Definition

For an integrable function f:RdCf:\mathbb R^d\to\mathbb C, its X-ray transform is

Xf(x,θ)=Rf(x+tθ)dt,θSd1.Xf(x,\theta)=\int_{\mathbb R}f(x+t\theta)\,dt, \qquad \theta\in S^{d-1}.

It depends only on the oriented affine line represented by (x,θ)(x,\theta): Xf(x+aθ,θ)=Xf(x,θ)Xf(x+a\theta,\theta)=Xf(x,\theta).

Redundant parameterization

One often restricts xθx\in\theta^\perp to choose a unique base point. Replacing θ\theta by θ-\theta leaves the unoriented line integral unchanged.

Relation to the Radon transform

The X-ray transform integrates over one-dimensional affine subspaces. The classical Radon transform in Rd\mathbb R^d integrates over ; they coincide only in dimension two after identifying lines with hyperplanes.

Role in plurisubharmonic extension

For the linewise extension used in higher-dimensional Beurling–Malliavin theory, transverse components of the Levi form are X-ray transforms of the real Hessian of the boundary weight.

References
  1. Sigurdur Helgason, The Radon Transform, 2nd ed., Birkhäuser, 1999. DOI record.