Valeriy V. Dvoeglazov
The Feynman-Dyson Propagators for Neutral Particles (Locality or Non-locality?)
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ABSTRACT. An analog of the S = 1/2 Feynman-Dyson propagator is presented
in the framework of the S = 1 Weinberg s theory. The basis for this
construction is the concept of the Weinberg field as a system of four field functions differing by parity and by dual transformations. Next, we analyze the recent controversy in the definitions of the Feynman-Dyson propagator for the field operator containing the S = 1/2 self/anti-self charge conjugate states in the papers by D. Ahluwalia et al. [11] and by W. Rodrigues Jr. et al [18, 19]. The solution of this mathematical controversy is obvious. It is related to the necessary doubling of the Fock Space (as in the Barut and Ziino works), thus extending the corresponding Clifford Algebra. However, the logical interrelations of different mathematical foundations with the physical
interpretations are not so obvious. We present some insights with
respect to.