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Radon Transform

  The Radon transform of a function f(x,y) is defined as the integral along a straight line defined by its distance from the origin and its angle of inclination , a definition very close to that of the Hough transform

where the delta function defines integration only over the line. The range of is limited to . Like in the Hough transform, the Radon operator maps the spatial domain (x,y) to the projection domain ( ), in which each point corresponds to a straight line in the spatial domain. Conversely, each point in the spatial domain becomes a sine curve in the projection domain, hence the use of the name sinogram.

In tomography, a back-projection operator and the inverse of the Radon transform are used to reconstruct images in three dimensions from intensities recorded in one or two dimensions (see [Barrett81], [Phelps86], [Jain89]).



Rudolf K. Bock, 7 April 1998