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Symmetry of Roots: Automorphisms & the Galois Group

Galois's revolutionary idea: instead of chasing roots, study the symmetries that shuffle them. Those symmetries form a group — and a group is something we know how to control.

An automorphism: a symmetry of a field

An automorphism of a field K is a relabeling of its elements that preserves all the arithmetic: σ(a + b) = σ(a) + σ(b) and σ(ab) = σ(a)σ(b). For an extension K/F we add one rule — σ must fix every element of the base field F, leaving the rationals untouched.

The classic example: complex conjugation. The map a + bi ↦ a − bi is an automorphism of C that fixes every real number. It is exactly a conjugate symmetry — and it swaps the two roots i and −i of x² + 1.

The Galois group

Collect every automorphism of K that fixes F. They form a group under composition — call it the Galois group Gal(K/F). The identity is the do-nothing map, the inverse of a relabeling undoes it, and composing two symmetries is again a symmetry. Everything you learned about groups now applies.

Because each σ just shuffles the roots, the Galois group acts as a group of permutations of the roots — a subgroup of the full symmetric group on n roots. Often it is a proper subgroup, not the whole thing, because the roots may have hidden relations the symmetries must respect.

Working one out by hand

Gal(Q(√2, √3) / Q):

Roots to shuffle:  √2 → ±√2,  √3 → ±√3 (independently)
Each automorphism is determined by these two sign choices:

  e   :  √2 → √2,   √3 → √3      (identity)
  σ   :  √2 → −√2,  √3 → √3
  τ   :  √2 → √2,   √3 → −√3
  στ  :  √2 → −√2,  √3 → −√3

4 elements, every one its own inverse  ⇒  the Klein four-group.
Note |Gal| = 4 = [Q(√2,√3) : Q].  The order MATCHES the degree.
Four sign-flips, four symmetries — and the group's size equals the extension's degree.

That last line — |Gal(K/F)| equals the degree [K : F] — is no accident. It holds exactly when K is a “nice” extension (a splitting field of a separable polynomial). When the sizes match like this, the extension is called Galois, and we are ready for the theorem that ties the two worlds together.