Diffusion Monte Carlo calculations of fully-heavy (multiquark) bound states
arXiv:2009.11889 · doi:10.1103/PhysRevD.102.114007
Abstract
We use a diffusion Monte Carlo method to solve the many-body Schrödinger equation describing fully-heavy tetraquark systems. This approach allows to reduce the uncertainty of the numerical calculation at the percent level, accounts for multi-particle correlations in the physical observables, and avoids the usual quark-clustering assumed in other theoretical techniques applied to the same problem. The interaction between particles was modeled by the most general and accepted potential, i.e. a pairwise interaction including Coulomb, linear-confining and hyperfine spin-spin terms. This means that, in principle, our analysis should provide some rigorous statements about the mass location of the all-heavy tetraquark ground states, which is particularly timely due to the very recent observation made by the LHCb collaboration of some enhancements in the invariant mass spectra of -pairs. Our main results are: (i) the , () and lowest-lying states are located well above their corresponding meson-meson thresholds; (ii) the ground state with preferred quark-antiquark pair configurations is compatible with the enhancement(s) observed by the LHCb collaboration; (iii) our results for the and sectors seem to indicate that the and ground states are almost degenerate with the located around above them; (iv) smaller mass splittings for the system are predicted, with absolute mass values in reasonable agreement with other theoretical works; (v) the tetraquark ground state lies at its lowest -wave meson-meson threshold and it is compatible with a molecular configuration.
19 pages, 7 figures, 15 tables
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