters” are valued in the multiplicative group of a field):

Lemma

Let K be a field, let G be a monoid, and let χ 1,,χ n:GK * be distinct monoid homomorphisms. Then the functions χ i, considered as functions valued in K, are K-linearly independent.

Proof

A single χ:GK * obviously forms a linearly independent set. Now suppose we have an equation

(1)a 1χ 1++a nχ n=0a_1 \chi_1 + \ldots + a_n \chi_n = 0

where a iK, and assume n is as small as possible. In particular, no a i is equal to 0, and n2. Choose gG such that χ 1(g)χ 2(g). Then for all hG we have

a 1χ 1(gh)++a nχ n(gh)=0a_1 \chi_1(g h) + \ldots + a_n \chi_n(g h) = 0

so that

(2)a 1χ 1(g)χ 1++a nχ n(g)χ n=0.a_1 \chi_1(g) \chi_1 + \ldots + a_n \chi_n(g)\chi_n = 0.

Dividing equation 2 by χ 1(g) and subtracting from it equation 1, the first term cancels, and we are left with a shorter relation

(a 2χ 2(g)χ 1(g)a 2)χ 2+=0(a_2\frac{\chi_2(g)}{\chi_1(g)} - a_2)\chi_2 + \ldots = 0

which is a contradiction.

A corollary of this result is an important result in its own right, the normal basis heorem.

(Will write this out later. I am puzzled that all the proofs I’ve so far looked at involve determinants. What happened to the battle cry, “Down with determinanats!”?)

  • Kummer theory?

References

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Revised on November 13, 2012 23:39:52 by Yaron Shany? (46.116.151.24)