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
Accelerating Research
Robert Robinson Avenue,
Oxford Science Park, Oxford
OX4 4GP, United Kingdom
Address
John Eccles HouseRobert Robinson Avenue,
Oxford Science Park, Oxford
OX4 4GP, United Kingdom