J=3/2 charmed hypertriton
arXiv:1508.03535 · doi:10.1103/PhysRevC.92.024006
Abstract
By solving exact three-body equations, we study the three-baryon system with charm . We look for possible bound states using baryon-baryon interactions obtained from a chiral constituent quark model. The smaller effect of the conversion reverses the order of the and states, rather close on the strange sector. The diminishing of the kinetic energy due to the large reduced mass gives rise to a bound state in the channel. After correcting for Coulomb effects the binding energy would be between 140 and 715 keV.
12 pages, 5 figures. To appear in Phys. Rev. C. arXiv admin note: text overlap with arXiv:hep-ph/0701275
References in corpus (7)
Cited by in corpus (19)
- Chiral perturbation theory for heavy hadrons and chiral effective field theory for heavy hadronic molecules
- Heavy Hadrons in Nuclear Matter
- Nuclear-bound quarkonia and heavy-flavor hadrons
- interaction from lattice QCD and its application to hypernuclei
- A model of charmed baryon-nucleon potential and 2- and 3-body bound states with charmed baryon
- Scattering of charmed baryons on nucleons
- interaction in chiral perturbation theory
- Search for doubly-heavy dibaryons in the quark-delocalization color-screening model
- Doubly charmed multibaryon systems
- Hadronic molecules with a meson in a medium
- Charmed baryonnucleon interaction
- Predictions for charmed nuclei based on forces inferred from lattice QCD simulations
- Single hypernuclei within quark mean-field model
- Charmed baryons in nuclear matter
- Hidden and open heavy-flavor hadronic states
- Nonmesonic weak decay of charmed hypernuclei
- Charmed hypernuclei within density-dependent relativistic mean-field theory
- Predicting possible molecular states of nucleons with , , and
- Pauli principle forbids bound states