Let MM be a . The wedge product is the canonical bilinear product on the graded algebra of .

For α∈Ωk(M)\alpha \in \Omega^k(M) and β∈Ωℓ(M)\beta \in \Omega^\ell(M), their wedge product α∧β∈Ωk+ℓ(M)\alpha\wedge\beta \in \Omega^{k+\ell}(M) is defined pointwise by the alternating product of multilinear forms on each :

(α∧β)p(v1,…,vk+ℓ)=1k! ℓ!∑σ∈Sk+ℓsgn⁡(σ) αp ⁣(vσ(1),…,vσ(k)) βp ⁣(vσ(k+1),…,vσ(k+ℓ)),(\alpha\wedge\beta)_p(v_1,\dots,v_{k+\ell}) =\frac{1}{k!\,\ell!}\sum_{\sigma\in S_{k+\ell}}\operatorname{sgn}(\sigma)\, \alpha_p\!\bigl(v_{\sigma(1)},\dots,v_{\sigma(k)}\bigr)\, \beta_p\!\bigl(v_{\sigma(k+1)},\dots,v_{\sigma(k+\ell)}\bigr),

where Sk+ℓS_{k+\ell} is the set of of k+ℓk+\ell symbols, sgn⁡\operatorname{sgn} is the , and k!k! and ℓ!\ell! are . The formula holds for all p∈Mp\in M and v1,…,vk+ℓ∈TpMv_1,\dots,v_{k+\ell}\in T_pM.

Equivalent characterizations

If alternation is normalized by

Alt⁡(T)(v1,…,vr)=1r!∑σ∈Srsgn⁡(σ)T(vσ(1),…,vσ(r)),\operatorname{Alt}(T)(v_1,\ldots,v_r) =\frac1{r!}\sum_{\sigma\in S_r}\operatorname{sgn}(\sigma) T(v_{\sigma(1)},\ldots,v_{\sigma(r)}),

then the same convention gives

(α∧β)p=(k+ℓ)!k!ℓ!Alt⁡(αp⊗βp).(\alpha\wedge\beta)_p =\frac{(k+\ell)!}{k!\ell!}\operatorname{Alt}(\alpha_p\otimes\beta_p).

Here the tensor product evaluates by multiplying the value of αp\alpha_p on the first kk arguments by that of βp\beta_p on the last ℓ\ell.

Examples
  1. Coordinate 1-forms on R3\mathbb{R}^3. With standard coordinates (x,y,z)(x,y,z), the 2-form dx∧dydx\wedge dy satisfies (dx∧dy)(∂x,∂y)=1(dx\wedge dy)(\partial_x,\partial_y)=1 and changes sign when the vectors are swapped: (dx∧dy)(∂y,∂x)=−1(dx\wedge dy)(\partial_y,\partial_x)=-1.
  1. A wedge computation with functions. Let α=f dx+g dy\alpha = f\,dx + g\,dy and β=h dz\beta = h\,dz on R3\mathbb{R}^3, where f,g,hf,g,h are smooth functions. Then
    α∧β=fh dx∧dz+gh dy∧dz.\alpha\wedge\beta = fh\,dx\wedge dz + gh\,dy\wedge dz.
  1. Wedge of a 1-form with itself is zero (odd degree). On any manifold, dx∧dx=0dx\wedge dx=0. More generally, if η\eta is any 1-form then η∧η=0\eta\wedge\eta=0 by graded-commutativity with k=ℓ=1k=\ell=1.
Properties

If α∈Ωk(M)\alpha\in\Omega^k(M), β∈Ωℓ(M)\beta\in\Omega^\ell(M), and γ∈Ωm(M)\gamma\in\Omega^m(M), then:

  • Bilinearity: ∧\wedge is R\mathbb{R}-bilinear in each argument.
  • Associativity: (α∧β)∧γ=α∧(β∧γ)(\alpha\wedge\beta)\wedge\gamma=\alpha\wedge(\beta\wedge\gamma).
  • Graded-commutativity:
    α∧β=(−1)kℓ β∧α.\alpha\wedge\beta = (-1)^{k\ell}\,\beta\wedge\alpha.
    In particular, if kk is odd then α∧α=0\alpha\wedge\alpha=0.
  • Compatibility with pullback: for any F:M→NF:M\to N, the satisfies F∗(α∧β)=F∗α∧F∗βF^*(\alpha\wedge\beta)=F^*\alpha\wedge F^*\beta.
  • The wedge product is the product appearing in the graded Leibniz rule for the .