scholarly journals Hexaquarks in the coupled-channel formalism

2010 ◽  
Vol 82 (5) ◽  
Author(s):  
S. M. Gerasyuta ◽  
E. E. Matskevich
1988 ◽  
Vol 209 (2-3) ◽  
pp. 168-172 ◽  
Author(s):  
M. Bernath ◽  
O. Dragún ◽  
J.E. Testoni ◽  
H. Massmann

2010 ◽  
Vol 3 ◽  
pp. 03031
Author(s):  
E.P. Biernat ◽  
W. Schweiger ◽  
K. Fuchsberger ◽  
W.H. Klink

2010 ◽  
Vol 19 (11) ◽  
pp. 2181-2188 ◽  
Author(s):  
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 u, d, s, and bottom quarks, are constructed. The poles of these amplitudes determine the masses and widths of S-wave bottom tetraquarks.


2016 ◽  
Vol 31 (10) ◽  
pp. 1650058 ◽  
Author(s):  
Peng Guo

From dispersion relation approach, a formalism that describes final state interaction among three particles in a coupled-channel system is presented. Different representations of coupled-channel three-body formalism for spinless particles in both initial and final states are derived.


2014 ◽  
Vol 23 (03) ◽  
pp. 1450011
Author(s):  
S. M. Gerasyuta ◽  
E. E. Matskevich

The relativistic six-quark equations for the molecule NΞ 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 pole of these amplitudes determines the mass of NΞ state M = 2252 MeV. The binding energy is equal to 3 MeV.


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