arXiv subjects
Publications and source records attributed to A. A. Arkhipov.
In this note we present additional arguments in favour of Kaluza and Klein picture of the world. In fact, we have shown that formula (\ref{KKpi}) provided by Kaluza-Klein approach with the fundamental scale early calculated (Eq.\ref{scale} \cite{1}) gives an excellent description for the mass spectrum of two-pion system.
In this note we present additional arguments in favour of Kaluza and Klein picture of the world. In fact, we show that formula (\ref{KK3pi}) provided by Kaluza-Klein approach with the fundamental scale early calculated \cite{1} gives an excellent description for the mass spectrum of three-pion system.
In this note we present additional arguments in favour of Kaluza and Klein picture of the world. We show that geniusly simple formula provided by Kaluza-Klein approach gives an excellent description for the mass spectrum of two-nucleon system. It has also been established that the experimental data obtained at low energies where the nucleon-nucleon dynamics has been studied reveal a special sort of (super)symmetry between fermionic (dibaryon) and bosonic states predicted by Kaluza-Klein scenario.
A manifestation of the three-body forces in multiparticle dynamics is discussed. The minireview of our recent results has been presented.
It has been shown that the great ancient Pythagorean ideas have found themselves in the latest researches in high energy elementary particles and nuclear physics. In this respect we concern and discuss the mathematical, physical and geometrical aspects of the famous Froissart theorem and in this way one establishes a link of this theorem to the mathematics and ideas elaborated in the Pythagorean school. A harmony of the Froissart theorem in fundamental dynamics of particles and nuclei has been displayed. We argue that a harmony of the Froissart theorem allow us to hear the new notes of {\it ``the music of the spheres"} just in the Pythagoreans sense.
The importance of cosmic-ray experimental measurements of proton-proton total cross sections to understand the underlying fundamental dynamics is discussed. It is shown that early discovered global structure of proton-proton total cross section [5,17] is completely compatible with the values obtained from cosmic-ray experiments.
Simple theoretical formula describing the global structure of pp and p\bar p total cross-secrions in the whole range of energies available up today has been derived. The fit to the experimental data with the formula has been made. It is shown that there is a very good correspondence of the theoretical formula to the existing experimental data.
A manifestation of narrow diproton resonances in the early discovered global structure of proton-proton total cross section at low energies is discussed. It is also discussed the existence of new particle with the mass $1.833 MeV$ predicted early.
The relationships between the fundamental dynamics and diffraction phenomena in scattering from two-body composite system are discussed. A new simple formula for the shadow corrections to the total cross-section in scattering from deuteron has been derived and new scaling characteristics with a clear physical interpretation have been established. The effect of weakening the inelastic screening at super-high energies is theoretically discovered. A comparison with the experimental data on proton(antiproton)-deuteron total cross-sections has been performed. It is shown that there is quite a remarkable correspondence of the theory with the experimental data.
New scaling structure for the shadow corrections in elastic scattering from deuteron at high energies has been presented and discussed. It is shown that this structure corresponds to the experimental data on proton(antiproton)-deuteron total cross sections. The effect of weakening for the inelastic screening at superhigh energies has been theoretically predicted.
The fundamental relation between the slopes of diffraction cone in single diffraction dissociation and elastic scattering has been derived.
The fundamental relations in the dynamics of single diffraction dissociation and elastic scattering at high energies are discussed.