Heavy Tetraquarks in the Diquark-Antidiquark Picture
arXiv:1511.08542 · doi:10.1016/j.physletb.2015.11.072
Abstract
The homogeneous Lippmann-Schwinger integral equation is solved in momentum space to calculate the masses of heavy tetraquarks with hidden charm and bottom. The tetraquark bound states are studied in the diquark-antidiquark picture as a two-body problem. A regularized form of the diquark-antidiquark potential is used to overcome the singularity of the confining potential at large distances or small momenta. Our numerical results indicate that the relativistic effect leads to a small reduction in the mass of heavy tetraquarks, which is less than for charm and less than for bottom tetraquarks. The calculated masses of heavy tetraquarks for , , , and states are in good agreement with other theoretical calculations and experimental data. Our numerical analysis predict the masses of heavy tetraquarks for , and states for the first time, and we are not aware of any other theoretical results or experimental data for these states.
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