Coincidence Measurement of the Nonmesonic Weak Decay of ^{12}_{Lambda}C

Phys.Lett. B641 (2006) 28-33 We have measured the angular correlation of the pair nucleons np and nn emitted from the nonmesonic weak decay (NMWD) of ^{12}_{Lambda}C produced via the (pi^+,K^+) reaction in coincidence measurement. The Lambda p -> np and Lambda n -> nn modes were clearly identi...

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Main Authors Kim, M. J, Ajimura, S, Aoki, K, Banu, A, Bhang, H, Fukuda, T, Hashimoto, O, Hwang, J. I, Kameoka, S, Kang, B. H, Kim, E. H, Kim, J. H, Maruta, T, Miura, Y, Miyake, Y, Nagae, T, Nakamura, M, Nakamura, S. N, Noumi, H, Okada, S, Okayasu, Y, Outa, H, Park, H, Saha, P. K, Sato, Y, Sekimoto, M, Shin, S, Takahashi, T, Tamura, H, Tanida, K, Toyoda, A, Tsukada, K, Watanabe, T, Yim, H. J
Format Journal Article
LanguageEnglish
Published 21.01.2006
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Summary:Phys.Lett. B641 (2006) 28-33 We have measured the angular correlation of the pair nucleons np and nn emitted from the nonmesonic weak decay (NMWD) of ^{12}_{Lambda}C produced via the (pi^+,K^+) reaction in coincidence measurement. The Lambda p -> np and Lambda n -> nn modes were clearly identified by measuring the back-to-back correlation of the emitted nucleon pairs which is the characteristic of two-body kinematics. From the measured nucleon pair numbers N_{nn} and N_{np}, the ratio Gamma_n/Gamma_p of the partial decay widths Gamma_n(Lambda n -> nn) and Gamma_p(Lambda p -> np) of ^{12}_{Lambda}C was extracted to be 0.51+-0.13(stat) +- 0.05(syst); this result is almost free from the ambiguity due to the nuclear final state interaction and 3-body decay process, which were inherent in the previous results. The obtained Gamma_n/Gamma_p ratio of ^{12}_{Lambda}C (p-shell) is close to that of ^5_{Lambda}He (s-shell). The results are consistent with those of recent theoretical calculations.
DOI:10.48550/arxiv.nucl-ex/0601029