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Rigorous Theory of Interaction Between Nuclear Particles
Author(s) -
E. C. G. Stueckelberg
Publication year - 1938
Publication title -
physical review
Language(s) - English
Resource type - Journals
eISSN - 1536-6065
pISSN - 0031-899X
DOI - 10.1103/physrev.54.889
Subject(s) - hamiltonian (control theory) , physics , quantum , classical mechanics , theoretical physics , elementary particle , quantum field theory , quantum mechanics , mathematics , mathematical optimization
In this chapter a double tensor index k implies summation from 1 to 4. There is no classical way to treat the spin and charge variables of elementary particles. ' Therefore we represent matter by a set of complex wave fields p„. The quantities J, and S„& occurring in (1.1) are formed from matrices j„and s„A, . if I =0. Eq. (1.3) takes the form of Dirac's equation for a particle with inherent magnetic moment p (proton ?).' A term —2xSii, .s~q p is added to (1.3). The last part of (1.3) now takes the form

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