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The Fourier-slice identity for the Euclidean Radon transform

Statement

For every f∈Cc∞(R2;C), every unit normal θ∈S1, and every σ∈R, the compact-support Fourier transform of the line data in the offset variable equals the restriction of the two-dimensional Fourier transform to the line in frequency space with direction θ: Rf^(θ,σ)=f^(σθ).

Facts & Assumptions

Given: f∈Cc∞(R2;C), θ∈S1, and σ∈R.

[F1]

The Euclidean Radon transform on R²: Rf(θ,s)=∫Rf(sθ+tθ⊥) dt, and the compact-support Fourier transform uses the phase e−2πix⋅ξ.

[F2]

A continuous real function on a compact Jordan measurable set is Riemann integrable over that set: a continuous real function on a compact Jordan set is Riemann integrable; apply this to real and imaginary parts on a bounding rectangle.

[F3]

Riemann--Fubini on product rectangles, with lower and upper section integrals and content-zero exceptional sections: for a Riemann-integrable function on a product of closed rectangles, the iterated Riemann integrals equal the product-rectangle integral when the sections are integrable.

[F4]

A compactly supported Riemann integrand admits the global change-of-variables formula from a diffeomorphism near the relevant compact preimage: an injective C1 change of variables with nonvanishing Jacobian carries a compactly supported Riemann integral to the integral multiplied by the absolute Jacobian.

[F5]

The second fundamental theorem: if G is differentiable on [a,b] with G′=f and f is integrable, then ∫abf=G(b)−G(a): if a real function G is differentiable on [a,b], including one-sided endpoint derivatives, and G′ is Riemann integrable there, then ∫abG′=G(b)−G(a).

[F6]

The chain rule for total derivatives: D(g∘f)(a)=Dg(f(a))∘Df(a): for totally differentiable maps between finite-dimensional real spaces, D(g∘T)=Dg(T)∘DT. Apply this separately to real and imaginary parts; when T is linear, DT=T is constant, so repeated application gives the corresponding directional derivatives of a smooth composition.

Proof

1.1givenF1choose

Fix θ and define T(s,t)=sθ+tθ⊥ and F(s,t)=f(T(s,t)). The columns of T are an orthonormal positively oriented basis, so T is a linear diffeomorphism and K:=T−1(supp⁡f) is compact. Choose M>0 with K⊂[−M,M]2. Then F(s,t)=0 for ∣t∣>M, and Rf(θ,s)=∫−MMF(s,t) dt; it vanishes unless s belongs to the compact projection of K onto the first coordinate.

2.1F1F2F5F6step 1.1

Write f=fR+ifI and Fν=fν∘T for ν∈{R,I}. Each fν is real smooth; since DT is constant, repeated applications of [F6] give ∂skFν(s,t)=(θ⋅∇)kfν(T(s,t)). Thus, for each integer k≥0, ∂skF is continuous. On every compact s-interval, ∂sk+1F is uniformly continuous on the product with [−M,M]. For each real component, apply [F5] on [0,1] to u↦∂skFν(s+uh,t). By [F6] its derivative is h ∂sk+1Fν(s+uh,t), continuous and hence integrable by [F2], with the same one-sided derivatives at the endpoints. Combining the two real equalities and dividing by h gives, for sufficiently small nonzero h of either sign, ∂skF(s+h,t)−∂skF(s,t)h=∫01∂sk+1F(s+uh,t) du. The right side converges uniformly for t∈[−M,M] to ∂sk+1F(s,t) as h→0. Integrating in t therefore proves inductively that dkdskRf(θ,s)=∫−MM∂skF(s,t) dt for every k, and uniform continuity also makes each derivative continuous in s. Thus Rf(θ,⋅)∈Cc∞(R;C), so its Fourier transform in [F1] is defined.

2.2F2step 1.1choose

Put H(s,t)=f(T(s,t))e−2πiσs. This is continuous and supported in K. Choose a nondegenerate product rectangle containing K. By [F2], the real and imaginary parts of H are Riemann integrable there, and all their one-variable sections are continuous and hence Riemann integrable.

3.1F1F3step 2.1step 2.2

By [F1], Rf^(θ,σ) is the iterated integral of H, first in t and then in s. Apply the real-valued Riemann-Fubini theorem [F3] separately to Re⁡H and Im⁡H on the chosen rectangle, then combine the two equalities. Since H vanishes outside that rectangle, this gives Rf^(θ,σ)=∫R2f(sθ+tθ⊥)e−2πiσs ds dt.

4.1F1F4step 3.1∎

Apply [F4] to T separately for the real and imaginary parts of the compactly supported Riemann integrand in step 3.1. Since s=x⋅θ and ∣det⁡DT∣=1, the integral becomes ∫R2f(x)e−2πiσx⋅θ dx=f^(σθ) by [F1]. This is the claimed identity.

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