2015
DOI: 10.1007/s10773-015-2852-3
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An Unbroken Axial-Vector Current Conservation Law

Abstract: The mass, energy and momentum of the neutrino of a true flavor have an axial-vector nature. As a consequence, the left-handed truly neutral neutrino in an axial-vector field of emission can be converted into a right-handed one and vice versa. This predicts the unidenticality of masses, energies and momenta of neutrinos of the different components. Recognizing such a difference in masses, energies, momenta and accepting that the left-handed axial-vector neutrino and the right-handed antineutrino of true neutral… Show more

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Cited by 4 publications
(27 citation statements)
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“…From this point of view, each of earlier experiments [4,5] about mixing angles may serve as the source of facts confirming the existence in all truly neutral particles of a kind of C-odd electric charge [6,7] responsible for the flavor symmetrical mode of neutrino oscillations. The Coulomb transitions of these types can explain the absence of vector currents of truly neutral neutrinos and the availability of an axial-vector nature of their mass [8,9].…”
Section: Introductionmentioning
confidence: 96%
“…From this point of view, each of earlier experiments [4,5] about mixing angles may serve as the source of facts confirming the existence in all truly neutral particles of a kind of C-odd electric charge [6,7] responsible for the flavor symmetrical mode of neutrino oscillations. The Coulomb transitions of these types can explain the absence of vector currents of truly neutral neutrinos and the availability of an axial-vector nature of their mass [8,9].…”
Section: Introductionmentioning
confidence: 96%
“…These interconversions together with the unity of flavor and gauge symmetry laws [2] express the unidenticality of masses, energies and momenta of truly neutral neutrinos of the different components. However, such a possibility, as was noted in [3] for the fist time, is realized only at the spontaneous mirror symmetry violation of axial-vector types of fermions. In other words, the left-handed neutrino of true neutrality and the right-handed axial-vector antineutrino are of long-lived leptons of C-oddity, and the right-handed truly neutral neutrino and the left-handed axial-vector antineutrino refer to short-lived C-odd fermions.…”
Section: Introductionmentioning
confidence: 93%
“…The mass, energy and momentum of the neutrino of a C-even charge are strictly vector (V ) type [4]. In contrast to this, the neutrino of a C-odd electric charge [5] has the mass, energy and momentum of an axial-vector (A) nature [3]. Therefore, the matrices (1) and ( 2) refer doubtless only to those elementary particles in which the vector C-even properties are absent.…”
Section: Introductionmentioning
confidence: 99%
“…where V must be accepted as an index of a distinction. We recognize that between the currents of C-even and C-odd charges there exists a range of paradoxical contradictions [2], which require their classification with respect to C-operation. It reflects the availability of the two types of particles and fields of vector V l and axial-vector A l currents of the different C-parity [3].…”
Section: Introductionmentioning
confidence: 98%
“…In contrast to this, a C-even neutrino has the mass, energy, and momentum of a vector (V ) nature [1]. In other words, the matrices (1) and (2) refer to those neutrinos (ν V l = ν V e , ν V µ , ν V τ , ...) and leptons (l V = e V , µ V , τ V , ...) in which axial-vector C-odd properties are absent. From their point of view, well known [5] Dirac equation itself for vector types of particles with the spin 1/2 and the four-component wave function ψ s (t s , x s ) accepts a latent united form…”
Section: Introductionmentioning
confidence: 99%