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Graded bracket of Lie-algebra-valued differential forms

Definition

Let M be a smooth manifold and g a finite-dimensional real Lie algebra. For homogeneous α∈Ωp(M,g) and β∈Ωq(M,g), define their graded bracket by

[α∧β](X1,…,Xp+q):=1p!q!∑σ∈Sp+qsgn⁡(σ)[α(Xσ(1),…,Xσ(p)),β(Xσ(p+1),…,Xσ(p+q))].

Here Ωp(M,g) is the space of smooth alternating p-linear forms with values in g, the inner bracket is the Lie-algebra bracket, and the sum is over all permutations. This is a smooth g-valued (p+q)-form. It obeys graded skew-symmetry [α∧β]=−(−1)pq[β∧α], graded Jacobi

[α∧[β∧γ]]=[[α∧β]∧γ]+(−1)pq[β∧[α∧γ]],

and the exterior-derivative rule

d[α∧β]=[dα∧β]+(−1)p[α∧dβ].

In particular, for g-valued 1-forms A,B, [A∧B](X,Y)=[A(X),B(Y)]−[A(Y),B(X)], so 12[A∧A](X,Y)=[A(X),A(Y)]. This fixes the normalization used by the Cartan curvature formula.

Facts & Assumptions

Given: A smooth manifold M, a finite-dimensional real Lie algebra g, and homogeneous forms α,β,γ of degrees p,q,r.

[F1]

A finite-dimensional real Lie algebra has a bilinear alternating bracket satisfying Jacobi. Finite-dimensional Lie algebra

[F2]

A smooth g-valued form has smooth scalar components in any finite basis, and its exterior derivative is taken componentwise. Finite-dimensional vector-valued forms and their exterior derivative

[F3]

The scalar exterior derivative is a graded derivation of the wedge product. The exterior derivative is a graded derivation

[F4]

Differential forms form an associative graded-commutative algebra. The wedge product of differential forms, Differential forms form a graded commutative algebra

Proof

1.1F1F2F4construct

Choose a finite basis (ea)a=1n of g with dual basis (ea)a=1n, and write α=∑aeaαa, β=∑bebβb, where αa=ea∘α and βb=eb∘β are smooth scalar forms. Expanding the alternating permutation sum gives [α∧β]=∑a,b[ea,eb] αa∧βb; this finite sum is smooth and alternating, hence is in Ωp+q(M,g).

2.1F1F4step 1.1algebra

Swapping the two blocks of p and q arguments in the defining permutation sum contributes the sign (−1)pq; antisymmetry of the inner Lie bracket contributes the minus sign. Therefore [α∧β]=−(−1)pq[β∧α].

2.2F2F3step 1.1

In the finite basis expansion of step 1.1, apply the scalar graded derivation rule [F3] to each αa∧βb and retain the fixed coefficient [ea,eb]. Summing the resulting finite terms gives d[α∧β]=[dα∧β]+(−1)p[α∧dβ].

2.3F1F4step 1.1

For homogeneous α,β,γ, the same basis expansion writes [α∧[β∧γ]] with coefficient [ea,[eb,ec]] and form factor αa∧βb∧γc. The right-hand terms have coefficients [ [ea,eb],ec] and, after commuting βb past αa using [F4], [eb,[ea,ec]], with the same form factor. The equality of coefficients is exactly the Lie-algebra Jacobi identity in [F1], so the graded Jacobi formula follows.

3.1F1F2F3F4step 1.1step 2.1step 2.2step 2.3∎

If g=0, all forms and brackets are zero; if p=0 or q=0, the same formulas use the empty wedge with sign +1. The finite basis in step 1.1 is one finite-dimensional coordinate calculation, not a choice from a family. The definition and identities hold on the empty manifold as well.

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