nLab
twisted bundle

Idea

A twisted principal-bundle is the object classified by a cocycle in twisted cohomology the way an ordinary principal bundle is the object classified by a cocycle in plain cohomology (generally in nonabelian cohomology).

For Ĝ a group, a Ĝ-principal bundle is classified in degree 1 nonabelian cohomology with coefficients in the delooped groupoid BĜ.

Given a realization of Ĝ as an abelian extension

AĜGA \to \hat G \to G

of groups, i.e. given a fibration sequence

BABĜBG\mathbf{B}A \to \mathbf{B}\hat G \to \mathbf{B}G

of groupoids such that BA is once deloopable so that the fibration sequence continues to the right at least one step as

BĜBGB 2A\mathbf{B}\hat G \to \mathbf{B}G \to \mathbf{B}^2 A

the general nonsense of twisted cohomology induces a notion of twisted Ĝ-cohomology. The fibrations classified by this are the twisted Ĝ-bundles.

Definition

For every B 2A-cocycle cH(X,B 2A) the c-twisted Ĝ-cohomology H c(X,GĜ) is the homotopy pullback

H c(X,BĜ) * c H(X,BG) H(X,B 2A).\array{ \mathbf{H}^c(X,\mathbf{B}\hat G) &\to& {*} \\ \downarrow && \downarrow^{c} \\ \mathbf{H}(X,\mathbf{B}G) &\stackrel{}{\to}& \mathbf{H}(X,\mathbf{B}^2 A) } \,.

The cocycles in H c(X,BĜ) are called the (representatives of) c-twisted Ĝ-principal bundles.

Details

One may unwrap this abstract definition to obtain a concrete cocycle formula for twisted bundles.

For that purpose the above homotopy pullback is conveniently computed as an ordinary pullback after making the fibrant replacement

H(X,B(AĜ)) H(X,B 2A) * Id Id H(X,BG) H(X,B 2A) *,\array{ \mathbf{H}(X,\mathbf{B}(A \to \hat G)) &\to & \mathbf{H}(X,\mathbf{B}^2 A) &\leftarrow& {*} \\ \downarrow^{\simeq} && \downarrow^{Id} && \downarrow^{Id} \\ \mathbf{H}(X,\mathbf{B}G) &\to & \mathbf{H}(X,\mathbf{B}^2 A) &\leftarrow& {*} } \,,

where (AĜ) denotes the 2-group corresponding to the crossed module obtained from the central extension Ĝ.

Similarly identifying B 2A=B(A1) as the delooping of the 2-group coming from the crossed module (A1) the morphism H(X,B(AG))H(X,B 2A) is now induced from the obvious projection of crossed modules

(AG)(A1).(A \to G) \to (A \to 1) \,.

This then says that c-twisted BĜ-cocycles are precisely those B(AĜ)-cocycles whose projection to an B(A1)-cocycle is the prescribed twisting cocycle c.

We may consider a Čech cocycle relative to a cover {U iX}, i.e. an anafunctor

C(U) ĝ tw B(AĜ) X\array{ C(U) &\stackrel{\hat g_{tw}}{\to}& \mathbf{B}(A \to \hat G) \\ \downarrow \\ X }

out of a Čech nerve C(U) and notice that the functor ĝ tw is an assignment

ĝ tw: (x,j) (x,i) (x,k) ĝ ij(x) c ijk(x) ĝ jk(x) ĝ ik(x) \hat g_{tw} \;\; : \;\; \array{ && (x,j) \\ & \nearrow &\Downarrow& \searrow \\ (x,i) &&\to&& (x,k) } \;\;\;\; \mapsto \;\;\;\; \array{ && \bullet \\ & {}^{\hat g_{i j}(x)}\nearrow &\Downarrow^{c_{i j k}(x)}& \searrow^{\hat g_{j k}(x)} \\ \bullet &&\stackrel{\hat g_{i k}(x)}{\to}&& \bullet }

As already indicated by the notation, the further projection

C(U)ĝ twB(AĜ)B 2AC(U) \stackrel{\hat g_{tw}}{\to} \mathbf{B}(A \to \hat G) \to \mathbf{B}^2 A

is constrained to be the cocycle c. Using the rules for crossed modules one reads off that the existence of the triangular cell on the right in B(AĜ) is equivalent to the equation

ĝ ij(x)ĝ jk(x)=ĝ ik(x)c ijk(x).\hat g_{i j}(x) \hat g_{j k}(x) = \hat g_{i k}(x) c_{i j k}(x) \,.

In this cocycle equation form twisted bundles traditionally appear in the literature. Alternatively, allowing a general surjective submersion instead of an open cover, this yields the description of twisted bundles as prefered in the literature on bundle gerbes, where they are called bundle gerbe modules: the B 2A-cocycle c represents the A-bundle gerbe.

Examples

twisted K-theory

Just as vector bundles model cocycles in K-theory, twisted vector bundles model cocycles in twisted K-theory.

For twists c that are torsion class (i.e. have finite order as group elements in the cohomology group H(X,B 2A) ) this was realized in

  • P. Bouwknegt, A. L. Carey, V. Mathai, M. K. Murray, D. Stevenson, Twisted K-theory and K-theory of bundle gerbes (arXiv)

which also, apparently, is the source where gerbe modules as such were first introduced.

The generalization of this construction to non-torsion twists requires using vectorial bundles instead of plain vector bundles. Full twisted K-theory in terms of twisted vectorial bundles was realized in

  • Kiyonori Gomi, Twisted K-theory and finite-dimensional approximation (arXiv)

There the twisted cocycle equation discussed above appears on the bottom of page 7.