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Exterior-power duality pairing
Statement
The canonical pairing
extends to a nondegenerate bilinear pairing
and for decomposable elements one has
Facts & Assumptions
Given: Covectors and vectors in a finite-dimensional real vector space .
A decomposable -vector is the functional on alternating -covectors (The finite-dimensional exterior power of vectors).
The wedge product is the signed shuffle sum on alternating covectors (The wedge product of alternating covectors).
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
By [F2], is the alternating sum over permutations of , which is exactly the determinant of the matrix . By [F1], this is the value of the pairing on the displayed decomposable elements.
Choose a basis of with dual basis . By [L1], the wedges form a basis of and the wedges form a basis of , and step 1.1 shows . Therefore the pairing matrix in these bases is the identity, so the pairing is nondegenerate.
Thus the canonical exterior-power pairing is bilinear, has the determinant formula on decomposables, and is nondegenerate.
Depends on
Used by
Dependency tree · two levels
19 results within two dependency steps of this one, each drawn at its shortest distance from it. An arrow runs from a result to what uses it, so the chart reads left to right and ends at this result, which carries a heavier outline. Every node is a link to that result. Click elsewhere on the chart to enlarge it.
Sources
- Will J. Merry, Differential Geometry (standard reference, not scraped)