# Linear form

In linear algebra, a **linear functional** or **linear form** (also called a **one-form** or **covector**) is a linear map from a vector space to its field of scalars. In **ℝ**^{n}, if vectors are represented as column vectors, then linear functionals are represented as row vectors, and their action on vectors is given by the matrix product with the row vector on the left and the column vector on the right. In general, if *V* is a vector space over a field *k*, then a linear functional *f* is a function from *V* to *k* that is linear:

- for all
- for all

The set of all linear functionals from *V* to *k*, denoted by Hom_{k}(*V*,*k*), forms a vector space over *k* with the operations of addition and scalar multiplication defined pointwise. This space is called the dual space of *V*, or sometimes the **algebraic dual space**, to distinguish it from the continuous dual space. It is often written *V*^{∗}, *V′*, or *V*^{ᐯ} when the field *k* is understood.

## Continuous linear functionals

If *V* is a topological vector space, the space of continuous linear functionals — the *continuous dual* — is often simply called the dual space. If *V* is a Banach space, then so is its (continuous) dual. To distinguish the ordinary dual space from the continuous dual space, the former is sometimes called the *algebraic dual space*. In finite dimensions, every linear functional is continuous, so the continuous dual is the same as the algebraic dual, but in infinite dimensions the continuous dual is a proper subspace of the algebraic dual.

## Examples and applications

### Linear functionals in R^{n}

^{n}

Suppose that vectors in the real coordinate space **R**^{n} are represented as column vectors

For each row vector [*a*_{1} … *a*_{n}] there is a linear functional *f* defined by

and each linear functional can be expressed in this form.

This can be interpreted as either the matrix product or the dot product of the row vector [*a*_{1} ... *a*_{n}] and the column vector :

### Integration

Linear functionals first appeared in functional analysis, the study of vector spaces of functions. A typical example of a linear functional is integration: the linear transformation defined by the Riemann integral

is a linear functional from the vector space C[*a*, *b*] of continuous functions on the interval [*a*, *b*] to the real numbers. The linearity of *I* follows from the standard facts about the integral:

### Evaluation

Let *P _{n}* denote the vector space of real-valued polynomial functions of degree ≤

*n*defined on an interval [

*a*,

*b*]. If

*c*∈ [

*a*,

*b*], then let ev

_{c}:

*P*→

_{n}**R**be the

**evaluation functional**

The mapping *f* → *f*(*c*) is linear since

If *x*_{0}, ..., *x _{n}* are

*n*+ 1 distinct points in [

*a*,

*b*], then the evaluation functionals ev

*,*

_{xi}*i*= 0, 1, ...,

*n*form a basis of the dual space of

*P*. (Lax (1996) proves this last fact using Lagrange interpolation.)

_{n}### Application to quadrature

The integration functional *I* defined above defines a linear functional on the subspace *P _{n}* of polynomials of degree ≤

*n*. If

*x*

_{0}, ...,

*x*

_{n}are

*n*+ 1 distinct points in [

*a*,

*b*], then there are coefficients

*a*

_{0}, ...,

*a*

_{n}for which

for all *f* ∈ *P*_{n}. This forms the foundation of the theory of numerical quadrature.

This follows from the fact that the linear functionals ev* _{xi}* :

*f*→

*f*(

*x*

_{i}) defined above form a basis of the dual space of

*P*

_{n}.[1]

### Linear functionals in quantum mechanics

Linear functionals are particularly important in quantum mechanics. Quantum mechanical systems are represented by Hilbert spaces, which are anti–isomorphic to their own dual spaces. A state of a quantum mechanical system can be identified with a linear functional. For more information see bra–ket notation.

### Distributions

In the theory of generalized functions, certain kinds of generalized functions called distributions can be realized as linear functionals on spaces of test functions.

## Properties

- Any linear functional
*L*is either trivial (equal to 0 everywhere) or surjective onto the scalar field. Indeed, this follows since just as the image of a vector subspace under a linear transformation is a subspace, so is the image of*V*under*L*. However, the only subspaces (that is,*k*-subspaces) of*k*are {0} and*k*itself. - A linear functional is continuous if and only if its kernel is closed. [2]
- Linear functionals with the same kernel are proportional.
- The absolute value of any linear functional is a seminorm on its vector space.

## Visualizing linear functionals

In finite dimensions, a linear functional can be visualized in terms of its level sets. In three dimensions, the level sets of a linear functional are a family of mutually parallel planes; in higher dimensions, they are parallel hyperplanes. This method of visualizing linear functionals is sometimes introduced in general relativity texts, such as *Gravitation* by Misner, Thorne & Wheeler (1973).

## Dual vectors and bilinear forms

Every non-degenerate bilinear form on a finite-dimensional vector space *V* induces an isomorphism *V* → *V*^{∗} : *v* ↦ *v*^{∗} such that

where the bilinear form on *V* is denoted ⟨ , ⟩ (for instance, in Euclidean space ⟨*v*, *w*⟩ = *v* ⋅ *w* is the dot product of *v* and *w*).

The inverse isomorphism is *V*^{∗} → *V* : *v*^{∗} ↦ *v*, where *v* is the unique element of *V* such that

The above defined vector *v*^{∗} ∈ *V*^{∗} is said to be the **dual vector** of *v* ∈ *V*.

In an infinite dimensional Hilbert space, analogous results hold by the Riesz representation theorem. There is a mapping *V* → *V*^{∗} into the *continuous dual space* *V*^{∗}. However, this mapping is antilinear rather than linear.

## Bases in finite dimensions

### Basis of the dual space in finite dimensions

Let the vector space *V* have a basis , not necessarily orthogonal. Then the dual space *V** has a basis called the dual basis defined by the special property that

Or, more succinctly,

where δ is the Kronecker delta. Here the superscripts of the basis functionals are not exponents but are instead contravariant indices.

A linear functional belonging to the dual space can be expressed as a linear combination of basis functionals, with coefficients ("components") *u _{i}*,

Then, applying the functional to a basis vector *e _{j}* yields

due to linearity of scalar multiples of functionals and pointwise linearity of sums of functionals. Then

So each component of a linear functional can be extracted by applying the functional to the corresponding basis vector.

### The dual basis and inner product

When the space *V* carries an inner product, then it is possible to write explicitly a formula for the dual basis of a given basis. Let *V* have (not necessarily orthogonal) basis . In three dimensions (*n* = 3), the dual basis can be written explicitly

for *i* = 1, 2, 3, where *ε* is the Levi-Civita symbol and the inner product (or dot product) on *V*.

In higher dimensions, this generalizes as follows

where is the Hodge star operator.

## Notes

- Lax 1996
- Rudin 1991, Theorem 1.18
- J.A. Wheeler; C. Misner; K.S. Thorne (1973).
*Gravitation*. W.H. Freeman & Co. p. 57. ISBN 0-7167-0344-0.

## References

- Bishop, Richard; Goldberg, Samuel (1980), "Chapter 4",
*Tensor Analysis on Manifolds*, Dover Publications, ISBN 0-486-64039-6 - Halmos, Paul (1974),
*Finite dimensional vector spaces*, Springer, ISBN 0-387-90093-4 - Lax, Peter (1996),
*Linear algebra*, Wiley-Interscience, ISBN 978-0-471-11111-5 - Misner, Charles W.; Thorne, Kip. S.; Wheeler, John A. (1973),
*Gravitation*, W. H. Freeman, ISBN 0-7167-0344-0 - Rudin, Walter (1991),
*Functional Analysis*, McGraw-Hill Science/Engineering/Math, ISBN 978-0-07-054236-5 - Schutz, Bernard (1985), "Chapter 3",
*A first course in general relativity*, Cambridge, UK: Cambridge University Press, ISBN 0-521-27703-5