Nonrelativistic treatment of fully-heavy tetraquarks as diquark-antidiquark states
The goal of the present work is to obtain a reliable estimate of the masses of the ground and radially excited states of fully-heavy tetraquark systems. In order to do this, we use a nonrelativistic model of tetraquarks which are assumed to be compact and consist of diquark-antidiquark pairs. This n...
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Published in | The European physical journal. C, Particles and fields Vol. 81; no. 4; pp. 1 - 14 |
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Main Author | |
Format | Journal Article |
Language | English |
Published |
Berlin/Heidelberg
Springer Berlin Heidelberg
01.04.2021
Springer Springer Nature B.V SpringerOpen |
Subjects | |
Online Access | Get full text |
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Summary: | The goal of the present work is to obtain a reliable estimate of the masses of the ground and radially excited states of fully-heavy tetraquark systems. In order to do this, we use a nonrelativistic model of tetraquarks which are assumed to be compact and consist of diquark-antidiquark pairs. This nonrelativistic model is composed of Hulthen potential, a linear confining potential and spin-spin interaction. We computed ground, first, and second radially excited
c
c
c
¯
c
¯
and
b
b
b
¯
b
¯
tetraquark masses. It was found that predicted masses of ground states of
c
c
c
¯
c
¯
and
b
b
b
¯
b
¯
tetraquarks are significantly higher than the thresholds of the fall-apart decays to the lowest allowed two-meson states. These states should be broad and are thus difficult to observe experimentally. First radially excited states are considerably lower than their corresponding (2S-2S) two-meson thresholds. We hope that our study may be helpful to the experimental search for ground and excited
c
c
c
¯
c
¯
and
b
b
b
¯
b
¯
tetraquark states. |
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ISSN: | 1434-6044 1434-6052 |
DOI: | 10.1140/epjc/s10052-021-09176-8 |