Let GG be a with a on a nonempty space FF. A GG-bundle with fiber FF is a π:E→B\pi:E\to B equipped with local trivializations Φi\Phi_i over an open cover {Ui}\{U_i\} and continuous maps gij:Ui∩Uj→Gg_{ij}:U_i\cap U_j\to G such that

ΦiΦj−1(b,f)=(b,gij(b)⋅f),gii=e,gijgjk=gik\Phi_i\Phi_j^{-1}(b,f)=(b,g_{ij}(b)\cdot f), \qquad g_{ii}=e,\qquad g_{ij}g_{jk}=g_{ik}

on the respective overlaps. The last identity is required on every triple overlap. Here GG is the . The chosen data are considered up to refinement of the cover and changes of trivializations by continuous maps hi:Ui→Gh_i:U_i\to G; replacing Φi\Phi_i by hiΦih_i\Phi_i replaces gijg_{ij} by higijhj−1h_i g_{ij}h_j^{-1}.

Smooth version and examples

For a , a Lie group acting smoothly on FF, and smooth maps gijg_{ij} and hih_i, this defines a smooth GG-bundle. A rank-nn has structure group GL(n,K)\mathrm{GL}(n,\mathbb K) acting on Kn\mathbb K^n.

Principal bundles and conventions

Taking F=GF=G with left multiplication gives a : right multiplication on each local copy of GG commutes with the transition maps and therefore defines a global right action. Its smooth version is a . For general FF, a GG-bundle need not carry a global GG-action on its total space.

Terminology. In gauge theory and algebraic geometry, “GG-bundle” often abbreviates “principal GG-bundle.” This knowl uses the broader structure-group meaning; principal-bundle statements link to their explicit definition.

If the action on FF is not faithful, the maps gijg_{ij} and their cocycle identities are extra data: the underlying changes of fiber coordinates do not determine them uniquely.

References
  1. Fiber Bundles lecture notes, §1.2, pp. 6–7: fiber bundles, G-atlases, equivalent atlases, and the non-effective-action convention.