nLab
frame bundle

Frame and coframe bundles

Definitions

Given a k-vector bundle p:EM of finite rank n, its frame bundle (or bundle of frames in EM) is the bundle FEM over the same base whose fiber over xM is the set of all vector space bases of E x=p 1(x). The frame bundle has a natural action of GL n(k) given by an ordered change of basis which is free and transitive, i. e., the frame bundle is a principal GL n(k)-bundle.

The frame bundle of a manifold M is the principal bundle FTMM (also denoted FMM) of frames in the tangent bundle TM.

In the finite-dimensional case, the dual GL n-principal bundle (FT) *M is the coframe bundle of the manifold. This means that F *M=(FT) *M is the associated bundle to FTM× GL n(k)GL n(k) where the left action of GL n(k) on GL n(k) is given by right multiplication by inverses g.h=hg 1. Also FTM(FT) *M× GL n(k)GL n(k) using the same formula. Furthermore, the right action of GL n(k) on this associated bundle is given by left multiplication by inverses on GL n(k) factor.

Coframe bundle F *M has the following independent description. One looks at the set 𝒰(M) of tuples of the form (p,(U,h)) where pU and (U,h) is chart of the smooth structure on M, UM, h:UR n (an atlas where U-s make a basis of topology suffices). GL n(k) acts on the right on 𝒰(M) by

(p,(U,h))A:=(p,(U,A 1h)).(p, (U, h)) A := (p, (U, A^{-1} h)).

Then ((p,(U,h))A)A=(p,(U,h))(AA) holds. The total space F *M of the coframe bundle by the definition, as a set, consists of classes of equivalence of tuples in 𝒰(M) where (p,(U,h))(p,(U,h)) iff p=p and the Jacobian matrix of the transition between charts at h(p) is the unit matrix: J h(p)(h(h) 1)=I. The left action of GL n(k) is induced on the quotient. There is an obvious projection π:[(p,(U,h)]p. To define the differential and principal bundle structure one charts F *MM with local trivializations from the neighborhoods of the form U×GL n(k), transfers the structure and checks that the transition functions are of the appropriate smoothness class and right GL n(k)-equivariant. The basic prescription is that to every chart (U,h) one defines a map

ϕ h=π 1(U)U×GL n(k),z(π(z),J h(π(z))(hh 1)),\phi_{h} = \pi^{-1}(U)\to U \times GL_n(k),\,\,\,\,\,\,z\mapsto (\pi(z), J_{h(\pi(z))}(h'\circ h^{-1})),

where z=[(π(z),(U,h))] with π(z)UU. This does not depend on the choice of the chart (U,h) around π(z). There is an equivariance

J h(π(zA))(hh 1))=A 1J h(π(z))(hh 1))J_{h(\pi(z A))}(h'\circ h^{-1})) = A^{-1} J_{h(\pi(z))}(h'\circ h^{-1}))

and on intersection of (U,h) and (V,g)

J h(π(z))(hh 1))=J g(π(z))(hg 1)J h(π(z))(gh 1)J_{h(\pi(z))}(h'\circ h^{-1})) = J_{g(\pi(z))}(h'\circ g^{-1})J_{h(\pi(z))}(g\circ h^{-1})

Then ϕ h is onto and

(ϕ h(ϕ g) 1)(p,A)=(p,AJ h(p)(gh 1)(\phi_h \circ (\phi_g)^{-1})(p,A) = (p, A J_{h(p)}(g\circ h^{-1})

what shows that the transition functions are smooth (where GL n(k) has the standard differential structure).

References

Revised on November 30, 2011 23:57:28 by Zoran Škoda (161.53.130.104)