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For AA a monoid equipped with an action on an object VV (often: a group with a group action on VV), an invariant of the action is an element of VV which is taken by the action to itself, hence which is a fixed point for all the operations of the monoid.

Definitions

A robust definition of invariants that generalizes to homotopy theory is via the expression of actions as action groupoids regarded as sitting over delooping groupoids, as discussed at infinity-action and at geometry of physics – representations and associated bundles.

We describe how the ordinary concept of invariants is recovered from this perspective and then consider its immediate generalizations to (infinity,1)-topos theory and its formalization in homotopy type theory.

Via sections of action groupoid projections

Proof

The sections in question are diagrams in Grpd of the form

BG ⟶σ S//G id↘ ⇙ ≃ ↙ p ρ BG, \array{ \mathbf{B}G && \stackrel{\sigma}{\longrightarrow} && S//G \\ & {}_{\mathllap{id}}\searrow &\swArrow_{\mathrlap{\simeq}}& \swarrow_{\mathrlap{p_\rho}} \\ && \mathbf{B}G } \,,

hence the groupoid which they form is equivalently the hom-groupoid

Grpd /BG(id BG,p ρ)∈Grpd Grpd_{/\mathbf{B}G}(id_{\mathbf{B}G}, p_\rho) \in Grpd

in the slice of Grpd over BG\mathbf{B}G. As in the proof of this proposition, with the fibrant presentation (p ρ) •(p_\rho)_\bullet of this proposition, this is equivalently given by strictly commuting diagrams of the form

(BG) • ⟶σ • (S//G) • id •↘ = ↙ (p ρ) • (BG) •. \array{ (\mathbf{B}G)_\bullet && \stackrel{\sigma_\bullet}{\longrightarrow} && (S//G)_\bullet \\ & {}_{\mathllap{id_\bullet}}\searrow &=& \swarrow_{\mathrlap{(p_\rho)_\bullet}} \\ && (\mathbf{B}G)_\bullet } \,.

These σ\sigma now are manifestly functors that are the identity on the group labels of the morphisms

σ •:(* ↓ g *)↦(σ(*) ↓ g σ(*) =ρ(σ(*)(g))). \sigma_\bullet \;\colon\; \left( \array{ \ast \\ \downarrow^{\mathrlap{g}} \\ \ast } \right) \;\; \mapsto \;\; \left( \array{ \sigma(\ast) \\ \downarrow^{\mathrlap{g}} \\ \sigma(\ast) & = \rho(\sigma(\ast)(g)) } \right) \,.

This shows that they pick precisely those elements σ(*)∈S\sigma(\ast) \in S which are fixed by the GG-action ρ\rho.

Moreover, since these functors are identity on the group labels, there are no non-trivial natural isomorphisms between them, and hence the groupoid of sections is indeed a set, the set of invariant elements.

More generally, we may consider sections of these groupoid projections after pulling them back along some cocycle:

Proposition

Given an associated bundle P× GV→XP \times_G V\to X modulated, as in this proposition, by a morphism of smooth groupoids of the form g:X⟶BGg \colon X \longrightarrow \mathbf{B}G, then its set of sections is equivalently the groupoid of diagrams

X ⟶σ S//G g↘ ⇙ ≃ ↙ p ρ BG, \array{ X && \stackrel{\sigma}{\longrightarrow} && S//G \\ & {}_{\mathllap{g}}\searrow &\swArrow_{\mathrlap{\simeq}}& \swarrow_{\mathrlap{p_\rho}} \\ && \mathbf{B}G } \,,

hence the groupoid of sections is the slice hom-groupoid

Γ X(P× GV)≃Grpd /BG(g,p ρ). \Gamma_X(P\times_G V) \simeq Grpd_{/\mathbf{B}G}(g, p_\rho) \,.

Invariants of ∞\infty-group actions

For H\mathbf{H} an (∞,1)-topos, G∈Grp(H)G \in Grp(\mathbf{H}) an ∞-group and

*:BG⊢:V(*):Type * : \mathbf{B} G \vdash : V(*) : Type

an ∞-action of GG on V∈HV \in \mathbf{H}, the type of invariants is the absolute dependent product

⊢∏ *:BGV(*):Type. \vdash \prod_{* : \mathbf{B}G} V(*) : Type \,.

The connected components of this is equivalently the group cohomology of GG with coefficients in the infinity-module VV.

Properties

Proof

Since the ground field has characteristic zero, group averaging exists and provides a linear map

V • ⟶p V • G x ↦ 1|G|∑g∈Gg(x) \array{ V_\bullet & \overset{p}{\longrightarrow} & V_\bullet^G \\ x &\mapsto& \frac{1}{{\vert G \vert}} \underset{g \in G}{\sum} g(x) }

onto the GG-invariants.

Now for a chain homology-class [x]∈H •((V •,∂))[x] \in H_\bullet((V_\bullet,\partial)) being GG-invariant means that g[x]≔[g(x)]=[x]g[x] \coloneqq [g(x)] = [x] for all g∈Gg \in G, which implies that [x]=[p(x)][x] = [p(x)]. This means that each invariant homology class has an invariant representative, hence that the map from invariant cycles to invariant chain homology-classes

Z((V • G,∂))⟶H •((V •,∂)) Z((V_\bullet^G,\partial)) \longrightarrow H_\bullet((V_\bullet,\partial))

is an epimorphism.

Next consider the kernel of this map, which a priori is Z((V • G,∂))∩B((V •,∂))Z((V_\bullet^G,\partial)) \cap B((V_\bullet,\partial)). It is now sufficient to show that this coincides with the space of GG-invariant boundaries:

Z((V • G,∂))∩B((V •,∂))≃B((V • G,∂)). Z((V_\bullet^G,\partial)) \cap B((V_\bullet,\partial)) \;\simeq\; B((V_\bullet^G, \partial)) \,.

It is clear that there is an inclusion

B((V • G,∂))↪Z((V • G,∂))∩B((V •,∂)) B((V_\bullet^G, \partial)) \hookrightarrow Z((V_\bullet^G,\partial)) \cap B((V_\bullet,\partial))

so it only remains to see that this is also a surjection.

To that end, consider any

x∈Z((V • G,∂))∩B((V •,∂)). x \in Z((V_\bullet^G,\partial)) \cap B((V_\bullet,\partial)) \,.

Since in particular x∈B((V •,∂))x \in B((V_\bullet,\partial)), there is y∈V •y \in V_\bullet with x=∂yx = \partial y; and since moreover x∈V •(G)x \in V_\bullet(G), the above implies that

x=p(x)=p(∂y)=∂(py) x = p(x) = p(\partial y) = \partial(p y)

and hence that

x∈B((V • G,∂)). x \in B((V_\bullet^G,\partial)) \,.

Examples

Last revised on July 12, 2024 at 08:49:09. See the history of this page for a list of all contributions to it.