[7] **viXra:1304.0172 [pdf]**
*replaced on 2013-05-01 06:31:25*

**Authors:** Keith D. Foote

**Comments:** 4 Pages.

This thesis explores the concept of proton splitting as a possible energy source. Possible methods of initiating the split are presented.

**Category:** High Energy Particle Physics

[6] **viXra:1304.0150 [pdf]**
*replaced on 2013-12-23 11:54:29*

**Authors:** Mario Everaldo de Souza

**Comments:** 4 Pages.

The allowed and suppressed Higgs-like bosons couplings to quarks are identified. The relative ratios of strengths of allowed couplings are calculated. The latter is extremely important for experimentalists in the determination of the nature of the recently found Higgs boson and in the search for the charged Higgs-like bosons.

**Category:** High Energy Particle Physics

[5] **viXra:1304.0108 [pdf]**
*replaced on 2015-12-16 05:50:50*

**Authors:** Sylwester Kornowski

**Comments:** 2 Pages.

Here within the lacking part of ultimate theory, i.e. the Scale-Symmetric Theory, we calculated the relative pseudorapidity density in inelastic proton-proton collisions. The derived very simple formula is consistent with all experimental data.

**Category:** High Energy Particle Physics

[4] **viXra:1304.0071 [pdf]**
*replaced on 2015-05-30 11:09:51*

**Authors:** Frank Dodd Tony Smith Jr

**Comments:** 16 Pages.

Real Clifford Algebras roughly represent the Geometry of Real Vector Spaces of signature (p,q) with the Euclidean Space (0,q) sometimes just being written (q) so that the Clifford algebra Cl(0,q) = Cl(q). A useful starting place for understanding how they work is to look at the most central example and then extend from it to others. This paper is only a rough introductory description to develop intuition and is NOT detailed or rigorous - for that see the references. Real Clifford Algebras have a tensor product periodicity property whereby Cl(q+8) = Cl(q) x Cl(8) so that if you understand Cl(8) you can understand larger Clifford Algebras such as Cl(16) = Cl(8) x Cl(8) and so on for as large as you want. So Cl(8) is taken to be the central example in this paper which has 4 parts: How Cl(8) works; What smaller Clifford Algebras inside Cl(8) look like; How the larger Clifford Algebra Cl(16) gives E8: How larger Clifford Algebras Cl(16N) = Cl(8(2N)) give in the large N limit a generalized Hyperfinite II1 von Neumann factor. V2 adds Creation and Annihilation Operators of AQFT as A7+h_92 Contraction of E8. V3 adds discussion about AQFT Possibility Space.

**Category:** High Energy Particle Physics

[3] **viXra:1304.0053 [pdf]**
*replaced on 2014-10-03 15:24:28*

**Authors:** Mario Everaldo de Souza

**Comments:** 4 Pages. Final version to be published in the proceedings of BEACH 2014.

The Morse molecular potential is used for the rst time as an effective potential for the overall interaction in charmonium. This procedure allows the calculation of the rotational
contributions of P states, the radii of ve S states, and an absolute threshold for bound states. The calculation of the latter provides important information on the character of the recently found levels X(3915), X(3940), Psi(4040),
X(4050), X(4140), Psi(4160), X(4160), X(4250),
X(4260), X(4350), Psi(4415), X(4430), and X(4660).

**Category:** High Energy Particle Physics

[2] **viXra:1304.0035 [pdf]**
*submitted on 2013-04-07 20:50:15*

**Authors:** Andrew Nassif, Nasir Germain

**Comments:** 2 Pages. Extremely short commentary

I Andrew Nassif believe that light travels
in curved paths that are straight lines,
however the paths are made of particles
which still technically goes under Nasir’s
theory as well as other scientific theories.
If I am correct then this would be a big
realization in the world of Physics and
science.

**Category:** High Energy Particle Physics

[1] **viXra:1304.0008 [pdf]**
*replaced on 2015-12-14 09:58:35*

**Authors:** Sylwester Kornowski

**Comments:** 8 Pages.

The Scale-Symmetric Theory (SST) is the lacking part of the Theory of Everything. SST describes the succeeding phase transitions of the non-gravitating Higgs field, the atom-like structure of baryons, and many other basic problems. Here, within SST, we calculated the magnetic moments and precise masses of hyperons, their spin and strangeness. Obtained results are consistent or very close to experimental data.

**Category:** High Energy Particle Physics