Abstract
I HAVE attempted to introduce in a certain way a constant a of dimension length in order to formulate a divergence-free theory of interaction. The functions of field,* are treated not as Fourier series: (we have taken as an example the scalar meson field) but as matrices: = kl¥, where The unsymmetrical part in the first (or second) brackets could as well be used as kl; we have taken both (with the factor 1/š2) on account of symmetry.
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RAYSKI, G. An Attempt to Formulate a Divergence-Free Quantum Mechanics of Fields. Nature 157, 873 (1946). https://doi.org/10.1038/157873a0
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DOI: https://doi.org/10.1038/157873a0
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