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Sunday, October 6, 2024

The Intersection of Galois Theory and Algebraic Geometry: Exploring the Orbit Space Structure of Spec F[T]

The first example

Let ι:Q↪Q[2] be a field extension, Gal(Q[2]/Q)≅Z/2Z​.

image-20241006103820271

We could induce a ring homomorphism

(1)ι′:Q[T]↪Q[2][T]

and act the spectrum functor both sides

(2)Spec(ι′):Spec(Q[2][T])→Spec(Q[T])

Consider b≠0,(T+(a+b2)),(T−(a−b2)),∈Spec(Q[2][T]),

(3)Spec(ι′)((T−(a+b2)))=Spec(ι′)(T−(a−b2))=(T2−2aT−a2+b2)

image-20241006103946382

and we could view the roots of irreducible polynomial f(x) as fiber at pf.

(4)p−1(T2−2aT−a2+b2)={(T+(a+b2)),(T−(a−b2)}

Let x∈p−1(pf), then p∘σ(x)=p(x), hence σ(x)∈p−1(pf) as well.

This is a geometric interpretation of the fact that the Galois group permutes the roots of f(x).

In this case, p−1(T2−2)={(T−2),(T+2)} correspond to the orbit of 2 under Gal(Q[2]/Q).

Fiber functor.

Consider the slice category B/Top. Let s be a point in B, then we can define a fiber functor Fs as follows:

(5)Fs(πX:X→B)=πX−1(s)

For a morphism

(6)f:(X→πXB)→(Y→πYB)

We have

(7)Fs(f)=fs:πX−1(s)→πY−1(s)

Splitting field

Let f∈F[T] be an irreducible polynomial and L be the splitting field of f, and f is separateble in L.

Then we could consider the following diagram:

image-20241006180308058

Again, for a point ph=(h(T))∈Spec(F[T]), the fiber correspond to the roots of h(T) in L.

(8)p−1(ph)={(T−α),(T−σ1(α)),...,(T−σn(α))}≅Spec(L[T]/(h(T)))≅OGal(L/K)(α)

The fiber functor F(f) shows that why the Galois group permute the roots of f via σf:p−1(f)→p−1(f).

Orbit Space

Let G be a group and let G acts on X via ϕ:G→AutC(X). We denote that X/G​ to be the space of orbit of this group action.

image-20241010210748843

For all the G invariant function, i.e. ∀g∈G,f(g⋅x)=f(x), we have an unique function f^:X/G→X such that

(9)f=f^∘π

Now think about the splitting field of f∈F[T] again.

Consider the orbit space

(10)Spec(L[T])/Gal(L/F)

We know that the Galois group act transitive at the roots of f since f is irreducible.

Then a irreducible polynomial g split in L iff g=∏σ∈Gal(L/F)(T−σ(α)),α∈L−F.

Hence the orbit space

(11)Spec(L[T])/Gal(L/F)≅Spec(F[T])

So the Galois Group ''glue them back''.

The p can be viewed as the projection from X to X/G.

(12)p:Spec(L[T])→Spec(L[T])/Gal(L/F)

Hence we get the universal property of the affine scheme Spec(F[T]):

image-20241010211107966

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