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Related papers: Scalar tetraquarks with open bottom

200 papers

Masses of tetraquarks with two heavy quarks and open charm and bottom are calculated in the framework of the diquark-antidiquark picture in the relativistic quark model. All model parameters were regarded as fixed by previous considerations…

High Energy Physics - Phenomenology · Physics 2008-11-26 D. Ebert , R. N. Faustov , V. O. Galkin , W. Lucha

The four-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 obtained. The…

High Energy Physics - Phenomenology · Physics 2014-04-25 S. M. Gerasyuta , V. I. Kochkin

Diquarks are found to have the right degrees of freedom to describe the tetraquark poles in hidden-charm to open-charm meson-meson amplitudes. Compact tetraquarks result as intermediate states in non-planar diagrams of the 1/N expansion and…

High Energy Physics - Phenomenology · Physics 2016-07-20 L. Maiani , A. D. Polosa , V. Riquer

The relativistic five-quark equations are found in the framework of the dispersion relation technique. The five-quark amplitude for the N(1688) resonance including u-, d- quarks is calculated. The pole of this amplitude determines the mass…

High Energy Physics - Phenomenology · Physics 2007-07-05 S. M. Gerasyuta , V. I. Kochkin

The relativistic four-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 leading singularities of the amplitudes are obtained. The…

High Energy Physics - Phenomenology · Physics 2009-10-31 S. M. Gerasyuta , V. I. Kochkin

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

Tetraquarks are studied with an approximation which reduces the in- ternal degrees of freedom of the system, using both finite differences and scattering theory. The existence of bound states and resonances is inspected and the masses and…

High Energy Physics - Phenomenology · Physics 2012-10-12 Marco Cardoso , Pedro Bicudo , Nuno Cardoso

Masses of the ground state light tetraquarks are dynamically calculated in the framework of the relativistic diquark-antidiquark picture. The internal structure of the diquark is taken into account by calculating the form factor of the…

High Energy Physics - Phenomenology · Physics 2010-04-15 D. Ebert , R. N. Faustov , V. O. Galkin

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

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

Scalar tetraquark states are studied within the diquark-antidiquark picture in a non-relativistic approach. We consider two types of confining potentials, a quadratic and a linear one, to which we also add spin-spin, isospin-isospin, and…

High Energy Physics - Phenomenology · Physics 2021-11-10 Zahra Ghalenovi , Francesco Giacosa , Dirk H. Rischke

The relativistic model of the ground state and excited heavy tetraquarks with hidden bottom is formulated within the diquark-antidiquark picture. The diquark structure is taken into account by calculating the diquark-gluon vertex in terms…

High Energy Physics - Phenomenology · Physics 2009-04-17 D. Ebert , R. N. Faustov , V. O. Galkin

The mass and meson-current coupling of the diquark-antidiquark states with the quantum numbers $J^{P}=0^{+}$ and quark contents $Z_{q}=[cq][\bar {b} \bar q ]$ and $Z_{s}=[cs][\bar {b} \bar s]$ are calculated using two-point QCD sum rule…

High Energy Physics - Phenomenology · Physics 2017-02-22 S. S. Agaev , K. Azizi , H. Sundu

The masses of heavy tetraquarks with hidden charm and bottom are calculated in the framework of the relativistic quark model. The tetraquark is considered as the bound state of a heavy-light diquark and antidiquark. The light quark in a…

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

We present a numerical solution of the four-quark Bethe-Salpeter equation for a scalar tetraquark. We find that the four-body equation dynamically generates pseudoscalar poles in the Bethe-Salpeter amplitude. The sensitivity to the pion…

High Energy Physics - Phenomenology · Physics 2015-07-20 Gernot Eichmann , Christian S. Fischer , Walter Heupel

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

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 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

We present a numerical solution of the four-quark Bethe-Salpeter equation for ground-state scalar tetraquarks with J^PC = 0^++. We find that the four-body equation dynamically generates pseudoscalar-meson poles in the Bethe-Salpeter…

High Energy Physics - Phenomenology · Physics 2015-12-21 Gernot Eichmann , Christian S. Fischer , Walter Heupel

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