Exercise 11.2 (The Dual Basis)

Exercise 11.2. Prove Proposition 11.1.

Proposition 11.1. Let V be a finite-dimensional vector space. Given any basis (E1,,En) for V , let 𝜀1,,𝜀n V be the covectors defined by

𝜀i (E j) = δji

where δji is the Kronecker delta symbol defined by (4.4). Then (𝜀1,,𝜀n) is a basis for V , called the dual basis to (Ej). Therefore, dim V = dim V .

Answers

Proof. To prove that ( 𝜀 1 , , 𝜀 n ) is a base for V , we verify that it is linearly independent and that it spans V .

Linear independence. Suppose for the sake of contradiction that ( 𝜀 1 , , 𝜀 n ) are linearly dependent, i.e., we can find scalars a 1 , , a n , not all zero, such that

a 1 𝜀 1 + + a n 𝜀 n = 0

Note that the 0 on the right denotes the function that sends every element of V to 0 . The above equality above is an equality of maps, which should hold on any v we evaluate either side on. In particular, it should hold for all E j for j = 1 , , n , i.e.,

1 j n : 0 = a 1 𝜀 1 ( E j ) + a n 𝜀 n ( E j ) = a j

In other words, a j = 0 for all j = 1 , , n - a contradiction.

Span. Now we show that ( 𝜀 1 , , 𝜀 n ) spans V . Let ω V . For each j = 1 , , n , let w j denote the scalar ω ( w j ) . We claim that

ω = w 1 𝜀 1 + w n 𝜀 n .

By Exercise B.13, to verify that two functions, LHS and RHS, are equal, it suffices to demonstrate that they agree on the basis elements. Indeed, for each 1 j n ,

w 1 𝜀 1 ( E j ) + w n 𝜀 n ( E j ) = w j = ω ( E j ) .

by the definition of the w j and the 𝜀 j . Thus, ω and w 1 𝜀 1 + w n 𝜀 n agree on the basis, so we conclude that they are equal as elements of V . Hence ( 𝜀 1 , , 𝜀 n ) spans V . □

User profile picture
2023-05-29 09:41
Comments