1970
DOI: 10.1016/0550-3213(70)90351-2
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The non-mesonic decay of helium hypernuclei

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Cited by 24 publications
(6 citation statements)
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“…A more conclusive proof for this suggestion would come from the observation of back-to-back Λ 3 He pairs in the two-body decay 4 Σ He → Λ+ 3 He. The branching ratio for this decay relative to the inclusive ΛX decay rate is perhaps a few percent, as may be argued by analogy with the approximately 8%(5%) branching ratio measured for the nonmesonic decay 4 Λ He( 5 Λ He) → n+ 3 He( 4 He) relative to the inclusive π − decay rate of 4 Λ He( 5 Λ He) [63,64]. Irrespective of whether or not the above conjecture of 4 Σ He production is correct for the FOPI-Detector GSI experiments, it would be a wise practice forK-nuclear bound state searches in heavy ion collisions to look first for known hypernuclear signals in order to determine their production rates as calibration and normalization standards.…”
Section: 1k-nuclear Bound States?supporting
confidence: 58%
“…A more conclusive proof for this suggestion would come from the observation of back-to-back Λ 3 He pairs in the two-body decay 4 Σ He → Λ+ 3 He. The branching ratio for this decay relative to the inclusive ΛX decay rate is perhaps a few percent, as may be argued by analogy with the approximately 8%(5%) branching ratio measured for the nonmesonic decay 4 Λ He( 5 Λ He) → n+ 3 He( 4 He) relative to the inclusive π − decay rate of 4 Λ He( 5 Λ He) [63,64]. Irrespective of whether or not the above conjecture of 4 Σ He production is correct for the FOPI-Detector GSI experiments, it would be a wise practice forK-nuclear bound state searches in heavy ion collisions to look first for known hypernuclear signals in order to determine their production rates as calibration and normalization standards.…”
Section: 1k-nuclear Bound States?supporting
confidence: 58%
“…The existing observations of two-body NMWD of Hypernuclei are very scarce and date back to bubble chamber [169] ≤ 0.24 4 Λ He, n and p spectra KEK-E508 [25] 0.27 ± 0.13 0.29 ± 0.13 12 Λ C, nn and np spectra FINUDA [26] 0.24±0.10 A =5-16, p spectra FINUDA [27] 0.21 ± 0.07stat +0.03 −0.02 sys A =5-16, np spectra and emulsion experiments [248][249][250]; in particular, reaction (67) has not yet been observed. The only existing calculation for the 4 Λ He two-body NMWD rates was performed long ago by Ref.…”
Section: Rare Two-body Nmwd Of S-shell Hypernucleimentioning
confidence: 99%
“…Coremans et al [30], by combining emulsion data on helium hypernuclei with the bubble chamber result for 4 Λ He, were able to determine Q − for 5 Λ He but only after making a large correction for the undetectable decay mode 3 He + n + n. Values for Q − for Λ Be and 11 Λ B were given by Montwill et al [20] whereas a ballpark number was given for heavy spallation hypernuclei by Lagnaux et al [31]. These results are summarised in Table 3.…”
Section: Non-mesonic Decaysmentioning
confidence: 98%
“…Moreover, the emulsion experiment, despite its limited statistics, does have the advantage that the protons in the spectrum are seen to come from hypernuclear decays. It should also be remarked that a considerable number, certainly in excess of 10%, of the so-called protons are in fact deuterons and tritons [30,36] Coremans et al [30] studied the non-mesonic decays of 5 Λ He and found the following partial decay rates with respect to the π − -mesonic rate for those decays which involve at most one neutron and these are presented in Table 4.…”
Section: Non-mesonic Decaysmentioning
confidence: 98%