Abstract

We continue the discussion of several explicit examples of generalizations in relativistic quantum mechanics. We discussed the generalized spin-1/2 equations for neutrinos and the spin-1 equations for photon. The equations obtained by means of the Gersten-Sakurai method and those of Weinberg for spin-1 particles have been mentioned. Thus, we generalized the Maxwell and Weyl equations. Particularly, we found connections of the well-known solutions and the dark 4-spinors in the Ahluwalia-Grumiller elko model. They are also not the eigenstates of the chirality and helicity. The equations may lead to the dynamics which are different from those accepted at the present time. For instance, the photon may have non-transverse components and the neutrino may be not in the energy states and in the chirality states. The second-order equations have been considered too. They have been obtained by the Ryder method.

Highlights

  • The Gersten Method and its Relation to Relativistic Quantum Equations.The content of this talk is the following

  • With the identification a/2m → α2 and m(1 − b2)/2a → κ the above set leads to the second-order equation of the Barut type

  • We presented two very natural ways of deriving the massive/massless equations in the (S, 0) ⊕ (0, S) representation space, which lead to the equations given by other researchers in the past

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Summary

Introduction

The Gersten Method and its Relation to Relativistic Quantum Equations.The content of this talk is the following. We discuss the massive/massless 2nd order equations. It has been known for a long time that “one cannot set the mass equal to zero in a manifestly covariant massive-particle equation, in order to obtain the corresponding massless case”, e. Apply the generalized Ryder relation [29] (see below, Eq (61)) and the standard scheme for the derivation of relativistic wave equations [30, footnote # 1], [16].

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