Difference of two principal connections is tensorial

The difference of two principal connection 1-forms is a tensorial one-form with values in the Lie algebra.
Difference of two principal connections is tensorial

Let π:PM\pi:P\to M be a with Lie group GG and Lie algebra g\mathfrak g (see ). Let ω,ωΩ1(P;g)\omega,\omega'\in \Omega^1(P;\mathfrak g) be connection 11-forms of two (see ).

Define their difference

a:=ωωΩ1(P;g). a := \omega' - \omega \in \Omega^1(P;\mathfrak g).

Lemma

The 11-form aa is tensorial of type Ad\mathrm{Ad}, meaning:

  1. (Horizontal) ap(v)=0a_p(v)=0 for every vertical vector vVpPv\in V_pP (equivalently ιX#a=0\iota_{X^\#}a=0 for all fundamental vertical fields X#X^\#).
  2. (Ad\mathrm{Ad}-equivariant) (Rg)a=Ad(g1)a(R_g)^*a = \mathrm{Ad}(g^{-1})\,a for all gGg\in G (see ).

Consequently, aa descends to a well-defined 11-form on the base with values in the adjoint bundle:

a  a~Ω1 ⁣(M;ad(P)), a \ \longleftrightarrow\ \widetilde a \in \Omega^1\!\big(M;\mathrm{ad}(P)\big),

where ad(P)=P×Adg\mathrm{ad}(P)=P\times_{\mathrm{Ad}}\mathfrak g is the (compare and ).

This tensoriality fact underlies many standard constructions, including transgression formulas (see ) and the description of the affine space of connections (compare ).

Examples

  1. Trivial bundle: local gauge potentials differ by a basic form.
    On the trivial principal bundle P=M×GP=M\times G (see ), a principal connection corresponds to a g\mathfrak g-valued 11-form AΩ1(M;g)A\in\Omega^1(M;\mathfrak g) via a global section. If ω,ω\omega,\omega' correspond to A,AA,A', then

    a=ωωcorresponds toAAΩ1(M;g), a=\omega'-\omega \quad \text{corresponds to} \quad A'-A\in\Omega^1(M;\mathfrak g),

    which is a genuine 11-form on MM (hence automatically horizontal/basic after pullback to PP).

  2. U(1) bundles: two connections differ by an ordinary real 1-form.
    For G=U(1)G=U(1), the adjoint action is trivial, so ad(P)M×iR\mathrm{ad}(P)\cong M\times i\mathbb R. Thus the difference of two U(1)U(1)-connections is simply an iRi\mathbb R-valued 11-form on MM. Concretely, if AA and AA' are local connection 11-forms (see ), then AAA'-A patches globally as an iRi\mathbb R-valued form.

  3. Frame bundle: change of linear connection is tensorial.
    Let EME\to M be a rank-nn vector bundle and let P=Fr(E)P=\mathrm{Fr}(E) be its frame bundle (see ). Two vector bundle connections on EE correspond to two principal connections on PP (compare ). Their difference is a tensorial 11-form on PP, which corresponds to a 11-form on MM with values in End(E)\mathrm{End}(E), i.e. the usual “difference tensor” between linear connections.