Alphabeta Math
PropositionStatement: Literature-sourcedProof: AI-adaptedprecheck passaudited 2026-09-01
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Exterior-power duality pairing

Statement

The canonical pairing

ω,v1vk:=ω(v1,,vk)

extends to a nondegenerate bilinear pairing

kV×kVR,

and for decomposable elements one has

α1αk, v1vk=det(αi(vj)).

Facts & Assumptions

Given: Covectors α1,,αk and vectors v1,,vk in a finite-dimensional real vector space V.

[F1]

A decomposable k-vector is the functional ωω(v1,,vk) on alternating k-covectors (The finite-dimensional exterior power of vectors).

[F2]

The wedge product is the signed shuffle sum on alternating covectors (The wedge product of alternating covectors).

[L1]

Wedges of a basis and of its dual basis give dual coordinate systems on exterior powers (Wedge monomials in a dual basis form a basis).

Proof

technique · direct
1.1

By [F2], (α1αk)(v1,,vk) is the alternating sum over permutations of iαi(vσ(i)), which is exactly the determinant of the matrix (αi(vj)). By [F1], this is the value of the pairing on the displayed decomposable elements.

F1F2givenalgebra
2.1

Choose a basis e1,,en of V with dual basis e1,,en. By [L1], the wedges eI form a basis of kV and the wedges eI form a basis of kV, and step 1.1 shows eI,eJ=δIJ. Therefore the pairing matrix in these bases is the identity, so the pairing is nondegenerate.

L1step 1.1choosealgebra
3.1

Thus the canonical exterior-power pairing is bilinear, has the determinant formula on decomposables, and is nondegenerate.

step 1.1step 2.1

Depends on

Used by

Dependency tree · two levels

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Sources