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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Bibliographic Details
Published inThe European physical journal. C, Particles and fields Vol. 81; no. 4; pp. 1 - 14
Main Author Mutuk, Halil
Format Journal Article
LanguageEnglish
Published Berlin/Heidelberg Springer Berlin Heidelberg 01.04.2021
Springer
Springer Nature B.V
SpringerOpen
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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.
ISSN:1434-6044
1434-6052
DOI:10.1140/epjc/s10052-021-09176-8