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Related papers: Relativistic five-quark equations and negative par…

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We have investigated uudd\sbar pentaquarks by employing quark models with the meson exchange and the effective gluon exchange as qq and q\qbar interactions. The system for five quarks is dynamically solved; two quarks are allowed to have a…

High Energy Physics - Phenomenology · Physics 2017-08-23 Sachiko Takeuchi , Kiyotaka Shimizu

The relativistic four-quark equations are found in the framework of the dispersion relation technique. The calculations of non-qq meson amplitudes estimate the contributions of three subamplitudes: four-quark amplitude, glueball amplitude…

High Energy Physics - Phenomenology · Physics 2007-05-23 S. M. Gerasyuta , V. I. Kochkin

The relativistic four-quark equations are found in the framework of coupled-channel formalism. The dynamical mixing of the meson-meson states with the four-quark states is considered. The approximate solutions of these equations using the…

High Energy Physics - Phenomenology · Physics 2008-12-30 S. M. Gerasyuta , V. I. Kochkin

The relativistic six-quark equations for the molecule $N\Xi$ are found in the dispersion relation technique. The relativistic six-quark amplitudes of the hexaquark including the quarks of three flavors ($u$, $d$, $s$) are calculated. The…

High Energy Physics - Phenomenology · Physics 2015-06-17 S. M. Gerasyuta , E. E. Matskevich

The relativistic four-quark equations are found in the framework of coupled-channel formalism. The dynamical mixing of the meson-meson states with the four-quark states is considered. The four-quark amplitudes of the tetraquarks with hidden…

High Energy Physics - Phenomenology · Physics 2008-12-02 S. M. Gerasyuta , V. I. Kochkin

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

High Energy Physics - Phenomenology · Physics 2016-04-18 S. M. Gerasyuta , E. E. Matskevich

The relativistic four-quark equations are found in the framework of coupled-channel formalism. The dynamical mixing of the meson-meson states with the four-quark states is considered. The four-quark amplitudes of the tetraquarks, including…

High Energy Physics - Phenomenology · Physics 2011-03-02 S. M. Gerasyuta , V. I. Kochkin

The relativistic nine-quark equations are found in the framework of the dispersion relation technique. $ ^3 He$ nucleus is described by these equations. We consider the $ ^3 He$ as the system of interacting quarks and gluons. The…

High Energy Physics - Phenomenology · Physics 2019-08-19 S. M. Gerasyuta , E. E. Matskevich

The relativistic four-quark equations with the open-charm and the open-strange are found in the framework of coupled-channel formalism. The dynamical mixing of the meson-meson states with the four-quark states is considered. The four-quark…

High Energy Physics - Phenomenology · Physics 2013-12-25 S. M. Gerasyuta , V. I. Kochkin

Hypernuclei $ ^4_Y He$, $ ^4_Y H$, $ ^4_{YY} He$, $ ^4_{YY} H$, where $Y=\Lambda$, $\Sigma_0$, $\Sigma_+$, $\Sigma_-$, A=4 are considered using the relativistic twelve-quark equations in the framework of the dispersion relation technique.…

Nuclear Theory · Physics 2015-09-30 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

In the framework of the dispersion relation technique the relativistic six-quark equations for the molecule $\Sigma_b \Sigma_b^*$ are found. The relativistic six-quark amplitudes of the hexaquark including the quarks of three flavors ($u$,…

High Energy Physics - Phenomenology · Physics 2014-03-26 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 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 four-quark equations are found in the framework of coupled-channel formalism. The dynamical mixing of the meson-meson states with the four-quark states is considered. The four-quark amplitudes of the tetraquarks with hidden…

High Energy Physics - Phenomenology · Physics 2008-09-17 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

We have investigated negative-parity uudd\bar{s} pentaquarks by employing a quark model with the meson exchange and the effective gluon exchange as qq and q\bar{q} interactions. The system for the five quarks is dynamically solved; the…

High Energy Physics - Phenomenology · Physics 2009-11-10 Sachiko Takeuchi , Kiyotaka Shimizu

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

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

High Energy Physics - Phenomenology · Physics 2012-04-02 S. M. Gerasyuta , E. E. Matskevich

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 masses of S-wave bottom baryons are calculated in the framework of coupled-channel formalism. The relativistic three-quark equations for the bottom baryons using the dispersion relation technique are found. The approximate solutions of…

High Energy Physics - Phenomenology · Physics 2015-05-13 S. M. Gerasyuta , E. E. Matskevich