Here is the link to my new paper (8 pages) titled:
The Positron Fraction in Primary Cosmic Rays and New Cosmological Problems
http://vixra.org/abs/1411.0018
Abstract
Here, within the Scale-Symmetric Everlasting Theory (S-SET), I calculated the positron fraction in primary cosmic rays as a function of energy and described positron flux. Obtained results are consistent with the data from the Alpha Magnetic Spectrometer (AMS) on the International Space Station (ISS). These data lead to the internal structure of the core of baryons and to phenomena characteristic for regions in the Universe filled with baryonic plasma described within S-SET. Here, as well within S-SET, I described the origin of new cosmological problems which lead to new cosmology. They are as follows. There are not in existence the B-modes associated with gravitational waves - it leads to conclusion that there was a separation in time of the inflation and the big bang of the Universe. In the very distant Universe there is too small number of dwarf galaxies. In the very distant Universe there are the massive galaxies which do not significantly evolve so a time for their formation was too short. In the very distant Universe there are too many barred galaxies - it is inconsistent with simulations grounded on the Cosmological Standard Model (CSM). There is a substantial asymmetry in the CMB signal observed in the two opposite hemispheres of the sky. These new problems suggest that CSM starts from wrong initial conditions.
In this paper I showed that all characteristic features of the positron fraction (the ratio of positrons to sum of positrons and electrons) and flux we obtain multiplying the characteristic features of the core of nucleons (it was described within the atom-like structure of baryons, within the S-SET, already in 1997) by the same number 651.88. The obtained theoretical results are consistent with the observational facts and are perfect.
What is the origin of the number 651.88? Due to the collisions of the cores of baryons inside baryonic plasma, there, due to the weak interactions, appear the characteristic condensates which follow from the structure of the core. The energy of the weak condensates leaks outside the baryonic plasma but then there appear the electromagnetic interactions. In the transitions from weak to electromagnetic interactions, the energy must increase just 651.88 times i.e. in such processes temperature of the baryonic plasma decreases. The number 651.88 is the ratio of the fine-structure constant (formula (21) in my book; online it was published on 6 March 2012) and the coupling constant for the weak interactions of protons and electrons/positrons (formula (58) in my book; online it was published on 6 March 2012).
Inside protons and neutrons, the core can be charged positively or can be neutral, it cannot be charged negatively (see my book). It causes that the positron-electron pairs produced inside baryonic plasma appear as the pairs of real positron and virtual electron - it leads to the excess of detected positrons in cosmic rays.
Moreover, my theory is testable. In future experiments we should observe rapid drop in positron fraction for energy of positrons equal to about 474 GeV. This value follows from the mass of the charged core of baryons 727.44 MeV. In present experiments, for energies close to 500 GeV, the uncertainties are too high to define correctly the threshold.
My Scale-Symmetric Everlasting Theory shows that the positron fraction has nothing with the dark matter as it is assumed in the other models.
Remember that the atom-like structure of baryons, which leads to the positron fraction and flux, leads as well to the exact mass, spin and electron and muon radii of proton. On the other hand, within the mainstream three-valence-quarks model we cannot calculate exact mass, spin and muon radius of proton.