arXiv subjects

Oleg A. Teplov

Publications and source records attributed to Oleg A. Teplov.

8 recordsLinked to original sources

arXiv2009

Quark flowers and quark condensation

The mass formation of basic vector mesons up to energy 3.8 GeV was studied. The investigation was done with using of jet mechanism, the harmonic quarks and neutral colorless groups. The stage of a whole string with a zero interquark momentum was considered as a separate stage of hadronization. The quark group with rest mass equal to experimental mass of hadron was named as flower. The quark flowers were found for $ρ$, $ω$, $φ$, $ψ/J$, $ψ$(2S) and $ψ$(3770). The flower mass of $ψ$(2S) was defined as 3686.09 MeV. The structure of quark flowers is symmetrical and consists from an aura and central part. The formation of quark shells, the condensation of quarks on the quark leaders, the floral schemes of kaon formation and complicated hadronization are discussed.

physics.gen-ph↗

arXiv2008

The exact interpretation of mass differences in upper part of the charmonium spectrum

Mass differences of the charmonium mesons $ψ$(3770), $X$(3872), $χ$(3929), $X$(3940), $ψ$(4040), $ψ$(4160), $X$(4259) and $ψ$(4415) have been studied. The analysis of data has shown, 5 of 7 mass differences with $ψ$(4415) are precisely interpreted by using of harmonic quarks and their complete oscillators. Upper part of the charmonium spectrum consists of two groups. Except for two particles ($ψ$(3770) and $ψ$(4040)) connected among themselves, the others 5 particles are connected with a meson $ψ$(4415). The levels are separated by elementary groups of harmonic quarks and completed oscillators. Experimental and calculated data are in the good consent. The masses of mesons $ψ$(4415), $X$(4260), $ψ$(4160), $X$(3943) and $χ$(3929) were recalculated. The second group demonstrates that harmonic quarks can also well work below threshold $D\bar{D}$.

physics.gen-ph↗

arXiv2007

The six-quark structure of long-lived $D$-mesons and $ψ/J$

The harmonic quarks are applied to the analysis of quark structures of long-lived $D$-mesons and $ψ/J$. In the harmonic quark model the quarks of long-lived mesons ($π^0$, $π^\pm$, $K^\pm$, $K^0$, $B^0$, $B^\pm$) are weakly relativistic objects with the excess energy of valent quarks less than 7 MeV. In contrast to this, the long-lived $D$-mesons in two-quark standard have the apparent excess energies of a few hundred MeV. It was established that all long-lived $D$-mesons and $ψ/J$ have the six-quark structures. There are two valent quarks and two additional neutral quark-antiquark $u$-pairs. The quark structures of $D^0$, $D^\pm$, $D_s^\pm$ and $ψ/J$ are given. The excess energies of six-quark $D$-mesons also does not exceed 7 MeV. A six-color quark composition and the absence of two-quark $D$-mesons in the context of QCD are discussed.

hep-ph↗

arXiv2006

The exact quantization of the CLEO and BELLE data for $D$ mass differences by the harmonic quarks and oscillators

The harmonic quarks and their complete oscillators are successfully used for the exact quantitative results and an explanation of the $D$ meson mass differences. For the first time it is shown that the mass differences of the charmed mesons with the same flavors are strictly quantized by the rest masses of harmonic quarks in both "free" state and complete oscillator state. The $D^*(2007)^0$ $\to$ $D^0$ transition has the following neutral quark group: $d$-oscillator + $u^0$-quark with rest energy 142.124 MeV. It is argued that it is the unique model solution within the 4$σ$ experimental interval. The $D_s^{*+}$ - $D_s^+$ mass difference is quantized by the simplest quark reaction with the difference energy 143.756 MeV. The energy of the $D_{sJ}$(2460)$^+$ $\to$ $D_s^+$ transition explains by the decay of the one complete $s$-oscillator with the energy 491.33 MeV. The full agreement with experimental data of CLEO and BELLE is obtained. The problems of a quark shells and the quantization by quark rest masses are discussed.

hep-ph↗

arXiv2005

Precise mass spectrum of mesons with open charm in the harmonic quarks and oscillators

The harmonic quarks and their complete oscillators are presenting the unprecedented exact solution for the mass spectrum of mesons with an explicit charm. The experimental and calculated spectrums coincide with standard deviation in 1.8 MeV. The four doublets and experimental errors of meson masses give the main contribution in this value. The harmonic spectrum is not sensitive to an isospin. The spectrum is simple, complete, precise and logically clear. It's easy to make predictions. The spectrum has not free parameters. It's supposed that the spectrum of harmonic and mixed levels is an exterior spectrum of allowed energy states in relation to a QCD states. The features of the harmonic spectrum, some levels of charm hadrons, the acceptor property of a c-quark, the mass rank of quarks and the nature of leptons are discussed.

hep-ph↗

arXiv2004

The harmonic quarks and hadrons up to 1000 MeV

The calculations and analysis of a variance have shown, that masses of mesons up to 1000 MeV strongly correlate with a model spectrum of potential wells at mass of harmonic up-quark 105.6 MeV. It is shown, that probability of casual correspondence of the meson and model spectrums is less than 1 ppm. The harmonic quark model is applied to L=0 hadrons for the analysis of them structures and detection of them filled quark shells. The possible quark structures of all mesons up to 1000 MeV are given. The completely neutral simple boson configurations are found for a threshold a proton-antiproton and the total mass of neutral pion and kaon. Mass relations are fulfilled with precision near 0.01%. It is supposed, that new relations is connected with Higgs mechanism of mass formation. The final precision of calculated masses of harmonic quarks is estimated as 0.005%.

hep-ph↗

arXiv2003

Harmonic quarks: properties and some applications

In this work the investigation of hadronic structures with the help of the harmonic quarks is prolonged. The harmonic quark model is good at describing the meson structures and the baryon excitations to resonances, in particular delta(1232). Harmonic quark reactions form the structure of the baryon resonances. Presumed quark structures of the mesons eta(548), omega(772), a(980) and f(980) are given. It became clear that the some hadronic structures contain the filled quark shells. The kinetic quark energy in the basic charged mesons are enough small for a using of perturbative methods. The following topics are briefly considered and discussed: harmonic quark series and its boundaries, the d-quark peculiarity, parallel quark series and quark mixing. The boundaries of quark chain can are closely related to a weak interaction. The cause of the quark mixing is probably an existence of the parallel quark chain and the special properties of the d-quark in the main quark chain. The new mass equation is found. It is probably a manifestation of Higgs mechanism. Using this equality enables to improve the accuracy of the harmonic quark masses calculation to 0.005%. The strong interaction should take into account the harmonic quark annihilation.

hep-ph↗

arXiv2003

Harmonic quarks and their precise masses

An examination of charged two-quark meson masses hinted that the mass ratio of neighboring quarks could simply be a constant. The concept of a harmonic quark oscillator based on a quark-antiquark pair is introduced. Unstable symmetric state of the harmonic quark oscillator can be broken to an asymmetric state with the formation the neighboring quark of lesser mass due to a weak reaction. A new recurrent equation of quark masses is obtained and the model of harmonic quark family is developed. The quark masses in the model are bound together into one rigid chain. With the electromagnetic contribution taken into account the quark masses are calculated with the 0.03 percent inaccuracy. It follows from the model that the muon is a single u-quark mass state fixed as a lepton. The neutral pion is probably a stable harmonic oscillator based on a quark-antiquark u-pair.

hep-ph↗