Predictions for charmed nuclei based on forces inferred from lattice QCD simulations
arXiv:2003.07768 · doi:10.1140/epja/s10050-020-00185-x
Abstract
Charmed nuclei are investigated utilizing and interactions that have been extrapolated from lattice QCD simulations at unphysical masses of -- MeV to the physical point using chiral effective field theory as guideline. Calculations of the energies of single-particle bound states for various charmed nuclei from Li to Bi are performed using a perturbative many-body approach. This approach allows one to determine the finite nuclei self-energy from which the energies of the different bound states can be obtained. Though the interaction inferred from the lattice results is only moderately attractive, it supports the existence of charmed nuclei. Already the lightest nucleus considered is found to be bound. The spin-orbit splitting of the p- and d-wave states turns out to be small, as in the case of single hypernuclei. Additional calculations based on the Faddeev-Yakubovsky equations suggest that also systems involving a baryon are likely to be bound, but exclude a bound He state.
13 pages, 5 figures
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- Chiral perturbation theory for heavy hadrons and chiral effective field theory for heavy hadronic molecules
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- Ground State Properties of Charmed Hypernuclei with Mean Field Approach
- Charmed hypernuclei within density-dependent relativistic mean-field theory
- Singly heavy baryons in nuclear matter from an SU(3) chiral soliton model
- A simple model of the charmed hypertriton