High Energy Particle Physics

1102 Submissions

[5] viXra:1102.0057 [pdf] submitted on 28 Feb 2011

NTEP: Chapter 8. Nonlinear Quantum Electron Equation

Authors: Alexander G. Kyriakos
Comments: 11 pages.

The derivation of nonlinear quantum electron equation in the framework of nonlinear theory of elementary particles (NTEP) is presented. It can help to understand many aspects of the quantum description of elementary particles. In particular, it is shown that the fields self-action is “the mechanism”, which introduces the mass into the quantum electron equation. This mechanism has a similarities with the Higgs mechanism of mass generation, however it is not needed a Higgs boson. The results of the experiments, which were set until now, to find the Higgs's boson, are negative. At the same time the NTEP has not difficulties, which will appear in Standard Model theory, if Higgs's boson is not discovered.
Category: High Energy Particle Physics

[4] viXra:1102.0041 [pdf] submitted on 23 Feb 2011

NTEP: Chapter 7. Classical Nonlinear Electron Theories and Their Connection with Qed

Authors: Alexander G. Kyriakos
Comments: 18 pages.

In this chapter of nonlinear theory of elementary particles (NTEP) a review of the nonlinear field theories in the framework of classical electrodynamics is presented. It is shown that the results found within these theories can be transferred to quantum theory. These results can also help us to understand many aspects of the quantum description of elementary particles. In particular, they explain why electron can be interpreted as a point and non-point particle simultaneously.
Category: High Energy Particle Physics

[3] viXra:1102.0034 [pdf] submitted on 20 Feb 2011

No Elementary Scalars in Experimental Supersymmetry

Authors: Alejandro Rivero
Comments: 2 Pages.

This sheet presents an extreme interpretation of the global SU(5) symmetry that has been gradually discovered in the spectrum of scalar particles of the Supersymmetric Standard Model. It postulates that such scalars are actually the different aspects of the QCD string. If so, only the gauginos and perhaps two neutral higgs particles are candidates for discovery in the LHC.
Category: High Energy Particle Physics

[2] viXra:1102.0021 [pdf] replaced on 2011-12-21 14:11:28

A Mathematical Model of the Quark and Lepton Mixing Angles (2011 Update)

Authors: J. S. Markovitch
Comments: 18 Pages.

A single mathematical model encompassing both quark and lepton mixing is described. This model exploits the fact that when a 3 × 3 rotation matrix whose elements are squared is subtracted from its transpose, a matrix is produced whose non-diagonal elements have a common absolute value, where this value is an intrinsic property of the rotation matrix. For the traditional CKM quark mixing matrix with its second and third rows interchanged (i.e., c - t interchange), this value equals one-third the corresponding value for the leptonic matrix (roughly, 0.05 versus 0.15). By imposing this and two additional related constraints on mixing, and letting leptonic φ23 equal 45°, a framework is defined possessing just two free parameters. A mixing model is then specified using values for these two parameters that derive from an equation that reproduces the fine structure constant. The resultant model, which possesses no constants adjusted to fit experiment, has mixing angles of θ23 = 2.367445°, θ13 = 0.190987°, θ12 = 12.920966°, φ23 = 45°, φ13 = 0.013665°, and φ12 = 33.210911°. A fourth, newly-introduced constraint of the type described above produces a Jarlskog invariant for the quark matirx of 2.758 ×10−5. Collectively these achieve a good fit with the experimental quark and lepton mixing data. The model predicts the following CKM matrix elements: |Vus| = √0.05 = 2.236 × 10−1, |Vub| = 3.333 × 10−3, and |Vcb| = 4.131 × 10−2. For leptonic mixing the model predicts sin2φ12 = 0.3, sin2φ23 = 0.5, and sin2φ13 = 5.688 × 10−8. At the time of its 2007 introduction the model's values for |Vus| and |Vub| had disagreements with experiment of an improbable 3.6σ and 7.0σ, respectively, but 2010 values from the same source now produce disagreements of just 2.4σ and 1.1σ, the absolute error for |Vus| having been reduced by 53%, and that for |Vub| by 78%.
Category: High Energy Particle Physics

[1] viXra:1102.0012 [pdf] replaced on 2012-02-29 14:27:18

The Fine Structure Constant Derived from the Broken Symmetry of Two Simple Algebraic Identities

Authors: J. S. Markovitch
Comments: 4 Pages.

The fine structure constant is shown to arise naturally in the course of altering the symmetry of two algebraic identities. Specifically, the symmetry of the identity M2 = M2 is "broken" by making the substitution MMy on its left side, and the substitution MnMnxp on its right side, where p equals the order of the identity; these substitutions convert the above identity into the equation (My)2 = M2x2. These same substitutions are also applied to the only slightly more complicated identity (M / N)3 + M2 = (M / N)3 + M2 to produce this second equation (My)3 / N3 + (My)2 = (M3x3) / N3 + M2x3. These two equations are then shown to share a mathematical property relating to dy/dx, where, on the second equation’s right side this property helps define the special case (M3x3) / N3 + M2x3 = (103 − 0.13) / 33 + 102 − 0.13 = 137.036, which incorporates a value close to the experimental fine structure constant inverse.
Category: High Energy Particle Physics