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Linear Functional 📂Linear Algebra

Linear Functional

Definitions1

Let’s call VV a vector space. A mapping ff from VV to C\mathbb{C} (or R\mathbb{R}) is called a functional.

f:VC f : V \to \mathbb{C}

If ff is linear, it is called a linear functional.

More Detailed Definitions2

Let’s call VV a vector space over the field FF. Here, the field FF itself becomes a 11-dimensional vector space over FF. A linear transformation f:VFf : V \to F is called a linear functional.

In other words, a linear functional is a linear transformation between a vector space and its field.

Explanation

The first definition given is the most common. Usually, it is not defined as abstractly as the second.

When translating functional into Korean, it becomes ‘범함수’ without much nuance, but it is important to note in English that functional is not an adjective but a noun. Also, the translation of functional as 범함수 (汎函數) is influenced by generalized function.

The distinction from linear operators is only that the codomain is defined as R\mathbb{R} or C\mathbb{C}, but this very difference makes it worthwhile to consider spaces such as dual spaces. Norm =V\| \cdot \| = \| \cdot \|_{V} already becomes a functional in itself, and considering its usefulness in connection with measure theory is inevitable.

Examples

Trace

Let’s assume V=Mn×n(R)V = M_{n\times n}(\mathbb{R}). Define the function ff as follows.

f:Mn×n(R)R by f(A)=tr(A) f : M_{n\times n}(\mathbb{R}) \to \mathbb{R} \quad \text{ by } \quad f(A) = \tr(A)

Then tr\tr is the trace of a matrix. Thus, ff is a linear functional.

Fourier Coefficients

Let’s assume VV is a vector space of continuous functions that satisfy f:[0,2π]Rf : [0, 2\pi] \to \mathbb{R}. For a fixed gVg \in V, define h:VRh : V \to \mathbb{R} as follows.

h(f)=12π02πf(x)g(x)dx h(f) = \dfrac{1}{2\pi} \int_{0}^{2\pi} f(x)g(x)dx

Then hh is a linear functional. When gg is either cosnx\cos nx or sinnx\sin nx, h(f)h(f) becomes the Fourier coefficient of ff.

Coordinate Function

Let’s consider VV as a finite-dimensional vector space. Assume β={v1,,vn}\beta = \left\{ \mathbf{v}_{1}, \dots, \mathbf{v}_{n} \right\} is the ordered basis of VV. Let the coordinate vector of xV\mathbf{x} \in V be as follows.

[x]β=[a1a2an] [\mathbf{x}]_{\beta} = \begin{bmatrix} a_{1} \\ a_{2} \\ \vdots \\ a_{n} \end{bmatrix}

Now, consider the following function for 1in1 \le i \le n.

fi(x)=ai f_{i}(\mathbf{x}) = a_{i}

Then fif_{i} is a linear functional defined on VV, called the iith coordinate function. Then, fi(vi)=δijf_{i}(\mathbf{v}_{i}) = \delta_{ij} holds true. δij\delta_{ij} is the Kronecker delta. Coordinate functions play an important role in discussing dual spaces.


  1. Kreyszig. (1989). Introductory Functional Analysis with Applications: p103~104. ↩︎

  2. Stephen H. Friedberg, Linear Algebra (4th Edition, 2002), p119 ↩︎