In mathematics, orthogonal functions belong to a function space that is a vector space equipped with a bilinear form. When the function space has an interval as the domain, the bilinear form may be the integral of the product of functions over the interval:
\langlef,g\rangle=\int\overline{f(x)}g(x)dx.
The functions
f
g
\langlef,g\rangle=0
f ≠ g
Suppose
\{f0,f1,\ldots\}
\left\{fn/\left\|fn\right\|2\right\}
See main article: article, Fourier series and Harmonic analysis. Several sets of orthogonal functions have become standard bases for approximating functions. For example, the sine functions and are orthogonal on the interval
x\in(-\pi,\pi)
m ≠ n
2\sin\left(mx\right)\sin\left(nx\right)=\cos\left(\left(m-n\right)x\right)-\cos\left(\left(m+n\right)x\right),
See main article: article and Orthogonal polynomials. If one begins with the monomial sequence
\left\{1,x,x2,...\right\}
[-1,1]
The study of orthogonal polynomials involves weight functions
w(x)
\langlef,g\rangle=\intw(x)f(x)g(x)dx.
(0,infty)
w(x)=e-x
Both physicists and probability theorists use Hermite polynomials on
(-infty,infty)
w(x)=
-x2 | |
e |
w(x)=
-x2/2 | |
e |
Chebyshev polynomials are defined on
[-1,1]
Zernike polynomials are defined on the unit disk and have orthogonality of both radial and angular parts.
Walsh functions and Haar wavelets are examples of orthogonal functions with discrete ranges.
Legendre and Chebyshev polynomials provide orthogonal families for the interval while occasionally orthogonal families are required on . In this case it is convenient to apply the Cayley transform first, to bring the argument into . This procedure results in families of rational orthogonal functions called Legendre rational functions and Chebyshev rational functions.
Solutions of linear differential equations with boundary conditions can often be written as a weighted sum of orthogonal solution functions (a.k.a. eigenfunctions), leading to generalized Fourier series.