Mathematics · Glossary

What is Dual space, dual basis?

Also known as: dual space · dual basis

Definition 2.1 University Mathematics — Year 2 · Chapter 2 — Linear Algebra

The dual of EE is E=L(E,K)E^* = \mathcal{L}(E, K), the space of linear forms. If B=(e1,,en)\mathcal{B} = (e_1, \dots, e_n) is a basis of EE, the coordinate forms e1,,ene_1^*, \dots, e_n^* defined by ei(ej)=δije_i^*(e_j) = \delta_{ij} (Kronecker: 11 if i=ji = j, else 00) form the dual basis B\mathcal{B}^* of EE^*; in particular dimE=dimE\dim E^* = \dim E, and

x=i=1nei(x)ei(xE),φ=i=1nφ(ei)ei(φE).x = \sum_{i=1}^{n} e_i^*(x)\, e_i \quad (x \in E), \qquad \varphi = \sum_{i=1}^{n} \varphi(e_i)\, e_i^* \quad (\varphi \in E^*).

Examples

Example 2.2

On Kn[X]K_n[X] with basis (1,X,,Xn)(1, X, \dots, X^n): the dual basis is PP(k)(0)k!P \mapsto \frac{P^{(k)}(0)}{k!} (Taylor coefficients). Another basis of the dual: the evaluations PP(xi)P \mapsto P(x_i) at n+1n + 1 distinct points — its “pre-dual” basis in Kn[X]K_n[X] is exactly the family of Lagrange polynomials LiL_i (Year 1 volume), since Li(xj)=δijL_i(x_j) = \delta_{ij}. Interpolation is duality.

Example 2.4 (A dual basis of R2\R^2, fully computed)

For the basis b1=(1,1)b_1 = (1, 1), b2=(1,1)b_2 = (1, -1) of R2\R^2: the dual basis (b1,b2)(b_1^*, b_2^*) must satisfy bi(bj)=δijb_i^*(b_j) = \delta_{ij}. Writing b1(x,y)=αx+βyb_1^*(x, y) = \alpha x + \beta y, the conditions α+β=1\alpha + \beta = 1 and αβ=0\alpha - \beta = 0 give

b1(x,y)=x+y2,and likewiseb2(x,y)=xy2.b_1^*(x, y) = \frac{x + y}{2}, \qquad\text{and likewise}\qquad b_2^*(x, y) = \frac{x - y}{2} .

Sanity checks: b1b_1^* is not e1+e2e_1^* + e_2^* evaluated naively — the dual basis depends on the whole basis, not on each vector separately (replacing b2b_2 by (0,1)(0, 1) changes b1b_1^* into xxx \mapsto x). And the expansion formula works: (x,y)=x+y2b1+xy2b2(x, y) = \frac{x+y}2\,b_1 + \frac{x-y}2\,b_2, the even/odd decomposition of a pair — dual bases are coordinate extractors, and this one extracts symmetric and antisymmetric parts.

Example 2.9 (The transpose, entry by entry)

Let u ⁣:R2R3u \colon \R^2 \to \R^3 have matrix A=(120130)A = \left(\begin{smallmatrix} 1 & 2\\ 0 & 1\\ 3 & 0\end{smallmatrix}\right) in the canonical bases. For ψ=b1f1+b2f2+b3f3(R3)\psi = b_1f_1^* + b_2f_2^* + b_3f_3^* \in (\R^3)^*, compute uT(ψ)=ψuu^{\mathsf T}(\psi) = \psi \circ u on the basis of R2\R^2:

(ψu)(e1)=ψ(1,0,3)=b1+3b3,(ψu)(e2)=ψ(2,1,0)=2b1+b2.(\psi \circ u)(e_1) = \psi(1, 0, 3) = b_1 + 3b_3, \qquad (\psi \circ u)(e_2) = \psi(2, 1, 0) = 2b_1 + b_2 .

So uT(ψ)=(b1+3b3)e1+(2b1+b2)e2u^{\mathsf T}(\psi) = (b_1 + 3b_3)\,e_1^* + (2b_1 + b_2)\,e_2^*, and in the dual bases the matrix of uTu^{\mathsf T} is

(103210)=AT:\begin{pmatrix} 1 & 0 & 3\\ 2 & 1 & 0\end{pmatrix} = A^{\mathsf T} :

the abstract transpose is the flipped matrix, with no computation left to believe on faith. Note the mechanism: the jj-th column of AA became the jj-th row of the new matrix because ψu\psi \circ u reads uu’s outputs through ψ\psi’s coefficients.

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