Statement

Let f∈L2(Rd)f\in L^2(\mathbb R^d) and σ>0\sigma>0. With the Fourier convention f^(ξ)=∫f(x)e−2πix⋅ξ dx\widehat f(\xi)=\int f(x)e^{-2\pi i x\cdot\xi}\,dx, the condition

supp⁡f^⊆Bσ/(2π)\operatorname{supp}\widehat f\subseteq B_{\sigma/(2\pi)}

holds if and only if ff is the restriction to Rd\mathbb R^d of an F:Cd→CF:\mathbb C^d\to\mathbb C for which

∣F(x+iy)∣≤Aeσ∣y∣|F(x+iy)|\le A e^{\sigma|y|}

for some A>0A>0 and all x,y∈Rdx,y\in\mathbb R^d.

Forward direction

Fourier inversion over the bounded support defines F(z)=∫f^(ξ)e2πiz⋅ξ dξF(z)=\int\widehat f(\xi)e^{2\pi i z\cdot\xi}\,d\xi. The bounded frequency region makes the integral entire and gives the exponential bound by .

Reverse direction

Shift the contour in a complex line parallel to a fixed frequency ξ\xi. When 2π∣ξ∣>σ2\pi|\xi|>\sigma, exponential decay in the shifted half-plane forces f^(ξ)=0\widehat f(\xi)=0. A standard approximation removes auxiliary Schwartz regularity used in the contour argument.

Normalization warning

If the Fourier exponential is e−ix⋅ξe^{-ix\cdot\xi}, the ball radius is σ\sigma rather than σ/(2π)\sigma/(2\pi).

References
  1. Lars Hörmander, The Analysis of Linear Partial Differential Operators I, Springer, 2003. DOI record. Relevant: Theorem 7.3.1.
  2. Alex Cohen, “Fractal uncertainty in higher dimensions,” 2024. arXiv record. Relevant: Theorem 2.1 and Appendix A.3.