Orthonormal basis

Orthonormal basis
In mathematics, particularly linear algebra, an orthonormal basis for an inner product space V with finite dimension is a basis for whose vectors are orthonormal, that is, they are all unit vectors and orthogonal to each other. For example, the standard basis for a Euclidean space is an orthonormal basis, where the relevant inner product is the dot product of vectors. The image of the standard basis under a rotation or reflection (or any orthogonal transformation) is also orthonormal, and every orthonormal basis for arises in this fashion.
For a general inner product space an orthonormal basis can be used to define normalized orthogonal coordinates on Under these coordinates, the inner product becomes a dot product of vectors. Thus the presence of an orthonormal basis reduces the study of a finite-dimensional inner product space to the study of under dot product. Every finite-dimensional inner product space has an orthonormal basis, which may be obtained from an arbitrary basis using the Gram–Schmidt process.
In functional analysis, the concept of an orthonormal basis can be generalized to arbitrary (infinite-dimensional) inner product spaces. Given a pre-Hilbert space an orthonormal basis for is an orthonormal set of vectors with the property that every vector in can be written as an infinite linear combination of the vectors in the basis. In this case, the orthonormal basis is sometimes called a Hilbert basis for Note that an orthonormal basis in this sense is not generally a Hamel basis, since infinite linear combinations are required. Specifically, the linear span of the basis must be dense in but it may not be the entire space.
If we go on to Hilbert spaces, a non-orthonormal set of vectors having the same linear span as an orthonormal basis may not be a basis at all. For instance, any square-integrable function on the interval can be expressed (almost everywhere) as an infinite sum of Legendre polynomials (an orthonormal basis), but not necessarily as an infinite sum of the monomials
A different generalisation is to pseudo-inner product spaces, finite-dimensional vector spaces equipped with a non-degenerate symmetric bilinear form known as the metric tensor. In such a basis, the metric takes the form with positive ones and negative ones.
Examples
For , the set of vectors is called the standard basis and forms an orthonormal basis of with respect to the standard dot product. Note that both the standard basis and standard dot product rely on viewing as the Cartesian product
Proof: A straightforward computation shows that the inner products of these vectors equals zero, and that each of their magnitudes equals one, This means that is an orthonormal set. All vectors can be expressed as a sum of the basis vectors scaled so spans and hence must be a basis. It may also be shown that the standard basis rotated about an axis through the origin or reflected in a plane through the origin also forms an orthonormal basis of .
For , the standard basis and inner product are similarly defined. Any other orthonormal basis is related to the standard basis by an orthogonal transformation in the group O(n).
For pseudo-Euclidean space , an orthogonal basis with metric instead satisfies if , if , and if . Any two orthonormal bases are related by a pseudo-orthogonal transformation. In the case , these are Lorentz transformations.
The set with where denotes the exponential function, forms an orthonormal basis of the space of functions with finite Lebesgue integrals, with respect to the 2-norm. This is fundamental to the study of Fourier series.
The set with if and otherwise forms an orthonormal basis of
Eigenfunctions of a Sturm–Liouville eigenproblem.
The column vectors of an orthogonal matrix form an orthonormal set.
Basic formula
If is an orthogonal basis of then every element may be written as
When is orthonormal, this simplifies to
and the square of the norm of can be given by
Even if is uncountable, only countably many terms in this sum will be non-zero, and the expression is therefore well-defined. This sum is also called the Fourier expansion of and the formula is usually known as Parseval's identity.
If is an orthonormal basis of then is isomorphic to in the following sense: there exists a bijective linear map such that
Incomplete orthogonal sets
Given a Hilbert space and a set of mutually orthogonal vectors in we can take the smallest closed linear subspace of containing Then will be an orthogonal basis of which may of course be smaller than itself, being an incomplete orthogonal set, or be when it is a complete orthogonal set.
Existence
Using Zorn's lemma and the Gram–Schmidt process (or more simply well-ordering and transfinite recursion), one can show that every Hilbert space admits an orthonormal basis; furthermore, any two orthonormal bases of the same space have the same cardinality (this can be proven in a manner akin to that of the proof of the usual dimension theorem for vector spaces, with separate cases depending on whether the larger basis candidate is countable or not). A Hilbert space is separable if and only if it admits a countable orthonormal basis. (One can prove this last statement without using the axiom of choice.)
Choice of basis as a choice of isomorphism
For concreteness we discuss orthonormal bases for a real, dimensional vector space with a positive definite symmetric bilinear form .
One way to view an orthonormal basis with respect to is as a set of vectors , which allow us to write for , and or . With respect to this basis, the components of are particularly simple:
We can now view the basis as a map which is an isomorphism of inner product spaces: to make this more explicit we can write
Explicitly we can write where is the dual basis element to .
The inverse is a component map
These definitions make it manifest that there is a bijection
The space of isomorphisms admits actions of orthogonal groups at either the side or the side. For concreteness we fix the isomorphisms to point in the direction , and consider the space of such maps, .
This space admits a left action by the group of isometries of , that is, such that , with the action given by composition:
This space also admits a right action by the group of isometries of , that is with the action again given by composition: .
As a principal homogeneous space
The set of orthonormal bases for with the standard inner product is a principal homogeneous space or G-torsor for the orthogonal group and is called the Stiefel manifold of orthonormal -frames.
In other words, the space of orthonormal bases is like the orthogonal group, but without a choice of base point: given the space of orthonormal bases, there is no natural choice of orthonormal basis, but once one is given one, there is a one-to-one correspondence between bases and the orthogonal group.
Concretely, a linear map is determined by where it sends a given basis: just as an invertible map can take any basis to any other basis, an orthogonal map can take any orthogonal basis to any other orthogonal basis.
The other Stiefel manifolds for of incomplete orthonormal bases (orthonormal -frames) are still homogeneous spaces for the orthogonal group, but not principal homogeneous spaces: any -frame can be taken to any other -frame by an orthogonal map, but this map is not uniquely determined.
The set of orthonormal bases for is a G-torsor for .
The set of orthonormal bases for is a G-torsor for .
The set of orthonormal bases for is a G-torsor for .
The set of right-handed orthonormal bases for is a G-torsor for
See also
References
(page 218, ch.9)
External links
This Stack Exchange Post discusses why the set of Dirac Delta functions is not a basis of L2([0,1]).
Fourier analysis
Functional analysis
Linear algebra