Titchmarsh theorem

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Not to be confused with the Titchmarsh convolution theorem.

In the mathematical field of Fourier analysis, the Titchmarsh theorem, named after Edward Charles Titchmarsh, gives necessary and sufficient conditions for a complex-valued square-integrable function F(x) on the real line to be the boundary value of a function in the Hardy space H2(U) of holomorphic functions in the upper half-plane U. The theorem is named for Edward Charles Titchmarsh, who proved the theorem in Titchmarsh (1948, Theorem 95).

The theorem states that the following conditions for a complex-valued square-integrable function F : RC are equivalent:

  • F(x) is the limit as z → x of a holomorphic function F(z) in the upper half-plane such that
  • −Im(F) is the Hilbert transform of Re(F), where Re(F) and Im(F) are real-valued functions with F = Re(F) + i Im(F).
  • The Fourier transform vanishes for x < 0.

A weaker result is true for functions of class Lp for p > 1 (Titchmarsh 1948, Theorem 103). Specifically, if F(z) is a holomorphic function such that

for all y, then there is a complex-valued function F(x) in Lp(R) such that F(x + iy) → F(x) in the Lp norm as y → 0 (as well as holding pointwise almost everywhere). Furthermore,

where ƒ is a real-valued function in Lp(R) and g is the Hilbert transform (of class Lp) of ƒ.

This is not true in the case p = 1. In fact, the Hilbert transform of an L1 function ƒ need not converge in the mean to another L1 function. Nevertheless (Titchmarsh 1948, Theorem 105), the Hilbert transform of ƒ does converge almost everywhere to a finite function g such that

This result is directly analogous to one by Andrey Kolmogorov for Hardy functions in the disc.

See also

References

  • Duren, P. (1970), Theory of  -Spaces, New York: Academic Press.
  • Titchmarsh, E (1948), Introduction to the theory of Fourier integrals (2nd ed.) (published 1986), ISBN 978-0828403245 {{citation}}: ISBN / Date incompatibility (help).
  • Weisstein, Eric W. "Titchmarsh theorem". MathWorld.