Rigorous Theory of Interaction Between Nuclear Particles
نویسنده
چکیده
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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