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Related papers: Heavy baryonia

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The relativistic six-quark equations are found in the framework of the dispersion relation technique. The strange baryonia are constructed without the mixing of the quarks and antiquarks. The relativistic six-quark amplitudes of the strange…

High Energy Physics - Phenomenology · Physics 2020-08-26 S. M. Gerasyuta , E. E. Matskevich

The relativistic six-quark equations including the u, d quarks and antiquarks are found. The nonstrange baryonia B/bar B are contructed without the mixing of the quarks and antiquarks. The relativistic six-quark amplitudes of the baryonia…

High Energy Physics - Phenomenology · Physics 2011-05-05 S. M. Gerasyuta , E. E. Matskevich

The relativistic six-quark equations including the $u$, $d$ quarks and antiquarks are found. The nonstrange baryonia $B \bar B$ are constructed without the mixing of the quarks and antiquarks. The relativistic six-quark amplitudes of the…

High Energy Physics - Phenomenology · Physics 2011-07-15 S. M. Gerasyuta , E. E. Matskevich

The relativistic six-quark equations are found in the framework of the dispersion relation technique. The approximate solutions of these equations using the method based on the extraction of leading singularities of the heavy hexaquark…

High Energy Physics - Phenomenology · Physics 2015-05-28 S. M. Gerasyuta , E. E. Matskevich

The relativistic six-quark amplitudes of the nonstrange baryonia with the open charm are calculated. The poles of these amplitudes determine the masses of baryonia. 9 masses of baryonia are predicted.

High Energy Physics - Phenomenology · Physics 2012-12-04 S. M. Gerasyuta , E. E. Matskevich

The relativistic six-quark equations are constructed in the framework of the dispersion relation technique. The relativistic six-quark amplitudes of dibaryons including the light $u$, $d$ and heavy $c$, $b$ quarks are calculated. The…

High Energy Physics - Phenomenology · Physics 2015-05-30 S. M. Gerasyuta , E. E. Matskevich

In the framework of dispersion relation technique the relativistic three-quark equations including heavy quarks are found. The approximate solutions of the relativistic three-particles equations based on the extraction of leading…

High Energy Physics - Phenomenology · Physics 2009-11-07 S. M. Gerasyuta , D. V. Ivanov

The relativistic six-quark equations are found in the framework of the dispersion relation technique. The approximate solutions of these equations using the method based on the extraction of leading singularities of the amplitudes are…

High Energy Physics - Phenomenology · Physics 2014-11-20 S. M. Gerasyuta , E. E. Matskevich

The masses of negative parity $(70,1^-)$ charmed nonstrange baryons are calculated in the relativistic quark model. The relativistic three-quark equations of the $(70,1^-)$ charmed baryon multiplet are found in the framework of the…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. M. Gerasyuta , E. E. Matskevich

Masses of heavy baryons and tetraquarks are calculated in the relativistic quark model using the heavy-quark--light-diquark and diquark-antidiquark approximations, respectively.

High Energy Physics - Phenomenology · Physics 2007-12-05 D. Ebert , R. N. Faustov , V. O. Galkin

The relativistic five-quark equations are found in the framework of the dispersion relation technique.The five-quark amplitudes for the low-lying exotic baryons including the up and down quarks are calculated.The poles of the five-quark…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. M. Gerasyuta , V. I. Kochkin

The relativistic five-quark equations are found in the framework of the dispersion relation technique. The solutions of these equations using the method based on the extraction of the leading singularities of the amplitudes are obtained.…

High Energy Physics - Phenomenology · Physics 2015-12-29 S. M. Gerasyuta , V. I. Kochkin

In this work, we explore the charmed pentaquarks, where the relativistic five-quark equations are obtained by the dispersion relation technique. By solving these equations with the method based on the extraction of the leading singularities…

High Energy Physics - Phenomenology · Physics 2015-03-27 S. M. Gerasyuta , V. I. Kochkin , Xiang Liu

Simple and plausible rules are used to correlate the masses of the ground-state baryons containing single heavy ($b$ or $c$) quarks. A comparison with the experimental data shows that the observed mass difference between the $\Sigma_b$ and…

High Energy Physics - Phenomenology · Physics 2008-02-03 Agnieszka Zalewska , Kacper Zalewski

The masses of the yet undiscovered baryons containing single $c$ or $b$ quarks are estimated from the known masses using the following rules: equal distances in mass between the isomultiplets forming sextets, equal mass differences between…

High Energy Physics - Phenomenology · Physics 2007-05-23 Agnieszka Zalewska , Kacper Zalewski

The masses of the ground state heavy baryons consisting of two light (u,d,s) and one heavy (c,b) quarks are calculated in the heavy-quark--light-diquark approximation within the constituent quark model. The light quarks, forming the…

High Energy Physics - Phenomenology · Physics 2009-11-11 D. Ebert , R. N. Faustov , V. O. Galkin

The relativistic five-quark equations are found in the framework of the dispersion relation technique. The behavior of the low-energy five-particle amplitude is determined by its leading singularities in the pair invariant masses. The…

High Energy Physics - Phenomenology · Physics 2009-11-07 S. M. Gerasyuta , V. I. Kochkin

The masses of positive parity $(70,0^+)$ and $(70,2^+)$ nonstrange and strange baryons are calculated in the relativistic quark model. The relativistic three-quark equations of the $(70,L^+)$ multiplets are found in the framework of the…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. M. Gerasyuta , E. E. Matskevich

The relativistic three-quark equations of the ${\bf (70,1^-)}$ baryons are found in the framework of the dispersion relation technique. The approximate solutions of these equations using the method based on the extraction of leading…

High Energy Physics - Phenomenology · Physics 2007-05-23 S. M. Gerasyuta , E. E. Matskevich

We generalized our approach to the hypernuclei with $A=B=3$ containing one charm or one bottom quark. We derive the relativistic nine-quark equations using the dispersion relation technique. The hypernuclei as the system of interacting…

Nuclear Theory · Physics 2015-10-08 S. M. Gerasyuta , E. E. Matskevich
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