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Lie infinity-algebroid representation

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This entry discusses the conceptual notion of representations of Lie ∞-algebroids and their realization in terms of modules for differential graded algebras and of modules of differential graded coalgebras. See the remarks at rational homotopy theory and Lie theory for background on the Lie-theoretic interpretation differential graded (co)algebra.

Contents

Idea

Recall that an L -algebroid is both a horizontal categorification as well as a vertical categorification of a Lie algebra: it is to Lie algebras as Lie ∞-groupoids are to Lie groups.

Accordingly, the notion of representation of a Lie--algebroid is a horizontal and vertical categorification of the ordinary notion of representation of a Lie algebra, which in turn is the linearization of the notion of representation of a Lie group.

In view of this notice that there are essentially two fundamental ways to express the notion of representation of a group or ∞-groupoid Gr:

  1. as a morphism out of Gr: the action;

  2. as a fibration sequence over Gr: the action groupoid.

While essentially equivalent, it is noteworthy that the first definition naturally takes place in the context of not-necessarily smooth (-)categories, while the second one usually remains within the context of smooth ()-groupoids:

namely for G a Lie group, for definiteness and for simplicity, with corresponding one-object Lie groupoid BG – the delooping of the group G –, a linear representation in terms of an action morphisms is a functor

ρ:BGVect\rho : \mathbf{B} G \to Vect

from BG to the category of vector spaces. In fact, there is a canonical equivalence of the functor category [BG,Vect] with the category Rep(G) of linear representations of G

[BG,Vect]Rep(G).[\mathbf{B}G, Vect] \simeq Rep(G) \,.

Every such functor ρ induces a fibration sequence V//GBG over BG, obtained as the pullback of the generalized universal bundle Vect *Vect along ρ

V//G Vect * BG ρ Vect.\array{ V//G &\to& Vect_* \\ \downarrow && \downarrow \\ \mathbf{B}G &\stackrel{\rho}{\to}& Vect } \,.

Here V//G is the action groupoid of the action of ρ on the representation vector space V:=ρ(), where is the single object of BG. This vector space, regarded as a discrete category on its underlying set, is the fiber of this fibration, so that the action gives rise to the fiber sequence

VV//GBG.V \hookrightarrow V//G \to \mathbf{B}G \,.

As described at generalized universal bundle, this may be thought of as (the groupoid incarnation of) the vector bundle which is associated via ρ to the universal G-bundle EGBG, which itself is the action groupoid of the fundamental representation? of G on itself,

G EG BG = = = G G//G BG.\array{ G &\hookrightarrow& \mathbf{E}G &\to& \mathbf{B}G \\ = && = && = \\ G &\hookrightarrow& G//G &\to& \mathbf{B}G } \,.

From this perspective a representation of a group G is nothing but a G-equivariant vector bundle over the point, or equivalently a vector bundle on the orbifold //G. So from this perspective the notion “representation” is not a primitive notion, but just a particular perspective on fibration sequences.

The definition of Lie- algebroid representation below is in this fibration sequence/fibration-theoretic/action groupoid spirit. The expected alternative definition in terms of action morphisms has been considered (and is well known) apparently only for special cases.

Definition

Recall that we take, by definition, Lie ∞-algebroids to be dual to non-negatively-graded, graded-commutative differential algebras, which are free as graded-commutative algebras (qDGCAs): we write CE A(g) for the qDGCA whose underlying graded-commutative algebra is the free (over the algebra A) graded commutative algebra g * for g a non-postively graded cochain complex of A-modules and g * its degree-wise dual over A, to remind us that this is to be thought of as the Chevalley-Eilenberg algebra of the Lie ∞-algebroid g whose space of objects is characterized dually by the algebra A.

The category DGCAs is naturally equipped with the model structure on differential graded algebras?.

Definition

A representation ρ of a Lie -algebroid (g,A) on a co-chain complex V of A-modules is a cofibration sequence

VCE ρ(g,V)CE A(g)\wedge^\bullet V \leftarrow CE_\rho(g,V) \leftarrow CE_A(g)

in DGCAs, i.e. a homotopy pushout

V CE ρ(g) 0 CE A(g).\array{ \wedge^\bullet V &\leftarrow& CE_\rho(g) \\ \uparrow && \uparrow \\ 0 &\leftarrow & CE_A(g) } \,.

What has been considered in the literature so far is the more restrictive version, where the pushout is taken to be strict (Urs: at least I think that this is the right way to say it):

A proper representation ρ is a strict cofiber sequence of morphisms of DGCAs

VCE ρ(g,V)CE A(g)\wedge^\bullet V \leftarrow CE_\rho(g,V) \leftarrow CE_A(g)

i.e. such that

  • CE ρ(g,V)=CE A(g) V as GCAs

  • VCE ρ(g,V) is the obvious surjection;

  • CE ρ(g,V)CE A(g) is the obvious injection;

  • the composite of both is the 0-map.

It follows that the differential d ρ on CE ρ(g,V) is given by a twisting map ρ *:V( V)(g *)( g *) as

  • d ρ g *=d g

  • d ρ V=d V+ρ *

which may be thought of as the dual of the representation morphism (see the examples below).

DG-category of Lie--algebroid representations

In

  • Jonathan Block, Duality and equivalence of module categories in noncommutative geometry I (arXiv)

the dg-category Rep(g,A) of proper representations of a Lie--algebroid (g,A) in the above sense – called dg-algebra modules there – is defined.

Definition

Given two objects CE ρ(g,V) and CE ρ(g,V) in Rep(g,A), the cochain complex

Hom(CE ρ(g,V),CE ρ(g,V))

consist in degree k of morphisms of degree k

ϕ:V gV g *\phi : V \otimes \wedge^\bullet g \to V' \otimes \wedge^\bullet g^*

satisfying ϕ(vt)=(1) kaϕ(v)t

and the differential d Hom is the usual differential on hom-complexes dϕ=d ρϕ(1) ϕϕd ρ.

For a fixed Lie -algebroid (g,A), the category

Rep(g,A)Rep(g,A)

with Lie representations of (g,A) as objects and chain comoplexes as above as hom-objects is a dg-category.

relation to coherent complexes of sheaves

Theorem

For X a smooth complex manifold and (g,A)=T holX the holomorphic tangent Lie algebroid of X (so that CE A(g)=Ω hol (X) the holomorphic deRham complex of X), and for Rep(T holX) taken to have as objects complexes of finitely generated and projective C (X)-modules (i.e. complexes of smooth vector bundles) the homotopy category HoRep(T holX) of the dg-category Rep(T holX) is equivalent to the bounded derived category of complexes of sheaves with coherent cohomology on X (see coherent sheaf).

This is theorem 2.22, p. 17 of Block’s article.

The objects of Rep(T holX) are literally complexes of smooth vector bundles that are equipped with “half a flat connection”, namely with a flat covariant derivative only along holomorphic tangent vectors. It is an old result that holomorphic vector bundles are equivalent to such smooth vector bundles with “half a flat connection”. This is what the theorem is based on.

relation to D-modules

For (g,A)=TX the tangent Lie algebroid of a smooth manifold X, it should be true, up to technicalities to be spelled out here eventually, that HoRep(TX) is equivelent to the derived category of D-modules on X, or the like.

Coalgebraic formulation

Examples

  • ordinary representation of a Lie algebra on a vector space: CE ρ(g,V) is essentially the Chevalley-Eilenberg complex that computes the cohomology of g with coefficients in V.

  • flat connections on bundles

  • adjoint representation? of L -algebras

References

This definition appears in

The definition of the dg-category of dg-algebra modules and its equivalence in special cases to derived categories of coherent complexes of sheaves is in

  • Jonathan Block, Duality and equivalence of module categories in noncommutative geometry I (arXiv)

A blog discussion of this is at

The same definition, up to inessential technical details, appears also in

  • Camilo Arias Abad, Marius Crainic, Representations up to homotopy of Lie algebroids (arXiv)

Some further discussion and examples of Lie--algebroid representations is at

  • Urs Schreiber, On Lie-oo theory

  • Hisham Sati, Urs Schreiber, Jim Stasheff, Twisted differential String- and Fivebrane structures (pdf)