In the case of diffraction of photons by an edge it can be shown simply by means of classical relativistic mechanics that the assumption of quantized angular momentum leads to a diffraction pattern which looks very similar to what is observd in experiments.

Are there any hints that in the very early days of QM Sommerfeld or Bohr or somebody else  ever considered the idea that the observed "interference" patterns in diffraction experiments with electrons and photons might result from the quantization of angular momentum and from an interchange of quantized portions of ang.mom. during the interaction of an electron or photon with the atoms of an edge, slid, double-slid, etc.?

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