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Exercise 11.2 (The Dual Basis)
Exercise 11.2. Prove Proposition 11.1.
Proposition 11.1. Let be a finite-dimensional vector space. Given any basis for , let be the covectors defined by
where is the Kronecker delta symbol defined by (4.4). Then is a basis for , called the dual basis to . Therefore, .
Answers
Proof. To prove that is a base for , we verify that it is linearly independent and that it spans .
Linear independence. Suppose for the sake of contradiction that are linearly dependent, i.e., we can find scalars , not all zero, such that
Note that the on the right denotes the function that sends every element of to . The above equality above is an equality of maps, which should hold on any we evaluate either side on. In particular, it should hold for all for , i.e.,
In other words, for all - a contradiction.
Span. Now we show that spans . Let . For each , let denote the scalar . We claim that
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 ,
by the definition of the and the . Thus, and agree on the basis, so we conclude that they are equal as elements of . Hence spans . □