Neutron–proton coincidences from Non-Mesonic Weak Decay of p-shell Λ-hypernuclei and determination of the two-nucleon induced process
FP7
Nuclear and High Energy Physics
EC
Λ-hypernuclei
530
Research Infrastructures
01 natural sciences
Two nucleon induced decay
Λ-hypernuclei; Non-mesonic weak decay; Two nucleon induced decay
0103 physical sciences
Non-mesonic weak decay
Λ-hypernuclei, Non-mesonic weak decay, Two nucleon induced decay
European Commission
Lambda-hypernuclei; Non-mesonic weak decay; Two nucleon induced decay
SP4-Capacities
Hypernuclear physics; weak decays
DOI:
10.1016/j.physletb.2011.06.035
Publication Date:
2011-06-24T17:58:49Z
AUTHORS (39)
ABSTRACT
AbstractThe decay of Λ-hypernuclei without π emission, known as Non-Mesonic Weak Decay (NMWD), gives an effective tool to investigate ΔS=1 four-baryon interactions. It was theoretically suggested that the two-nucleon induced mechanism could play a substantial role in reproducing the observed NMWD decay rates and nucleon spectra, but at present no direct evidence of such a mechanism has been obtained. The FINUDA experiment, exploiting the possibility to detect both charged and neutral particles coming from the hypernucleus decay, has allowed us to deduce the relative weight of the two nucleon induced decay rate to the total NMWD rate. The value of Γ2N/ΓNMWD=0.21±0.07stat−0.02sys+0.03sys has been deduced, well consistent with the previous determinations.
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