Maurer–Cartan equation

The structure equation satisfied by the Maurer–Cartan form on a Lie group.
Maurer–Cartan equation

Let GG be a with Lie algebra g\mathfrak g.

Statement

Let θ\theta denote the on GG, i.e. the g\mathfrak g-valued 1-form characterized by

  • θe=idg\theta_e=\mathrm{id}_{\mathfrak g} under the identification TeGgT_eG\cong \mathfrak g, and
  • left-invariance: (Lg)θ=θ(L_g)^*\theta=\theta for all gGg\in G.

Then θ\theta satisfies the Maurer–Cartan equation

dθ+12[θ,θ]=0. d\theta + \frac12[\theta,\theta]=0.

Here [θ,θ][\theta,\theta] denotes the g\mathfrak g-valued 2-form obtained by combining wedge product with the : for vector fields X,YX,Y on GG,

[θ,θ](X,Y)=[θ(X),θ(Y)]. [\theta,\theta](X,Y) = [\theta(X),\theta(Y)].

Equivalent form (often used in calculations)

For any vector fields X,YX,Y on GG,

(dθ)(X,Y)=[θ(X),θ(Y)]. (d\theta)(X,Y) = -[\theta(X),\theta(Y)].

A clean proof is packaged in .

Context

This equation is the differential-geometric encoding of the Lie algebra structure inside the group: it is the reason that brackets of are controlled by the structure constants of g\mathfrak g, and it underlies many constructions with and .