Bochner's theorem

In mathematics, Bochner's theorem characterizes the Fourier transform of a positive finite Borel measure on the real line.

Background

Given a positive finite Borel measure μ on the real line R, the Fourier transform Q of μ is the continuous function

$Q(t)=\int _{\mathbb {R} }e^{-itx}d\mu (x).$

Q is continuous since for a fixed x, the function e^-itx is continuous and periodic. The function Q is a positive definite function, i.e. the kernel K(x, y) = Q(y - x) is positive definite; this can be checked via a direct calculation.

The theorem

Bochner's theorem says the converse is true, i.e. every positive definite function Q is the Fourier transform of a positive finite Borel measure. A proof can be sketched as follows.

Let F₀(R) be the family of complex valued functions on R with finite support, i.e. f(x) = 0 for all but finitely many x. The positive definite kernel K(x, y) induces a sesquilinear form on F₀(R). This in turn results in a Hilbert space

$({\mathcal {H}},\langle \;,\;\rangle )$

whose typical element is an equivalence class [g]. For a fixed t in R, the "shift operator" U_t defined by (U_tg)(x) = g(x - t), for a representative of [g] is unitary. In fact the map

$t\;{\stackrel {\Phi }{\mapsto }}\;U_{t}$

is a strongly continuous representation of the additive group R. By the Stone-von Neumann theorem, there exists a (possibly unbounded) self-adjoint operator A such that

$U_{-t}=e^{-iAt}.\;$

This implies there exists a finite positive Borel measure μ on R where

$\langle U_{-t}[e_{0}],[e_{0}]\rangle =\int e^{-iAt}d\mu (x),$

where e₀ is the element in F₀(R) defned by e₀(m) = 1 if m = 0 and 0 otherwise. Because

$\langle U_{-t}[e_{0}],[e_{0}]\rangle =K(-t,0)=Q(t),$

the theorem holds.

See also

• Positive definite function

Reference

• M. Reed and B. Simon, Methods of Modern Mathematical Physics, vol. II, Academic Press, 1975.