Induced connection on an associated bundle via horizontals

Construction of an Ehresmann connection on an associated bundle from a principal connection on P.
Induced connection on an associated bundle via horizontals

Let π:PM\pi:P\to M be a with ω\omega, and let E=P×GFE=P\times_G F be the for a left GG-space FF. Write q:P×FEq:P\times F\to E for the quotient map and denote by πE:EM\pi_E:E\to M the bundle projection.

Construction (horizontal distribution on E). For [p,u]E[p,u]\in E, define the horizontal subspace

H[p,u]E:=dq(p,u)(Hp×{0})T[p,u]E, H^E_{[p,u]} := dq_{(p,u)}(H_p \times \{0\}) \subset T_{[p,u]}E,

where Hp=ker(ωp)TpPH_p=\ker(\omega_p)\subset T_pP is the horizontal subspace of PP and 0TuF0\in T_uF is the zero vector. This is well-defined (independent of the representative (p,u)(p,u)) because HH is GG-equivariant and the quotient identifies (pg,g1u)(pg,g^{-1}u) with (p,u)(p,u).

Then TETE splits as

T[p,u]E=H[p,u]Eker(dπE)[p,u], T_{[p,u]}E = H^E_{[p,u]} \oplus \ker(d\pi_E)_{[p,u]},

giving an Ehresmann connection on EE.

In the vector bundle case (fiber a vector space), this induced connection coincides with the usual notion of .

Examples

  1. For E=P×GGE=P\times_G G with left multiplication, the induced connection recovers the original principal connection under the identification EPE\cong P.
  2. For E=Ad(P)E=\mathrm{Ad}(P), the construction produces a natural connection on the adjoint bundle used in gauge theory to differentiate gauge parameters.
  3. If PP is trivial over UU and AA is the local gauge potential, the induced horizontals on U×FU\times F are determined by AA acting through the infinitesimal action of g\mathfrak g on FF.