First observation of a nuclear s-state of a Ξ\Xi hypernucleus, Ξ15C^{15}_{\Xi}{\rm C}

Mar 15, 2021
26 pages
Published in:
  • PTEP 2021 (2021) 7, 7
  • Published: Jul 18, 2021
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Abstract: (Oxford University Press)
Bound systems of |Ξ\Xi^-|–|14N^{14}_{}{\rm N}| are studied via |Ξ\Xi^-| capture at rest followed by emission of a twin single-|Λ\Lambda| hypernucleus in the emulsion detectors. Two events forming extremely deep |Ξ\Xi^-| bound states were obtained by analysis of a hybrid method in the E07 experiment at J-PARC and reanalysis of the E373 experiment at KEK-PS. The decay mode of one event was assigned as |Ξ+14 ⁣ ⁣ ⁣NΛ5 ⁣ ⁣ ⁣He+Λ5 ⁣ ⁣He+4 ⁣ ⁣He+n\Xi^-+^{14}\!\,\!\!{\rm N}\to^{5}_{\Lambda}\!\!\!{\rm He} + ^{5}_{\Lambda}\!\!{\rm He} + ^{4}\!\!{\rm He} + \mathrm{n}|⁠. Since there are no excited states for daughter particles, the binding energy of the |Ξ\Xi^-| hyperon, |BΞB_{\Xi^-}|⁠, in the |14N^{14}_{}{\rm N}| nucleus was uniquely determined to be |6.27±0.276.27 \pm 0.27| MeV. Another |Ξ\Xi^-|–|14N^{14}_{}{\rm N}| system via the decay |Λ9Be+Λ5 ⁣ ⁣ ⁣He+n^{9}_{\Lambda}{\rm Be} + ^{5}_{\Lambda}\!\!\!{\rm He} + \mathrm{n}| brings a |BΞB_{\Xi^-}| value, |8.00±0.778.00 \pm 0.77| MeV or |4.96±0.774.96 \pm 0.77| MeV, where the two possible values of |BΞB_{\Xi^-}| correspond to the ground and the excited states of the daughter |Λ9Be^{9}_{\Lambda}{\rm Be}| nucleus, respectively. Because the |BΞB_{\Xi^-}| values are larger than those of the previously reported events (KISO and IBUKI), which are both interpreted as the nuclear |1p1p| state of the |Ξ\Xi^-|–|14N^{14}_{}{\rm N}| system, these new events give the first indication of the nuclear |1s1s| state of the |Ξ\Xi| hypernucleus, |Ξ15C^{15}_{\Xi}{\rm C}|⁠.
Note:
  • 26 pages, 7 figures
  • D14 Hypernuclei
  • D25 Hadron reactions
  • D29 Nuclear decays and radioactivities (including fission)
  • capture
  • nucleus
  • hypernucleus
  • excited state
  • nuclear emulsion
  • binding energy
  • decay modes