In mathematics, the fundamental theorem of Galois theory is a result that describes the structure of certain types of field extensions in relation to groups. It was proved by Évariste Galois in his development of Galois theory.
In its most basic form, the theorem asserts that given a field extension E/F that is finite and Galois, there is a one-to-one correspondence between its intermediate fields and subgroups of its Galois group. (Intermediate fields are fields K satisfying F ⊆ K ⊆ E; they are also called subextensions of E/F.)
For finite extensions, the correspondence can be described explicitly as follows.
The fundamental theorem says that this correspondence is a one-to-one correspondence if (and only if) E/F is a Galois extension.For example, the topmost field E corresponds to the trivial subgroup of Gal(E/F), and the base field F corresponds to the whole group Gal(E/F).
The notation Gal(E/F) is only used for Galois extensions. If E/F is Galois, then Gal(E/F) = Aut(E/F). If E/F is not Galois, then the "correspondence" gives only an injective (but not surjective) map from
\{subgroupsofAut(E/F)\}
\{subfieldsofE/F\}
The correspondence has the following useful properties.
Consider the field
K=\Q\left(\sqrt{2},\sqrt{3}\right)=\left[\Q(\sqrt{2})\right](\sqrt{3}).
Since is constructed from the base field
Q
(a+b\sqrt{2})+(c+d\sqrt{2})\sqrt{3}, a,b,c,d\in\Q.
Its Galois group
G=Gal(K/\Q)
f\left((a+b\sqrt{2})+(c+d\sqrt{2})\sqrt{3}\right)=(a-b\sqrt{2})+(c-d\sqrt{2})\sqrt{3}=a-b\sqrt{2}+c\sqrt{3}-d\sqrt{6},
and exchanges and, so
g\left((a+b\sqrt{2})+(c+d\sqrt{2})\sqrt{3}\right)=(a+b\sqrt{2})-(c+d\sqrt{2})\sqrt{3}=a+b\sqrt{2}-c\sqrt{3}-d\sqrt{6}.
These are clearly automorphisms of, respecting its addition and multiplication. There is also the identity automorphism which fixes each element, and the composition of and which changes the signs on both radicals:
(fg)\left((a+b\sqrt{2})+(c+d\sqrt{2})\sqrt{3}\right)=(a-b\sqrt{2})-(c-d\sqrt{2})\sqrt{3}=a-b\sqrt{2}-c\sqrt{3}+d\sqrt{6}.
Since the order of the Galois group is equal to the degree of the field extension,
|G|=[K:Q]=4
G=\left\{1,f,g,fg\right\},
which is isomorphic to the Klein four-group. Its five subgroups correspond to the fields intermediate between the base
Q
\Q.
\Q(\sqrt{3}),
\Q(\sqrt{2}),
\Q(\sqrt{6}),
The following is the simplest case where the Galois group is not abelian.
x3-2
\Q
K=\Q(\theta,\omega)
\theta=\sqrt[3]{2}
\omega=-\tfrac{1}2+i\tfrac{\sqrt3}2.
x2+x+1
Q\subsetK
\Q
\{1,\theta,\theta2,\omega,\omega\theta,\omega\theta2\}
G=Gal(K/\Q)
x3-2
\alpha1=\theta, \alpha2=\omega\theta,
2\theta. \alpha 3=\omega
Since there are only 3! = 6 such permutations, G must be isomorphic to the symmetric group of all permutations of three objects. The group can be generated by two automorphisms f and g defined by:
f(\theta)=\omega\theta, f(\omega)=\omega,
g(\theta)=\theta, g(\omega)=\omega2,
and
G=\left\{1,f,f2,g,gf,gf2\right\}
f3=g2=(gf)2=1
\alpha1,\alpha2,\alpha3
f=(123),g=(23)
The subgroups of G and corresponding subfields are as follows:
\Q
H=\{1,f,f2\}
\Q(\omega)
[\Q(\omega):\Q]=\tfrac{|G|}{|H|}=2
\Q
x2+x+1
G/H=\{[1],[g]\}
\{1,g\},\{1,gf\}
\{1,gf2\},
\Q(\theta),\Q(\omega\theta),\Q(\omega2\theta).
\Q
\Q
\alpha1,\alpha2,\alpha3
Let
E=\Q(λ)
G=\left\{λ,
1 | |
1-λ |
,
λ-1 | |
λ |
,
1 | |
λ |
,
λ | |
λ-1 |
,1-λ \right\}\subsetAut(E);
here we denote an automorphism
\phi:E\toE
\phi(λ)
f(λ)\mapstof(\phi(λ))
S3
F
G
{\rmGal}(E/F)=G
If
H
G
P(T):=\prodh(T-h)\inE[T]
generate the fixed field of
H
E/F
H=\{λ,1-λ\}
\Q(λ(1-λ))
H=\{λ,\tfrac{1}{λ}\}
\Q(λ+\tfrac{1}{λ})
G
F=\Q(j),
Similar examples can be constructed for each of the symmetry groups of the platonic solids as these also have faithful actions on the projective linej=
256(1-λ(1-λ))3 (λ(1-λ))2 =
256(1-λ+λ2)3 λ2(1-λ)2 .
P1(\Complex)
\Complex(x)
The theorem classifies the intermediate fields of E/F in terms of group theory. This translation between intermediate fields and subgroups is keyto showing that the general quintic equation is not solvable by radicals (see Abel–Ruffini theorem). One first determines the Galois groups of radical extensions (extensions of the form F(α) where α is an n-th root of some element of F), and then uses the fundamental theorem to show that solvable extensions correspond to solvable groups.
Theories such as Kummer theory and class field theory are predicated on the fundamental theorem.
Given an infinite algebraic extension we can still define it to be Galois if it is normal and separable. The problem that one encounters in the infinite case is that the bijection in the fundamental theorem does not hold as we get too many subgroups generally. More precisely if we just take every subgroup we can in general find two different subgroups that fix the same intermediate field. Therefore we amend this by introducing a topology on the Galois group.
Let
E/F
G=Gal(E/F)
i\inI
\varphii:G → Gi
\sigma\mapsto
\sigma | |
|Li |
G
i\inI
\varphii:G → Gi
Gi
G\cong\varprojlimGi
Gi
G
E/F
Now that we have defined a topology on the Galois group we can restate the fundamental theorem for infinite Galois extensions.
Let
l{F}(E/F)
E/F
l{C}(G)
G=Gal(E/F)
l{F}(E/F)
l{C}(G)
\Phi:l{F}(E/F) → l{C}(G)
L\mapstoGal(E/L)
\Gamma:l{C}(G) → l{F}(E/F)
N\mapstoFixE(N):=\{a\inE~|~\sigma(a)=aforall\sigma\inN\}
\Phi
\Phi(L)
G
L