Scattering of charmed baryons on nucleons
arXiv:1711.06470 · doi:10.1140/epja/i2018-12638-7
Abstract
Chiral effective field theory is utilized for extrapolating results on the interaction, obtained in lattice QCD at unphysical (large) quark masses, to the physical point. The pion-mass dependence of the components that constitute the potential up to next-to-leading order (pion-exchange diagrams and four-baryon contact terms) is fixed by information from lattice QCD simulations. No recourse to SU(3) or SU(4) flavor symmetry is made. It is found that the results of the HAL QCD Collaboration for quark masses corresponding to -- MeV imply a moderately attractive interaction at MeV with scattering lengths of fm for the as well as the partial waves. For such an interaction the existence of a charmed counterpart of the hypertriton is unlikely but four- and/or five-baryons systems with a baryon could be indeed bound.
7 pages, 2 figures; table added, several comments added
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- Precision Studies of QCD in the Low Energy Domain of the EIC
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- Spin-isospin Kondo effects for and baryons and and mesons
- Pion-mass dependence of the nucleon-nucleon interaction
- Charmed nuclei within a microscopic many-body approach
- Femtoscopic correlations and the interaction
- interaction in leading order covariant chiral effective field theory
- Charmed baryonnucleon interaction
- Predictions for charmed nuclei based on forces inferred from lattice QCD simulations
- Charmed dibaryon resonances in the potential quark model
- Charmed baryons in nuclear matter
- Single hypernuclei within quark mean-field model
- Towards modeling the short-range interactions of hidden/open charm pentaquark molecular states
- Ground State Properties of Charmed Hypernuclei with Mean Field Approach
- Predicting possible molecular states of nucleons with , , and
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- Finding Interaction Mechanism between Exotic Molecule and Conventional Hadron