nLab
infinity-action

Contents

Idea

The notion of -action is the notion of action (module/representation) in homotopy theory/(∞,1)-category theory, from algebra to higher algebra.

Notably a monoid object in an (∞,1)-category A may act on another object N by a morphism ANN which satisfies an action property up to coherent higher homotopy.

If the -action is suitably linear in some sense, this is also referred to as ∞-representation.

Definition

We discuss the actions of ∞-groups in an (∞,1)-topos. (For groupoid ∞-actions see there.)

Let H be an (∞,1)-topos.

Let GGrp(H) be an group object in an (∞,1)-category in H, hence a homotopy-simplicial object on H of the form

(G×GG*)\left( \cdots \stackrel{\to}{\stackrel{\to}{\stackrel{\to}{\to}}} G \times G \stackrel{\to}{\stackrel{\to}{\to}} G \stackrel{\to}{\to} * \right)

satisfying the groupoidal Segal conditions.

hence an ∞-group.

Definition

An action (or -action, for emphasis) of G on an object VH is a groupoid object in an (∞,1)-category which is equivalent to one of the form

(V×G×GV×Gp 1ρV)\left( \cdots \stackrel{\to}{\stackrel{\to}{\stackrel{\to}{\to}}} V \times G \times G \stackrel{\to}{\stackrel{\to}{\to}} V \times G \stackrel{\overset{\rho}{\to}}{\underset{p_1}{\to}} V \right)

such that the projection maps

V×G×G V×G p 1ρ V G×G G *\array{ \cdots &\stackrel{\to}{\stackrel{\to}{\stackrel{\to}{\to}}}& V \times G \times G &\stackrel{\to}{\stackrel{\to}{\to}}& V \times G &\stackrel{\overset{\rho}{\to}}{\underset{p_1}{\to}}& V \\ && \downarrow && \downarrow && \downarrow \\ \cdots &\stackrel{\to}{\stackrel{\to}{\stackrel{\to}{\to}}}& G \times G &\stackrel{\to}{\stackrel{\to}{\to}}& G &\stackrel{\overset{}{\to}}{\underset{}{\to}}& * }

constitute a morphism of groupoid objects VG*G.

The (∞,1)-category of such actions is the slice of groupoid objects over *G on these objects.

There is an equivalent formulation which does not invoke the notion of groupoid object in an (∞,1)-category explicitly. This is based on the fundamental fact, discussed at ∞-group, that delooping constitutes an equivalence of (∞,1)-categories

B:Grp(H)H 1 */.\mathbf{B} : Grp(\mathbf{H}) \to \mathbf{H}^{*/}_{\geq 1} \,.

form group objects in an (∞,1)-category to the (∞,1)-category of connected pointed objects in H.

Proposition

Every -action ρ:V×GV has a classifying morphism c ρ:V//GBG in that there is a fiber sequence

V V//G ρ¯ BG\array{ V \\ \downarrow \\ V//G &\stackrel{\overline{\rho}}{\to}& \mathbf{B}G }

such that ρ is the G-action on V regarded as the corresponding G-principal ∞-bundle modulated by ρ¯.

This allows to characterize -actions in the following convenient way. See (NSS) for a detailed discussion.

Definition

For VH an object, a G--action ρ on V is a fiber sequence in H of the form

V VG ρ¯ BG.\array{ V &\to& V \sslash G \\ && \downarrow^{\mathrlap{\overline{\rho}}} \\ && \mathbf{B}G } \,.

The (∞,1)-category of G-actions in H is the slice (∞,1)-topos of H over BG:

Act H(G)H /BG.Act_{\mathbf{H}}(G) \coloneqq \mathbf{H}_{/\mathbf{B}G} \,.
Remark

A ρAct H(G) corresponds to a morphism denoted ρ¯:VGBG in H hence to an object ρ¯H /BG.

A morphism ϕ:ρ 1ρ 2 in Act H(G) corresponds to a diagram

V 1G V 2G ρ 1¯ ρ 2¯ BG\array{ V_1 \sslash G &&\stackrel{}{\to}&& V_2 \sslash G \\ & {}_{\mathllap{\overline{\rho_1}}}\searrow && \swarrow_{\mathrlap{\overline{\rho_2}}} \\ && \mathbf{B}G }

in H.

Remark

The bundle ρ¯ in def. 2 is the universal ρ-associated V-fiber ∞-bundle.

Remark

In the form of def. 2 -actions have a simple formulation in the internal language of homotopy type theory: a G-action on V is simply a dependent type over BG with fiber V:

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

Notions in higher representation theory

We discuss some basic representation theoretic notions of -actions.

In summary, for c:BGV(c):Type an action of G on V, we have

  • the dependent sum

    c:BGV(c):Type\vdash \sum_{\mathbf{c} : \mathbf{B}G} V(\mathbf{c}) : Type

    is the quotient VG of V by G;

  • the dependent product

    c:BGV(c):Type\vdash \prod_{\mathbf{c} : \mathbf{B}G} V(\mathbf{c}) : Type

    is the collection of invariants of the actions.

And for V 1,V 2 two actions we have

Invariants

Definition

The invariants of a G--action are the sections of the morphism VGBG,

Invariants(V)= BG*(VGBG),Invariants(V) = \prod_{\mathbf{B}G \to *} (V \sslash G \to \mathbf{B}G) \,,

where BG*:H /BGH is the direct image of the base change geometric morphism.

In homotopy type theory syntax: for

c:BGV(c):Type\mathbf{c} : \mathbf{B}G \vdash V(\mathbf{c}) : Type

an action as in remark 3, its type of invariants is the dependent product

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

Quotients

From def. 2 we read off:

Definition

The quotient of a G-action

c:BGV(c):Type\mathbf{c} : \mathbf{B}G \vdash V(\mathbf{c}) : Type

is the dependent sum

c:BGV(c):Type.\vdash \sum_{\mathbf{c} : \mathbf{B}G} V(\mathbf{c}) : Type \,.

Conjugation actions

Remark

By def. 2, and basic facts disussed at slice (∞,1)-topos, the (∞,1)-category Act H(G) is an (∞,1)-topos and in particular is a cartesian closed (∞,1)-category.

We describe here aspects of the cartesian product and internal hom of -actions given this way. The following statements are essentially immediate consequences of basic homotopy type theory.

Proposition

For (V 1,ρ 1),(V 2,ρ 2)Act(G) their cartesian product is a G-action on the product of V 1 with V 2 in H.

Proof

Let

V i VG ρ¯ i BG\array{ V_i &\to& V\sslash G \\ && \downarrow^{\bar \rho_i} \\ && \mathbf{B}G }

be the principal ∞-bundles exhibiting the two actions.

Along the lines of the discussion at locally cartesian closed category we find that (V 1,ρ 1)×(V 2,ρ 2)Act(G) is given in H by the (∞,1)-pullback

BGρ¯ 1×ρ¯ 2V 1G× BGV 2G\sum_{\mathbf{B}G} \bar \rho_1 \times \bar \rho_2 \simeq V_1\sslash G \times_{\mathbf{B}G} V_2 \sslash G

in H, with the product action being exhibited by the principal ∞-bundle

V 1×V 2 V 1G× BGV 2G ρ 1×ρ 2¯ BG.\array{ V_1 \times V_2 &\to& V_1\sslash G \times_{\mathbf{B}G} V_2 \sslash G \\ && \downarrow^{\mathrlap{\overline{ \rho_1 \times \rho_2 }}} \\ && \mathbf{B}G } \,.

Here the homotopy fiber on the left is identified as V 1×V 2 by using that (∞,1)-limits commute over each other.

Proposition

For ρ 1,ρ 2Act(G) their internal hom [ρ 1,ρ 2]Act H(G) is a G-action on the internal hom [V 1,V 2]H.

Proof

Taking fibers

pt BG *:H /BGHpt_{\mathbf{B}G}^* : \mathbf{H}_{/\mathbf{B}G} \to \mathbf{H}

is the inverse image of an etale geometric morphism, hence is a cartesian closed functor (see the Examples there for details). Therefore it preserves exponential objects:

pt BG *[ρ¯ 1,ρ¯ 2] [pt BG *ρ¯ 1,pt BG *ρ¯ 2] [V 1,V 2].\begin{aligned} pt_{\mathbf{B}G}^* [\bar \rho_1, \bar \rho_2] & \simeq [pt_{\mathbf{B}G}^* \bar \rho_1, pt_{\mathbf{B}G}^* \bar \rho_2] \\ & \simeq [V_1, V_2] \end{aligned} \,.
Remark

The above internal-hom action

[V 1,V 2] V 1G× BGV 2G [ρ 1,ρ 2]¯ BG\array{ [V_1,V_2] &\to& V_1 \sslash G \times_{\mathbf{B}G} V_2 \sslash G \\ && \downarrow^{\mathrlap{\overline{[\rho_1,\rho_2]}}} \\ && \mathbf{B}G }

encodes the conjugation action of G on [V 1,V 2] by pre- and post-composition of functions V 1V 2 with the G-action on V 1 and on V 2, respectively.

See also at Conjugation actions below.

Internal object of homomorphisms

Remark

The invariant, def. 3 of the conjugation action, prop. 3 are the action homomorphisms. (See also at Examples - Conjugation actions).

Therefore

Definition

For ρ¯ i:V iGBG two G-actions, the object of homomorphisms is

BG*[ρ¯ 1,ρ¯ 2]H.\prod_{\mathbf{B}G \to *}[\bar \rho_1, \bar \rho_2] \in \mathbf{H} \,.

In the syntax of homotopy type theory

c:BGV 1(c)V 2(c):Type.\vdash \prod_{\mathbf{c} : \mathbf{B}G} V_1(\mathbf{c}) \to V_2(\mathbf{c}) : Type \,.

Stabilizer subgroups

See at stabilizer subgroup.

Examples

Of -group actions in an -topos

Let H be an (∞,1)-topos and let GGrp(H) be an ∞-group in H.

The following lists some fundamental classes of examples of -actions of G, and of other canonical -groups. By the discussion above these actions may be given by the classifying morphisms.

Trivial action

Consider the étale geometric morphism

Act H(G)H /BGp *()×BGH.Act_{\mathbf{H}}(G) \coloneqq \mathbf{H}_{/\mathbf{B}G} \stackrel{\overset{p^* \coloneqq (-) \times \mathbf{B}G}{\leftarrow}}{\underset{}{\to}} \mathbf{H} \,.
Definition

For VH any object, the trivial action of G on V is p *VAct H(G), exhibited by the split fiber sequence

V V×BG BG.\array{ V &\to& V \times \mathbf{B}G \\ && \downarrow \\ && \mathbf{B}G } \,.

Fundamental action

The right -action of G on itself is given by the fiber sequence

G * BG\array{ G \\ \downarrow \\ * &\to& \mathbf{B}G }

which exhibits BG as the delooping of G.

G//G*.G//G \simeq * \,.

Adjoint action

The fiber sequence

G BG ev * BG\array{ G \\ \downarrow \\ \mathcal{L} \mathbf{B}G &\stackrel{ev_*}{\to}& \mathbf{B}G }

given by the free loop space object BG exhibits the higher adjoint action of G on itself:

G// AdGBG.G//_{Ad}G \simeq \mathcal{L}\mathbf{B}G \,.

Automorphism action

Definition

For VH any object, there is a canonical action of the internal automorphism infinity-group Aut(V):

V V//Aut(V) BAut(V)\array{ V \\ \downarrow \\ V//\mathbf{Aut}(V) &\to& \mathbf{B} \mathbf{Aut}(V) }

Conjugation actions

We discuss the simple case of the cartesian closed category of G-sets (G-permutation representations) for G an ordinary discrete group as a simple illustration of the internal hom of -actions, prop. 3.

This example spells out everything completely in components:

Example

Let H= ∞Grpd, let GGrp(Grpd) be an ordinary discrete group and let V,Σ,X be sets equipped with G-action (permutation representations).

In this case [Σ,X] is simply the set of functions f:ΣX of sets. Its G-action as the internal hom of G-actions given, for every gG and σΣ, by

g(f)(σ)=g(f(g 1(σ))),g(f)(\sigma) = g(f(g^{-1}(\sigma))) \,,

(where we write generically g() for the given action on the set specified implicitly by the type of the argument).

Hence a morphism of G-actions

ϕ:V[Σ,X]\phi : V \to [\Sigma,X]

is a function ϕ of the underlying sets such that for all VV, gG and all σΣ we have

(1)ϕ(g(v))(σ)=g(ϕ(v)(g 1(σ)).\phi(g(v))(\sigma) = g(\phi(v)(g^{-1}(\sigma)) \,.

On the other hand, a morphism of actions

ψ:V×ΣX\psi : V \times \Sigma \to X

is a function of the underlying sets, such that for all these terms we have

ψ(g(v),g(σ))=g(ψ(v,σ))\psi(g(v), g(\sigma)) = g(\psi(v,\sigma))

which is equivalent to

(2)ψ(g(v),σ)=g(ψ(v,g 1(σ))).\psi(g(v), \sigma) = g(\psi(v,g^{-1}(\sigma))) \,.

Comparison of (1) and (2) shows that the identification

ψ(v,σ)ϕ(v)(σ)\psi(v,\sigma) \coloneqq \phi(v)(\sigma)

establishes a natural equivalence (a natural bijection of sets in this case)

Act H(G)(V,[Σ,X])Act H(G)(V×Σ,X]),Act_{\mathbf{H}}(G)(V, [\Sigma,X]) \simeq Act_{\mathbf{H}}(G)(V \times \Sigma, X]) \,,

showing how [Σ,X] is indeed the internal hom of G-actions.

Remark

Generally, for G a discrete ∞-group we have an equivalence of (∞,1)-categories

Grpd /BGFunc(BG,Grpd)\infty Grpd_{/\mathbf{B}G} \simeq \infty Func(\mathbf{B}G, \infty Grpd)

(by the (∞,1)-Grothendieck construction), and hence

Act Grpd(G)Func(BG,Grpd)Act_{\infty Grpd}(G) \simeq \infty Func(\mathbf{B}G, \infty Grpd)

is the (∞,1)-category of ∞-permutation representations.

General covariance

Let XH be a moduli infinity-stack for field in a gauge theory or sigma-model. Let ΣH be the corresponding spacetime or worldvolume, respectively.

We have the automorphism action, def. 7

Σ ΣAut(Σ) BAut(Σ).\array{ \Sigma &\to& \Sigma \sslash \mathbf{Aut}(\Sigma) \\ && \downarrow \\ && \mathbf{B} \mathbf{Aut}(\Sigma) } \,.

The slice H /Aut(Σ)=Act H(Aut(Σ)) is the context of types which are generally covariant over Σ.

On X consider the trivial Aut(Σ)-action, def. 6. Then the internal-hom action of prop. 3

[Σ,X]Aut(Σ)[ΣAut(Σ),X×BAut(Σ)] BAut(Σ)[\Sigma, X]\sslash \mathbf{Aut}(\Sigma) \simeq [\Sigma \sslash \mathbf{Aut}(\Sigma), X \times \mathbf{B}\mathbf{Aut}(\Sigma)]_{\mathbf{B}\mathbf{Aut}(\Sigma)}

is the configuration space of fields on Σ modulo automorphisms (diffeomorphisms, in smooth cohesion) of Σ. This is the configuration space of “generally covariant” field theory on Σ.

Semidirect product groups

Let G,AGrp(H) be 0-truncated group objects and let ρ be an action of G on A by group homomorphisms. This is equivalently an action of G on BA, hence a fiber sequence

BA B(GA) BG.\array{ \mathbf{B}A &\to& \mathbf{B} (G \ltimes A) \\ && \downarrow \\ && \mathbf{B}G } \,.

The corresponding action groupoid (BA)GB(GA) is the delooping of the corresponding semidirect product group.

G-Modules

Definition

For GGrp(H) the -category of G-modules is

Stab(H /BG)Stab(GAct),Stab( \mathbf{H}_{/\mathbf{B}G}) \simeq Stab(G Act) \,,

the stabilization of the -category of G-actions.

Example

For G and A 0-truncated groups, A an abelian group with G-module structure, the semidirect product group GA from above exhibits A as a G-module in the sense of def. 8.

References

Actions of A-∞ algebras in some symmetric monoidal (∞,1)-category are discussed in section 4.2 of

Aspects of actions of ∞-groups in an ∞-topos in the contect of associated ∞-bundles are discussed in section I 4.1 of

Revised on April 3, 2013 14:22:10 by Urs Schreiber (82.169.65.155)