The Fundamental Theorem of Galois Theory

⚡ Key Takeaways

The Fundamental Theorem of Galois Theory (FTGT) establishes an order-reversing bijection between the intermediate fields of a finite Galois extension L/KL/K and the subgroups of its Galois group Gal(L/K)\mathrm{Gal}(L/K). In words: the lattice of fields between KK and LL is the mirror image of the lattice of subgroups of the symmetry group of the extension. Where it applies: finite (and with care, infinite) Galois extensions of arbitrary fields; central to solvability of polynomials, algebraic number theory, and arithmetic geometry. Who/when: envisioned by Évariste Galois (1830–1832), made rigorous by Dedekind, Weber, Emil Artin (1940s), and Krull (infinite case, 1928).

💡 The Core Insight

Symmetry organizes structure. The automorphisms of LL fixing KK form a group whose subgroup lattice is a faithful, inverted photograph of the field lattice. Bigger groups fix smaller fields; bigger fields are fixed by smaller groups. The dimension counts and the symmetry counts coincide exactly (∣Gal∣=[L:K]|\mathrm{Gal}| = [L:K]) only in the Galois case — that exact equality is what makes the correspondence a bijection rather than a mere injection.

Formal Statement

DefinitionGalois Extension and Galois Group

Let L/KL/K be a field extension.

  • Aut(L/K)\mathrm{Aut}(L/K) is the group of field automorphisms σ:L→L\sigma: L \to L with σ∣K=idK\sigma|_K = \mathrm{id}_K, under composition.
  • For a subset S⊆Aut(L/K)S \subseteq \mathrm{Aut}(L/K), the fixed field is
1
LS={ x∈L:σ(x)=x for all σ∈S }.\quad L^{S} = \{\, x \in L : \sigma(x) = x \ \text{for all } \sigma \in S \,\}.

Derivation hint: LSL^S is closed under +,⋅,(−)−1+,\cdot,(-)^{-1} because each σ\sigma is a field homomorphism, so the fixed set inherits all field operations.

  • L/KL/K is finite Galois iff it is finite, normal (every irreducible f∈K[x]f \in K[x] with a root in LL splits in LL), and separable (the minimal polynomial of every α∈L\alpha \in L has no repeated roots). In that case we write G=Gal(L/K)=Aut(L/K)G = \mathrm{Gal}(L/K) = \mathrm{Aut}(L/K).

The defining numerical criterion (Artin) is:

2
L/K Galois  ⟺  ∣Aut(L/K)∣=[L:K]  ⟺  LAut(L/K)=K.\quad L/K \text{ Galois} \iff |\mathrm{Aut}(L/K)| = [L:K] \iff L^{\mathrm{Aut}(L/K)} = K.

Derivation hint: in general ∣Aut(L/K)∣≤[L:K]|\mathrm{Aut}(L/K)| \le [L:K] with equality forcing KK to be the full fixed field; Artin's lemma gives the reverse implication.

TheoremFundamental Theorem of Galois Theory

Let L/KL/K be a finite Galois extension with group G=Gal(L/K)G = \mathrm{Gal}(L/K), ∣G∣=[L:K]=n|G| = [L:K] = n. Define

3
Φ:{ M:K⊆M⊆L }⟶{ H:H≤G },Φ(M)=Gal(L/M),\quad \Phi: \{\,M : K \subseteq M \subseteq L\,\} \longrightarrow \{\,H : H \le G\,\}, \qquad \Phi(M) = \mathrm{Gal}(L/M),

Derivation hint: L/ML/M is automatically Galois for any intermediate MM since normality and separability descend to the top of the tower.

4
Ψ:{ H:H≤G }⟶{ M:K⊆M⊆L },Ψ(H)=LH.\quad \Psi: \{\,H : H \le G\,\} \longrightarrow \{\,M : K \subseteq M \subseteq L\,\}, \qquad \Psi(H) = L^{H}.

Derivation hint: Ψ\Psi is well-defined because LHL^H is a field containing K=LG⊆LHK = L^G \subseteq L^H. Then:

(1) Bijection. Φ\Phi and Ψ\Psi are mutually inverse:

5
LGal(L/M)=MandGal(L/LH)=H.\quad L^{\mathrm{Gal}(L/M)} = M \quad\text{and}\quad \mathrm{Gal}(L/L^{H}) = H.

Derivation hint: L/ML/M Galois gives the first identity from criterion [2]; Artin's lemma applied to HH acting on LL gives the second.

(2) Order-reversal. M1⊆M2  ⟺  Φ(M2)⊆Φ(M1)M_1 \subseteq M_2 \iff \Phi(M_2) \subseteq \Phi(M_1).

(3) Degree–index match.

6
[L:M]=∣Gal(L/M)∣,[M:K]=[G:Gal(L/M)].\quad [L:M] = |\mathrm{Gal}(L/M)|, \qquad [M:K] = [G : \mathrm{Gal}(L/M)].

Derivation hint: the first is criterion [2] for L/ML/M; the second is the tower law [L:K]=[L:M][M:K][L:K]=[L:M][M:K] combined with Lagrange's index formula.

(4) Normality correspondence. M/KM/K is normal (equivalently Galois)   ⟺  H=Gal(L/M)\iff H = \mathrm{Gal}(L/M) is normal in GG. In that case restriction induces an isomorphism

7
Gal(M/K)  ≅  G/Gal(L/M).\quad \mathrm{Gal}(M/K) \;\cong\; G\big/\mathrm{Gal}(L/M).

Derivation hint: restriction σ↦σ∣M\sigma \mapsto \sigma|_M is well-defined precisely when σ(M)=M\sigma(M)=M for all σ\sigma, which is conjugation-invariance of HH; the kernel is Gal(L/M)\mathrm{Gal}(L/M).

(5) Conjugation. For any σ∈G\sigma \in G, σ(M)\sigma(M) corresponds to the conjugate subgroup σGal(L/M)σ−1\sigma \mathrm{Gal}(L/M)\sigma^{-1}.

Why It Holds / Derivation

ProofProof of the Fundamental Theorem

The engine is Artin's Lemma: if HH is a finite group of automorphisms of a field LL, then [L:LH]=∣H∣[L : L^{H}] = |H|.

Step 1 — Artin's Lemma (linear independence of characters). Distinct automorphisms σ1,…,σm\sigma_1,\dots,\sigma_m are linearly independent over LL as functions L×→L×L^\times \to L^\times (Dedekind). For H={σ1,…,σm}H = \{\sigma_1,\dots,\sigma_m\} put F=LHF = L^{H}. One shows [L:F]≤m[L:F] \le m: any m+1m+1 elements of LL are FF-linearly dependent, by solving a homogeneous system whose coefficient matrix has rows (σi(xj))(\sigma_i(x_j)) and exploiting a minimal nontrivial dependence to land in FF. Conversely [L:F]≥∣H∣[L:F] \ge |H| since the mm distinct embeddings of LL over FF are linearly independent. Hence

8
[L:LH]=∣H∣.\quad [L : L^{H}] = |H|.

Derivation hint: equality is squeezed from two inequalities — the upper from a counting/linear-algebra argument, the lower from independence of characters forcing at least ∣H∣|H| embeddings.

Step 2 — Ψ\Psi then Φ\Phi recovers HH. Let F=LHF=L^H. Then H⊆Gal(L/F)H \subseteq \mathrm{Gal}(L/F) trivially. By Artin, [L:F]=∣H∣[L:F]=|H|, while ∣Gal(L/F)∣≤[L:F]|\mathrm{Gal}(L/F)| \le [L:F]. So ∣Gal(L/F)∣≤∣H∣|\mathrm{Gal}(L/F)| \le |H|, forcing Gal(L/LH)=H\mathrm{Gal}(L/L^H)=H. This proves the second identity in [5].

Step 3 — Φ\Phi then Ψ\Psi recovers MM. For intermediate MM, L/ML/M is normal and separable (subextension at the top of a normal separable tower), hence Galois, so by criterion [2], LGal(L/M)=ML^{\mathrm{Gal}(L/M)} = M. This is the first identity in [5]. Steps 2–3 establish the bijection (1).

Step 4 — Order reversal and degrees. If M1⊆M2M_1 \subseteq M_2, any automorphism fixing M2M_2 fixes M1M_1, so Gal(L/M2)⊆Gal(L/M1)\mathrm{Gal}(L/M_2) \subseteq \mathrm{Gal}(L/M_1). Equation [6] follows from [8] with H=Gal(L/M)H=\mathrm{Gal}(L/M) and the tower law.

Step 5 — Normal subgroups. Fix σ∈G\sigma \in G and intermediate MM with H=Gal(L/M)H=\mathrm{Gal}(L/M). Then for τ∈G\tau \in G, τ\tau fixes σ(M)\sigma(M) pointwise iff σ−1τσ\sigma^{-1}\tau\sigma fixes MM, i.e.

9
Gal(L/σ(M))=σ Gal(L/M) σ−1.\quad \mathrm{Gal}\big(L/\sigma(M)\big) = \sigma\, \mathrm{Gal}(L/M)\, \sigma^{-1}.

Derivation hint: τ(σm)=σm  ⟺  (σ−1τσ)(m)=m\tau(\sigma m)=\sigma m \iff (\sigma^{-1}\tau\sigma)(m)=m; translate the pointwise-fixing condition through σ\sigma. Thus σ(M)=M\sigma(M)=M for all σ\sigma (i.e. M/KM/K normal) iff HH is invariant under all conjugations, i.e. H⊴GH \trianglelefteq G.

Step 6 — The quotient. When H⊴GH \trianglelefteq G, every σ∈G\sigma \in G satisfies σ(M)=M\sigma(M)=M, so restriction ρ:σ↦σ∣M\rho:\sigma \mapsto \sigma|_M maps G→Gal(M/K)G \to \mathrm{Gal}(M/K). Its kernel is exactly {σ:σ∣M=id}=Gal(L/M)=H\{\sigma : \sigma|_M=\mathrm{id}\} = \mathrm{Gal}(L/M)=H. Surjectivity follows because every KK-automorphism of MM extends to LL (normality of L/KL/K). The first isomorphism theorem yields [7]. ■\blacksquare

∎
mathematician · Évariste Galois | 1811–1832

Galois, dead in a duel at twenty, never wrote "the Fundamental Theorem" — he wrote of the group of permutations of the roots that leaves all rational relations invariant. His 1831 memoir, rejected and nearly lost, contained the decisive idea: solvability by radicals corresponds to a chain of subgroups with abelian quotients (a solvable group). The modern lattice-theoretic statement, the fixed-field formalism, and the clean bijection are due to later hands — Dedekind introduced field automorphisms abstractly, Heinrich Weber systematized "Galois groups," and Emil Artin reorganized the entire theory around linear algebra and Artin's lemma, dethroning the primitive-element argument and making the proof characteristic-free and conceptually transparent.

Building Intuition

🧠 Intuition

Think of LL as a crystal and GG as its symmetry group. Each intermediate field MM is a substructure you can carve out by demanding invariance under part of the symmetry. Demand invariance under the whole group GG: you get the smallest possible field, KK (the most symmetric part). Demand invariance under only the trivial subgroup {1}\{1\}: nothing is forced, you get all of LL. The order reversal is the natural "more constraints ⇒\Rightarrow smaller object" logic: a larger subgroup imposes more symmetry constraints, so its fixed field is smaller. The degree of LL over MM literally counts how many symmetries you have left after pinning MM down — exactly ∣Gal(L/M)∣|\mathrm{Gal}(L/M)|. Normality is the subtle part. A subfield MM is "stable" — globally fixed as a set, not pointwise — exactly when the symmetries fixing it form a normal subgroup. Normal subgroups are the ones you can quotient by to get a new group; correspondingly normal subfields are the ones that carry their own self-contained Galois theory, with group the quotient.

Figure
The Galois correspondence for Q(2,3)/Q\mathbb{Q}(\sqrt 2,\sqrt 3)/\mathbb{Q}: fields (left) mirror subgroups (right)
Field lattice Subgroup lattice (Klein four V) Q(√2,√3) Q(√2) Q(√3) Q(√6) Q {1} ⟨τ₃⟩ ⟨τ₂⟩ ⟨τ₂τ₃⟩ V = {1,τ₂,τ₃,τ₂τ₃} Φ is order-REVERSING (dashed): top↔bottom

Worked Examples

ExampleThe biquadratic field Q(2,3)\mathbb{Q}(\sqrt2,\sqrt3)

Given. L=Q(2,3)L=\mathbb{Q}(\sqrt2,\sqrt3), K=QK=\mathbb{Q}. The minimal polynomials x2−2x^2-2 and x2−3x^2-3 split in LL and are separable (char 0), so L/QL/\mathbb{Q} is Galois.

Step 1 — Degree. [Q(2):Q]=2[\mathbb{Q}(\sqrt2):\mathbb{Q}]=2 and 3∉Q(2)\sqrt3 \notin \mathbb{Q}(\sqrt2), so [L:Q]=2⋅2=4[L:\mathbb{Q}] = 2\cdot 2 = 4.

Step 2 — Group. Each automorphism sends 2↦±2\sqrt2 \mapsto \pm\sqrt2, 3↦±3\sqrt3 \mapsto \pm\sqrt3 independently, giving 44 automorphisms. Thus G≅Z/2×Z/2G \cong \mathbb{Z}/2 \times \mathbb{Z}/2, the Klein four-group VV. Write τ2:2↦−2\tau_2:\sqrt2\mapsto-\sqrt2 (fixes 3\sqrt3), τ3:3↦−3\tau_3:\sqrt3\mapsto-\sqrt3 (fixes 2\sqrt2).

Step 3 — Subgroups → fixed fields.

  • ⟨τ3⟩\langle\tau_3\rangle fixes 2\sqrt2 ⟹ L⟨τ3⟩=Q(2)L^{\langle\tau_3\rangle}=\mathbb{Q}(\sqrt2).
  • ⟨τ2⟩\langle\tau_2\rangle fixes 3\sqrt3 ⟹ Q(3)\mathbb{Q}(\sqrt3).
  • ⟨τ2τ3⟩\langle\tau_2\tau_3\rangle fixes 23=6\sqrt2\sqrt3=\sqrt6 ⟹ Q(6)\mathbb{Q}(\sqrt6).

Step 4 — Normality. VV is abelian ⟹ every subgroup is normal ⟹ every intermediate field is Galois over Q\mathbb{Q} (each is a degree-2, hence normal, extension).

  3 nontrivial subgroups↔Q(2), Q(3), Q(6);G≅V4  \boxed{\;\text{3 nontrivial subgroups} \leftrightarrow \mathbb{Q}(\sqrt2),\ \mathbb{Q}(\sqrt3),\ \mathbb{Q}(\sqrt6);\quad G\cong V_4\;}

:::example[A non-abelian group: Q(23,ω)\mathbb{Q}(\sqrt[3]{2},\omega)] Given. Splitting field LL of x3−2x^3-2 over Q\mathbb{Q}, where ω=e2πi/3\omega=e^{2\pi i/3}. Roots: 23, ω23, ω223\sqrt[3]2,\ \omega\sqrt[3]2,\ \omega^2\sqrt[3]2.

Step 1 — Degree. [Q(23):Q]=3[\mathbb{Q}(\sqrt[3]2):\mathbb{Q}]=3 (Eisenstein), and [Q(23,ω):Q(23)]=2[\mathbb{Q}(\sqrt[3]2,\omega):\mathbb{Q}(\sqrt[3]2)]=2 (since ω∉R\omega\notin\mathbb{R}). Tower law: [L:Q]=6[L:\mathbb{Q}]=6.

Step 2 — Group. GG permutes the three roots faithfully, ∣G∣=6|G|=6, so G≅S3G\cong S_3.

Step 3 — Subgroup lattice. S3S_3 has: trivial; three order-2 subgroups (transpositions); one order-3 subgroup A3A_3; and S3S_3 itself.

Step 4 — Correspondence.

  • A3⊴S3A_3 \trianglelefteq S_3 ⟹ its fixed field is normal over Q\mathbb{Q}. A3A_3 (order 3, index 2) ⟹ fixed field has degree 2: LA3=Q(ω)L^{A_3}=\mathbb{Q}(\omega), which is Galois (cyclotomic) ✓, with Gal(Q(ω)/Q)≅S3/A3≅Z/2\mathrm{Gal}(\mathbb{Q}(\omega)/\mathbb{Q})\cong S_3/A_3\cong\mathbb{Z}/2.
  • The three order-2 subgroups are not normal ⟹ their fixed fields Q(23), Q(ω23), Q(ω223)\mathbb{Q}(\sqrt[3]2),\ \mathbb{Q}(\omega\sqrt[3]2),\ \mathbb{Q}(\omega^2\sqrt[3]2) are not Galois over Q\mathbb{Q} (each degree 3, but x3−2x^3-2 does not split in any one of them). They are the three conjugates of each other, matching the three conjugate subgroups.
  G≅S3; normal subgroup A3↔Q(ω); 3 non-normal ↔3 cube-root fields  \boxed{\;G\cong S_3;\ \text{normal subgroup }A_3\leftrightarrow\mathbb{Q}(\omega);\ \text{3 non-normal }\leftrightarrow\text{3 cube-root fields}\;}

Common Misconceptions

⚠️ Galois is not automatic

The bijection requires L/KL/K to be both normal and separable. Either failure breaks the theorem:

  • Inseparable failure: K=Fp(t)K=\mathbb{F}_p(t), L=K(t1/p)L=K(t^{1/p}). Then xp−t=(x−t1/p)px^p-t=(x-t^{1/p})^p has a single repeated root, Aut(L/K)={1}\mathrm{Aut}(L/K)=\{1\}, yet [L:K]=p[L:K]=p. The fixed field of the trivial group is all of LL, not KK, so [5] fails. The map Ψ\Psi is not surjective onto {K⊆M⊆L}\{K \subseteq M \subseteq L\}.
  • Non-normal failure: L=Q(23)/QL=\mathbb{Q}(\sqrt[3]2)/\mathbb{Q} has Aut={1}\mathrm{Aut}=\{1\} but degree 3; x3−2x^3-2 does not split.
CounterexampleOrder-reversal must not be dropped, and conjugates need not coincide

In Q(23,ω)\mathbb{Q}(\sqrt[3]2,\omega) the three subfields Q(ωk23)\mathbb{Q}(\omega^k\sqrt[3]2) are distinct fields of the same degree 3 over Q\mathbb{Q}, corresponding to three distinct conjugate order-2 subgroups of S3S_3. A common error is to assume "same degree ⟹ same field" or "all index-3 subgroups are normal." Both are false here: the lattice genuinely has three separate branches, and none of these subfields is Galois over Q\mathbb{Q} because the matching subgroups are not normal. Equation [9] is what forces conjugate subgroups to give conjugate (isomorphic but possibly unequal) subfields.

⚠️ Infinite extensions need topology

For an infinite Galois extension (e.g. Q‾/Q\overline{\mathbb{Q}}/\mathbb{Q}, or Fp‾/Fp\overline{\mathbb{F}_p}/\mathbb{F}_p), the naive bijection fails: there are more subgroups than intermediate fields. The fix (Krull) is to topologize GG with the Krull (profinite) topology, where a base of open neighborhoods of 11 is given by Gal(L/M)\mathrm{Gal}(L/M) for finite M/KM/K. Then the correspondence holds between intermediate fields and closed subgroups, not all subgroups. See Infinite Galois Theory.

Connections

connection

The FTGT is a hub linking many fields:

  • <a class="wiki-link" href="/wiki/math-algebra-solvability-by-radicals">Solvability by Radicals</a>: A polynomial is solvable by radicals iff its Galois group is a solvable group; the chain of subfields obtained by adjoining radicals mirrors a chain of normal subgroups with abelian quotients via [7].
  • <span class="wiki-link-missing">Class Field Theory</span>: describes abelian extensions of number fields — those with abelian Galois group — via the idele class group; the FTGT's normality/quotient structure is the foundation.
  • <span class="wiki-link-missing">Inverse Galois Problem</span>: which finite groups arise as Gal(L/Q)\mathrm{Gal}(L/\mathbb{Q})? The correspondence makes this a precise question about realizing abstract groups.
  • <span class="wiki-link-missing">Covering Space Theory</span>: the topological analogue — the deck transformation group of a covering corresponds to subgroups of the fundamental group, with normal subgroups giving regular (Galois) covers. This is the prototype of a Galois Category.
  • <span class="wiki-link-missing">Differential Galois Theory</span>: replaces field automorphisms with those commuting with a derivation, yielding algebraic groups; solvability of linear ODEs in closed form mirrors solvability of the differential Galois group.

Real-World Applications

🔬 Where this appears

Historical Development

⏳ History
- 1770 — Lagrange. Réflexions sur la résolution algébrique des équations: studies how rational functions of roots permute, foreshadowing the "Galois resolvent."
- 1799–1813 — Ruffini. Argues (incompletely) that the general quintic is unsolvable by radicals.
- 1824 — Abel. Gives the first rigorous proof of quintic unsolvability, but without the conceptual group-theoretic framework.
- 1830–1832 — Galois. Introduces the group of an equation and the solvability criterion; memoir submitted to the Académie, rejected/lost. Dies in a duel May 1832 at 20.
- 1846 — Liouville. Publishes Galois's manuscripts in his Journal, finally making the work accessible.
- 1870 — Jordan. Traité des substitutions: first systematic treatment, framing Galois theory through permutation groups.
- 1893–1895 — Weber & Dedekind. Recast the theory abstractly using fields and automorphisms; "Galois group" enters standard language.
- 1928 — Krull. Extends the correspondence to infinite extensions via the profinite topology.
- 1942–1944 — Artin. Reformulates the entire subject around linear independence of characters and fixed fields (Artin's lemma), giving the clean, primitive-element-free proof used in modern graduate courses.

Subtleties & Limits

open-problem
  • Inverse Galois Problem. Is every finite group the Galois group of some extension of Q\mathbb{Q}? Known for all solvable groups (Shafarevich) and many simple groups, but open in general. The FTGT defines the question but does not solve it.
  • Grothendieck's anabelian program. To what extent does the absolute Galois group Gal(Q‾/Q)\mathrm{Gal}(\overline{\mathbb{Q}}/\mathbb{Q}), as a profinite group with its action on geometric fundamental groups, determine arithmetic varieties? The Section Conjecture remains open. This generalizes FTGT to a correspondence between covers and group actions (Grothendieck's Galois Theory).
  • Explicit Langlands reciprocity. The Langlands program seeks to understand all (including non-abelian) Galois representations via automorphic forms — a vast generalization of the abelian case settled by class field theory; large parts are conjectural.
  • Differential and difference Galois theory extend FTGT to linear ODEs/recurrences (Picard–Vessiot theory), with subtle constraints (algebraic closure of constants) and open inverse problems for differential Galois groups.

See Also

Field Extensions · Splitting Fields and Normal Extensions · Separable Extensions · Solvability by Radicals · Infinite Galois Theory · Class Field Theory · Inverse Galois Problem · Grothendieck's Galois Theory · Differential Galois Theory · Galois Representations · Covering Space Theory