Abstract

The angular spectra of the diffraction fields of small and weak phase objects calculated by scalar Kirchhoff and Rayleigh-Sommerfield diffraction theories with adapted Kirchhoff boundary conditions are compared with the angular spectrum evaluated by Wolf [Optics Comm. 1 (1969) 153] derived in close analogy to the first Born approximation. Contour plots show the deviations from the theories depending on phase object thickness and spatial frequency. The phase objects should have a finite thickness d of approximately λ to minimize the deviations caused by the first Rayleigh-Sommerfeld diffraction theory, a result in contradiction to calculations of Evans [Optics Comm. 2 (1970) 317]. On the other hand a vanishing thickness is required in the second Rayleigh-Sommerfeld diffraction theory. The results agree with experiments carried out with electromagnetic cm-waves.

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