Universal Kernel

Galois category

What are objects and seams, read in Grothendieck’s Galois theory?

A category of finite sets with an action, and a functor that forgets the action: the objects of a group are its connected objects, seams its isomorphisms, markings identifications of fibre functors, and seams over automorphisms its twists by Out(G).

∛2ω∛2ω²∛2complex conjugationQ(∛2, ω)1Q(∛2)C2Q(ω∛2)C2Q(ω²∛2)C2Q(ω)C3QS3Aut = C2
Plate 2.7The Galois category of S3S_3, read in fields: the fields between Q\Q and Q(23,ω)\Q(\sqrt[3]2,\omega) over the subgroups that fix them. The three cubic fields, gold, are three incarnations of one rigid object, joined by exactly one Q\Q-isomorphism each; complex conjugation fixes 23\sqrt[3]2 and is the automorphism of Q(ω)\Q(\omega).
Definition

A category equivalent to the category of finite continuous π\pi-sets, for a profinite group π\pi, is a Galois category, and a functor FF to finite sets satisfying Grothendieck’s axioms is a fundamental functor, or fibre functor. For a finite group GG, the category CG\mathcal C_G of finite GG-sets and GG-maps, with the functor FGF_G that forgets the action, is one, and Aut⁡(FG)≅G\Aut(F_G)\cong G.

Theorem(Objects are the connected objects of a Galois category) proved

Let CG\mathcal C_G be the category of finite GG-sets and GG-maps, and FG ⁣:CG→FinSetF_G\colon\mathcal C_G\to\mathbf{FinSet} the functor that forgets the action.

(a) (CG,FG)(\mathcal C_G,F_G) satisfies Grothendieck’s axioms (G1)–(G6), and g↦(x↦gx)g\mapsto(x\mapsto gx) is an isomorphism from GG onto Aut⁡(FG)\Aut(F_G).

(b) The connected objects of CG\mathcal C_G are the objects of GG, its transitive sets. The object G/HG/H is Galois, that is, its automorphism group acts transitively on its fibre, if and only if HH is normal.

(c) A Galois category whose fundamental functor has automorphism group isomorphic to GG is equivalent to CG\mathcal C_G, by an equivalence that carries the fundamental functor to FGF_G.

Proof

(a) Limits, sums, and quotients by finite groups of GG-automorphisms are formed on the underlying sets. The image of a GG-map and its complement are GG-stable, so a GG-map is a surjection onto its image followed by the inclusion of a direct summand, and a bijective GG-map is a GG-isomorphism: FGF_G is exact and reflects isomorphisms. Let η\eta be an automorphism of FGF_G and put g=ηG(1)g=\eta_G(1), its value at the regular set. For x∈Xx\in X the map fx(k)=kxf_x(k)=kx is a GG-map, and naturality gives ηX(x)=ηX(fx(1))=fx(ηG(1))=gx\eta_X(x)=\eta_X(f_x(1))=f_x(\eta_G(1))=gx. Conversely each gg defines an automorphism of FGF_G, and composition corresponds to multiplication.

(b) A GG-set is the sum of its orbits, so it is connected exactly when it is transitive. The automorphism group of G/HG/H is NG(H)/HN_G(H)/H, acting freely on G/HG/H, and transitively exactly when NG(H)=GN_G(H)=G. (c) is Grothendieck’s theorem (SGA 1, Exposé V).

Proposition(Markings are fibre-functor data) proved

Let a theory supply a finite group Γ\Gamma acting on a set YY, and let μ ⁣:G→Γ\mu\colon G\to\Gamma be a marking.

(a) Restriction along μ\mu is an exact functor μ∗ ⁣:CΓ→CG\mu^*\colon\mathcal C_\Gamma\to\mathcal C_G with FG∘μ∗=FΓF_G\circ\mu^*=F_\Gamma, and the marked set is Yμ=μ∗(Y)Y_\mu=\mu^*(Y).

(b) Conversely, let H ⁣:CΓ→CGH\colon\mathcal C_\Gamma\to\mathcal C_G be a functor and η ⁣:FG∘H→FΓ\eta\colon F_G\circ H\to F_\Gamma an isomorphism of functors. There is exactly one homomorphism μ ⁣:G→Γ\mu\colon G\to\Gamma for which every ηY\eta_Y is a GG-isomorphism H(Y)→YμH(Y)\to Y_\mu. Replacing η\eta by γ∘η\gamma\circ\eta, for γ∈Γ=Aut⁡(FΓ)\gamma\in\Gamma=\Aut(F_\Gamma), replaces μ\mu by γμ(⋅)γ−1\gamma\mu(\cdot)\gamma^{-1}.

(c) In particular, a change of marking by an inner automorphism is a change of the identification of fibre functors, that is, of base point: the maps y↦μ(h)yy\mapsto\mu(h)y form an isomorphism of functors μ∗→(μ∘ιh)∗\mu^*\to(\mu\circ\iota_h)^*, where ιh(g)=hgh−1\iota_h(g)=hgh^{-1}.

Proof

(a) is immediate. (b) For g∈Gg\in G, the maps x↦gxx\mapsto gx on the sets FG(H(Y))F_G(H(Y)) form an automorphism of FG∘HF_G\circ H. Transported by η\eta it is an automorphism of FΓF_\Gamma, hence the action of a unique element μ(g)∈Γ\mu(g)\in\Gamma. Then ηY(gx)=μ(g)ηY(x)\eta_Y(gx)=\mu(g)\eta_Y(x) for all YY and xx, and μ\mu is a homomorphism; it is the only one with this property, because Γ\Gamma acts faithfully on its regular set. Replacing η\eta by γη\gamma\eta conjugates the transported automorphisms by γ\gamma. (c) μ(h)μ(g)y=μ(hgh−1)μ(h)y\mu(h)\mu(g)y=\mu(hgh^{-1})\mu(h)y.

Theorem(Seam monodromy is non-abelian H1H^{1}) proved

Let G\mathcal G be a connected graph with base vertex vv and π=π1(G,v)\pi=\pi_1(\mathcal G,v), and let XX be an object with stabilizer HH and automorphism group A=Aut⁡G(X)≅NG(H)/HA=\Aut_G(X)\cong N_G(H)/H.

(a) The gauge classes of seam systems for XX over G\mathcal G correspond to H1(π,A)=Hom⁡(π,A)/AH^1(\pi,A)=\operatorname{Hom}(\pi,A)/A, the first non-abelian cohomology set for the trivial action. They also correspond to the isomorphism classes of principal AA-coverings of G\mathcal G: to a system corresponds the covering whose fibre over a vertex ww is the set of alignments Iso⁡G(X,Yw)\Iso_G(X,Y_w), with AA acting by precomposition and the seams as transition maps. The system is coherent exactly when its class is trivial.

(b) Let Aut⁡tw(X)\Aut^{\mathrm{tw}}(X) be the group of pairs (β,f)(\beta,f), with β∈Aut⁡(G)\beta\in\Aut(G) and ff a seam over β\beta from XX to XX, an extension 1→A→Aut⁡tw(X)→Aut⁡(G)[H]→11\to A\to\Aut^{\mathrm{tw}}(X)\to\Aut(G)_{[H]}\to1. With an incarnation of XX at each vertex, a seam over an automorphism on each edge, and changes of marking as gauge transformations, such systems correspond to H1(π,Aut⁡tw(X))H^1(\pi,\Aut^{\mathrm{tw}}(X)). Their image in H1(π,Aut⁡(G)[H])H^1(\pi,\Aut(G)_{[H]}) is the monodromy of the markings, and since π\pi is free, every class there arises.

Proof

(a) The correspondence with Hom⁡(π,A)/A\operatorname{Hom}(\pi,A)/A is the gauge theorem of Chapter 4. A principal AA-covering of a connected graph is determined up to isomorphism by its holonomy, a homomorphism π→A\pi\to A up to conjugation, and in a gauge the transition maps of the covering of alignments are the link variables. (b) The gauge theorem uses only that link variables compose in a group, so it applies with Aut⁡tw(X)\Aut^{\mathrm{tw}}(X) in place of AA. A homomorphism from a free group lifts along a surjection, generator by generator.

Example(The cube roots of two)

Let K=Q(23,ω)K=\Q(\sqrt[3]2,\omega), ω=e2πi/3\omega=e^{2\pi i/3}, with group G≅S3G\cong S_3. The fields Q(23)\Q(\sqrt[3]2), Q(ω23)\Q(\omega\sqrt[3]2) and Q(ω223)\Q(\omega^2\sqrt[3]2) are the fixed fields of the three subgroups of order 2. They are three incarnations of the object S3/C2S_3/C_2, which is rigid because C2C_2 is self-normalizing. So between two of them there is exactly one Q\Q-isomorphism, such as 23↦ω23\sqrt[3]2\mapsto\omega\sqrt[3]2, and these compose coherently. The field Q(ω)=KC3\Q(\omega)=K^{C_3} has automorphism group N(C3)/C3≅C2N(C_3)/C_3\cong C_2, complex conjugation. The description Q(ω)⊂K\Q(\omega)\subset K forgets the three cube roots of 2, which form the fibre C3C_3 of S3→S3/C3S_3\to S_3/C_3.

Remark(What the language of seams adds)

Everything in the Galois-categorical reading is classical: Galois categories, the Galois theory of fields in this form, categorical Galois theory, non-abelian H1H^1 and twisted forms, and gerbes. What the language of seams adds is an emphasis, not a theorem. Several theories meet one connected object through different pointed Galois categories (CΓ,FΓ)(\mathcal C_\Gamma,F_\Gamma), joined by markings, and the subject is the isomorphisms that those theories single out and whether they cohere. A Galois category contains every isomorphism between two incarnations and prefers none. Which ones a construction picks out, and whether the picks commute around a cycle, are data that the Galois category does not contain. Likewise the statuses of a bridge record knowledge, not structure.