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When dealing with differentiable manifolds, we define a "differential k-form" to be a function that assigns to every point x of the manifold an element of the k-th exterior power of the cotangent space at x. (Or, what is the same thing: a function that assigns to every point x an anti-symmetric map from (TxM)k to the base field, where TxM is the tangent space at x).
Such a form is said to be differentiable if, when applied to k differentiable vector fields, the result is a differentiable function. The wedge product makes pointwise sense for differential forms. In the de Rham and Alexander-Spanier cohomology theories it is used to define a multiplication on the associated cohomology ring, in an analogous way to the cup product in singular cohomology.
Given a commutative ring R and an R- module M, we can define the exterior algebra Λ(M) just as above, as a suitable quotient of the tensor algebra T(M). It will satisfy the analogous universal property.
Grassmann algebras have some important applications in physics where they are used to model various concepts related to fermions and supersymmetry.
See also: superspace, superalgebra, supergroup