Diffusion Monte Carlo calculations of fully-heavy compact hexaquarks

Abstract

We used a diffusion Monte Carlo technique to describe the properties of fully-heavy compact arrangements (no dibaryon molecules) including six quarks and no antiquarks within the framewok of a constituent quark model. Only arrangements whose wavefunctions were eigenvectors of $L^2$ with eigenvalue $\ell$ = 0 were taken into account, what means that we only considered the subset of all the possible color-spin combinations that make the total wavefunctions antisymmetric with respect to the interchange of any two quarks of the same type. This means arrangements with spin $S=0$ for $cccccc$, $bbbbbb$, $cccccb$, $bbbbbc$ and $cccbbb$ and spin $S=0,1,2$ for the $ccccbb$ and $bbbbcc$ hexaquarks. In all cases, the masses of the six-quark arrangements are larger that the ones corresponding to the sum of any of the two baryons we can split them into, but smaller that the ones for a set of six isolated quarks, i.e., all them are bound systems. The analysis of their structure indicates that all the hexaquarks considered in this work are compact objects, except the $cccbbb$, that appears to be a loose association of two baryons.

5 pages, 4 figures; Paper has been structured in parts. Method part has been rewritten to clarify some steps. Results for cccccb and bbbbbc 1+ states and cccbbb 1+, 2+ and 3+ states has been added

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Cited by in corpus (11)

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• Doubly charmed dibaryon states
• Systematics of fully heavy dibaryons
• Prediction of charmed-bottom pentaquarks in quark model
• Heavy Hexaquarks in the Flux Tube Model
• Observation of $e^{+}{e}^{-}\to pp\bar{p}\bar{n}{\pi }^{-}+c.c.$
• Possible bound states in the triple-${\eta }_c$ and triple-$J/\psi$ systems
• Study of the ${\Omega }_{ccc}{\Omega }_{ccc}$ and ${\Omega }_{bbb}{\Omega }_{bbb}$ dibaryons in QCD Sum Rules