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Exterior powers represent alternating multilinear maps and are unique up to unique isomorphism
Statement
Let be a vector space over a field and . The basic wedge map , , is -linear and alternating. For every -vector space and every alternating -linear map of Alternating -linear maps, there is a unique linear map with
Moreover, if is a vector space and is a -linear alternating map with the same property, then there is a unique linear isomorphism with .
Facts & Assumptions
Given: A field , a vector space , an integer , a vector space , and an alternating -linear map .
An alternating -linear map vanishes whenever two arguments are equal (Alternating -linear maps).
The exterior power is , and the wedge is the universal multilinear map composed with the quotient projection (The th exterior power as the tensor-power quotient by repeated-vector relations).
The iterated tensor product represents -linear maps: every -linear map out of factors uniquely through the pure-tensor map (Finite iterated tensor products represent multilinear maps independently of parenthesization).
A linear map out of factors uniquely through when it kills (Universal property of the quotient vector space).
Two pairs representing the same class of maps are related by a unique isomorphism carrying structure maps to structure maps (Tensor products are unique up to a unique isomorphism carrying elementary tensors to elementary tensors).
Proof
The wedge is multilinear and alternating: by [L2] it is the composition of the universal multilinear map of [L3] with the quotient projection, and the projection kills every pure tensor with a repeated pair, which is exactly the vanishing condition of [L1].
Since is -linear, [L3] supplies a unique linear map with .
The map kills : each generator is a pure tensor with a repeated pair, on which agrees with the alternating map , which vanishes by [L1]; hence vanishes on the whole span .
By [L4], factors uniquely through the quotient of [L2], giving a unique linear with the displayed value on every wedge.
For the uniqueness up to unique isomorphism, apply the universal property of to and that of to , obtaining and with and . Then and , so the uniqueness clause of step 3.1 forces and ; this is the two-application argument of [L5].
Steps 1.1 and 3.1 prove the representing property, and step 4.1 the uniqueness of the representing pair.
Depends on
Alternating -linear maps
The th exterior power as the tensor-power quotient by repeated-vector relations
Tensor products are unique up to a unique isomorphism carrying elementary tensors to elementary tensors
Finite iterated tensor products represent multilinear maps independently of parenthesization
Universal property of the quotient vector space