English

Connection (principal bundle)

In mathematics, a connection is a device that defines a notion of parallel transport on the bundle; that is, a way to 'connect' or identify fibers over nearby points. A principal G-connection on a principal G-bundle P over a smooth manifold M is a particular type of connection which is compatible with the action of the group G. In mathematics, a connection is a device that defines a notion of parallel transport on the bundle; that is, a way to 'connect' or identify fibers over nearby points. A principal G-connection on a principal G-bundle P over a smooth manifold M is a particular type of connection which is compatible with the action of the group G. A principal connection can be viewed as a special case of the notion of an Ehresmann connection, and is sometimes called a principal Ehresmann connection. It gives rise to (Ehresmann) connections on any fiber bundle associated to P via the associated bundle construction. In particular, on any associated vector bundle the principal connection induces a covariant derivative, an operator that can differentiate sections of that bundle along tangent directions in the base manifold. Principal connections generalize to arbitrary principal bundles the concept of a linear connection on the frame bundle of a smooth manifold. Let π:P→M be a smooth principal G-bundle over a smooth manifold M. Then a principal G-connection on P is a differential 1-form on P with values in the Lie algebra g {displaystyle {mathfrak {g}}} of G which is G-equivariant and reproduces the Lie algebra generators of the fundamental vector fields on P. In other words, it is an element ω of Ω 1 ( P , g ) ≅ C ∞ ( P , T ∗ P ⊗ g ) {displaystyle Omega ^{1}(P,{mathfrak {g}})cong C^{infty }(P,T^{*}Potimes {mathfrak {g}})} such that Sometimes the term principal G-connection refers to the pair (P,ω) and ω itself is called the connection form or connection 1-form of the principal connection. Most known non-trivial computations of principal G-connections are done with homogeneous spaces because of the triviality of the (co)tangent bundle. (For example, let G → H → H / G {displaystyle G o H o H/G} , be a principal G-bundle over H / G {displaystyle H/G} ) This means that 1-forms on the total space are canonically isomorphic to C ∞ ( H , g ∗ ) {displaystyle C^{infty }(H,{mathfrak {g}}^{*})} , where g ∗ {displaystyle {mathfrak {g}}^{*}} is the dual lie algebra, hence G-connections are in bijection with C ∞ ( H , g ∗ ⊗ g ) G {displaystyle C^{infty }(H,{mathfrak {g}}^{*}otimes {mathfrak {g}})^{G}} . A principal G-connection ω on P determines an Ehresmann connection on P in the following way. First note that the fundamental vector fields generating the G action on P provide a bundle isomorphism (covering the identity of P) from the bundle VP to P × g {displaystyle P imes {mathfrak {g}}} , where VP = ker(dπ) is the kernel of the tangent mapping d π : T P → T M {displaystyle {mathrm {d} }pi colon TP o TM} which is called the vertical bundle of P. It follows that ω determines uniquely a bundle map v:TP→V which is the identity on V. Such a projection v is uniquely determined by its kernel, which is a smooth subbundle H of TP (called the horizontal bundle) such that TP=V⊕H. This is an Ehresmann connection. Conversely, an Ehresmann connection H⊂TP (or v:TP→V) on P defines a principal G-connection ω if and only if it is G-equivariant in the sense that H p g = d ( R g ) p ( H p ) {displaystyle H_{pg}=mathrm {d} (R_{g})_{p}(H_{p})} . A trivializing section of a principal bundle P is given by a section s of P over an open subset U of M. Then the pullback s*ω of a principal connection is a 1-form on U with values in g {displaystyle {mathfrak {g}}} .If the section s is replaced by a new section sg, defined by (sg)(x) = s(x)g(x), where g:M→G is a smooth map, then (sg)*ω = Ad(g)−1 s*ω+g−1dg. The principal connection is uniquely determined by this family of g {displaystyle {mathfrak {g}}} -valued 1-forms, and these 1-forms are also called connection forms or connection 1-forms, particularly in older or more physics-oriented literature.

[ "Cotangent bundle", "Tangent bundle", "Principal bundle", "Normal bundle", "Fiber bundle", "Frame bundle", "Geometry", "Structural engineering", "Mechanical engineering", "Pullback (differential geometry)", "Dual bundle", "Bundle gerbe", "Algebra bundle", "Pushforward (differential)", "Jet (mathematics)", "Connection form", "Connection (mathematics)", "Stiefel–Whitney class" ]
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