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Related papers: Widths of tetraquarks with open charm

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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 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 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 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

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 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 negative parity…

High Energy Physics - Phenomenology · Physics 2015-05-20 S. M. Gerasyuta , V. I. Kochkin

The relativistic four-quark equations in the framework of the dispersion relation technique are derived. The four-quark amplitudes of the scalar tetraquarks with open bottom, including u, d, s and bottom quarks, are constructed. The poles…

Nuclear Theory · Physics 2008-12-04 S. M. Gerasyuta , V. I. Kochkin

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 relativistic four-quark equations are found in the framework of the dispersion relation technique. The dynamical mixing of the four-quark amplitudes and the glueball amplitudes is considered. The approximate solutions of these equations…

High Energy Physics - Phenomenology · Physics 2009-09-02 S. M. Gerasyuta , V. I. Kochkin

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 masses of the excited heavy tetraquarks with hidden charm are calculated within the relativistic diquark-antidiquark picture. The dynamics of the light quark in a heavy-light diquark is treated completely relativistically. The diquark…

High Energy Physics - Phenomenology · Physics 2008-12-18 D. Ebert , R. N. Faustov , V. O. Galkin

The masses of the heavy tetraquarks with open charm and bottom are calculated within the diquark-antidiquark picture in the framework of the relativistic quark model. The dynamics of the light quarks and diquarks is treated completely…

High Energy Physics - Phenomenology · Physics 2011-01-27 D. Ebert , R. N. Faustov , V. O. Galkin

The masses of the ground state and excited heavy tetraquarks with hidden charm and bottom are calculated within the relativistic diquark-antidiquark picture. The dynamics of the light quark in a heavy-light diquark is treated completely…

High Energy Physics - Phenomenology · Physics 2009-11-13 D. Ebert , R. N. Faustov , V. O. Galkin

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

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 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 2011-08-11 S. M. Gerasyuta , I. V. Kochkin

The relativistic five-quark equations are found in the framework of the dispersion relation technique. The five-quark amplitudes for the low-lying pentaquarks including the u,d,s-quarks are calculated. The poles of these amplitudes…

High Energy Physics - Phenomenology · Physics 2015-06-25 S. M. Gerasyuta , V. I. Kochkin

The relativistic generalization of Faddeev-Yakubovsky approach is constructed in the form of the dispersion relations. The five-quark amplitudes for the low-lying pentaquarks contain u,d,s-quarks. The poles of these amplitudes determine the…

High Energy Physics - Phenomenology · Physics 2009-11-11 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

Masses of the ground, orbitally and radially excited states of the asymmetric fully heavy tetraquarks, composed of charm (c) and bottom (b) quarks and antiquarks are calculated in the relativistic diquark-antidiquark picture. The…

High Energy Physics - Phenomenology · Physics 2024-05-07 V. O. Galkin , E. M. Savchenko
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