Radial function

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In mathematics, a radial function is a real-valued function defined on a Euclidean space Template:Tmath whose value at each point depends only on the distance between that point and the origin. The distance is usually the Euclidean distance. For example, a radial function Template:Math in two dimensions has the form[1] Φ(x,y)=φ(r),r=x2+y2 where Template:Mvar is a function of a single non-negative real variable. Radial functions are contrasted with spherical functions, and any descent function (e.g., continuous and rapidly decreasing) on Euclidean space can be decomposed into a series consisting of radial and spherical parts: the solid spherical harmonic expansion.

A function is radial if and only if it is invariant under all rotations leaving the origin fixed. That is, Template:Mvar is radial if and only if fρ=f for all Template:Math, the special orthogonal group in Template:Mvar dimensions. This characterization of radial functions makes it possible also to define radial distributions. These are distributions Template:Mvar on Template:Tmath such that S[φ]=S[φρ] for every test function Template:Mvar and rotation Template:Mvar.

Given any (locally integrable) function Template:Mvar, its radial part is given by averaging over spheres centered at the origin. To wit, ϕ(x)=1ωn1Sn1f(rx)dx where Template:Math is the surface area of the (n−1)-sphere Template:Math, and Template:Math, Template:Math. It follows essentially by Fubini's theorem that a locally integrable function has a well-defined radial part at almost every Template:Mvar.

The Fourier transform of a radial function is also radial, and so radial functions play a vital role in Fourier analysis. Furthermore, the Fourier transform of a radial function typically has stronger decay behavior at infinity than non-radial functions: for radial functions bounded in a neighborhood of the origin, the Fourier transform decays faster than Template:Math. The Bessel functions are a special class of radial function that arise naturally in Fourier analysis as the radial eigenfunctions of the Laplacian; as such they appear naturally as the radial portion of the Fourier transform.

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