Hypernuclei
arXiv:nucl-th/0407007 · doi:10.1016/j.physletb.2005.01.001
Abstract
We present results for the selfenergy of the pentaquark in nuclei associated with two sources: the decay of the and the two meson baryon decay channels of the partners in an antidecuplet of baryons. The first source is shown to produce a small potential, unable to bind the in nuclei, while the second source gives rise to a large attractive potential. At the same time we show that the width of the in nuclei is small, such that, in light and medium nuclei, many bound states would appear with a separation between levels appreciably larger than the width of the states, thus creating an ideal scenario for pentaquark spectroscopy in nuclei.
16 pages, 8 figures
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Cited by in corpus (11)
- Generalized mass formula for non-strange and hyper nuclei with SU(6) symmetry breaking
- The effect of the in-medium pentaquark on the kaon optical potential
- Pentaquark in nuclear matter and hypernuclei
- Two-meson cloud contribution to the baryon antidecuplet binding
- Strange and Heavy Flavoured Hypernuclei in Chiral Soliton Models
- Phenomenological study of two-meson couplings of Theta+
- Strange Exotic States and Compact Stars
- Production of Hypernuclei with the reaction
- In-medium Properties of as a KN structure in Relativistic Mean Field Theory
- Antikaon angular distributions in the reaction near the threshold and the parity of the pentaquark
- Pentaquarks in the medium in the quark-meson coupling model