| viXra.org > High Energy Particle Physics > 2011 |
 |
 |
| viXra.org > High Energy Particle Physics > 2011 |
|
|
[5] viXra:2011.0205 [pdf] submitted on 2020-11-30 08:58:27
Authors: Dominic Espree
Comments: 14 Pages.
Quantum gravity is the most profound outstanding question in fundamental physics. How do we describe spacetime itself quantum mechanically? In this article we present a novel approach called “geometrodynamics,” which uses the interconnections between space, time, and mechanical entropy. In particular we will show how quantum scattering processes indicate that Lorentz symmetry must be broken, in a way manifested physically through transformation of energy into mass that can no longer be accelerated. Throughout we apply our theoretical ideas to specific physical situations.
Category: High Energy Particle Physics
[4] viXra:2011.0186 [pdf] submitted on 2020-11-26 10:58:06
Authors: Valeriy V. Dvoeglazov
Comments: 7 Pages. [Corrections made by viXra Admin to conform with the rules of viXra.org]
The second-order equation in the $(1/2,0)\oplus (0,1/2)$ representation of the Lorentz group
has been proposed by A. Barut in the 70s, ref.~\cite{barut}. It permits to explain
the mass splitting
of leptons $(e,\mu,\tau)$. The interest is growing in this model (see, for instance, the papers by
S. Kruglov~\cite{kroug} and J. P. Vigier {\it et al.}~\cite{vig,dvo}). We noted some additional points of this model.
Category: High Energy Particle Physics
[3] viXra:2011.0185 [pdf] submitted on 2020-11-25 16:05:13
Authors: Valeriy V. Dvoeglazov
Comments: 7 Pages. Some parts have also be presented at the XIII DGFM SMF Workshop, Nov. 4-8, 2019. Leon, Gto., M\'exico.
Both algebraic equation $Det (\hat p - m) =0$ and $Det (\hat p + m) =0$ for $u-$ and $v-$ 4-spinors have solutions with $p_0= \pm E_p =\pm \sqrt{{\bf p}^2 +m^2}$. The same is true for higher-spin equations (or they may even have more complicated dispersion relations). Meanwhile, every book considers
the equality $p_0=E_p$ for both $u-$ and $v-$ spinors of the $(1/2,0)\oplus (0,1/2))$ representation only, thus applying the Dirac-Feynman-Stueckelberg procedure for elimination of negative-energy solutions. The recent Ziino works (and, independently,
the articles of several other authors) show that the Fock space can be doubled. We re-consider this possibility on the quantum-field level for both
$s=1/2$ and higher spin particles.
Some parts have also be presented at the XIII DGFM SMF Workshop, Nov. 4-8, 2019. Leon, Gto., M\'exico.
Category: High Energy Particle Physics
[2] viXra:2011.0066 [pdf] submitted on 2020-11-09 20:03:18
Authors: Eugene V. Stefanovich
Comments: 9 Pages. Published in the General Science Journal on September 23, 2019
Modern theories of strong interactions suggest that baryon-antibaryon forces can be strongly attractive, and manifestations of ``baryonium'' states have been seen in experiments. In light of these new data, we attempt to revisit the Fermi-Yang-Sakata idea that mesons and baryons are bound states of few fundamental ``sakatons'' identified with $p, n, \Lambda$, and $\Lambda_c$ particles. We optimized parameters of inter-sakaton potentials and calculated meson and baryon mass spectra in fair agreement with experiment. Moreover, the same set of potentials
allows us to reproduce approximately elastic scattering cross sections of baryons and binding energies of light nuclei and hypernuclei. This suggests that the Sakata model could be a promising organizing principle in particle and nuclear physics. This principle may also coexist with the modern quark model, where both valence and sea quark contributions to the hadron structure are allowed.
Category: High Energy Particle Physics
[1] viXra:2011.0032 [pdf] submitted on 2020-11-04 08:19:45
Authors: Michael Tzoumpas
Comments: 8 Pages.
There is no a nucleus with more than two neighboring protons, because the presence of a third proton creates an increased negative potential that exceeds their stability potential, causing a cleaving (beta decay β+) of this third proton. These two protons are next to each other and due to their opposite magnetic moments they create a column of magnetic field, while a magnetic column is created by the rotated neutrons as well. So, the first phase of the nuclei structure ends in He-4. Of course, protons are immobile, while neutrons are rotating around them. However, how is the second nucleus He-4 added? Apparently having a common axis with the first He-4. But why is beryllium Be-8, with the two superimposed nuclei He-4, unstable? We will prove that column construction is based on the stability of carbon C-12 and oxygen O-16, which
consist of three superimposed nuclei He-4 and four He-4 respectively. Consequently, the
structure of the nuclei begins with the so-called lower-order nuclei, as the deuterium, tritium and helium He-3, which evolve into helium He-4 and then first upper-order oxygen nucleus, that has four helium nuclei He-4 in a column of strong negative electric field.
Category: High Energy Particle Physics
| Third-Party Links: |
|