Precision Analysis of the ^{136}Xe Two-Neutrino ββ Spectrum in KamLAND-Zen and Its Impact on the Quenching of Nuclear Matrix Elements.

A Gando,Y Gando,T Hachiya, M Ha Minh, S Hayashida, Y Honda, K Hosokawa, H Ikeda,K Inoue, K Ishidoshiro,Y Kamei, K Kamizawa, T Kinoshita,M Koga,S Matsuda,T Mitsui, K Nakamura,A Ono, N Ota,S Otsuka,H Ozaki, Y Shibukawa,I Shimizu, Y Shirahata,J Shirai, T Sato,K Soma, A Suzuki, A Takeuchi,K Tamae, K Ueshima, H Watanabe, D Chernyak,A Kozlov,S Obara, S Yoshida,Y Takemoto, S Umehara,K Fushimi,S Hirata, B E Berger, B K Fujikawa,J G Learned,J Maricic, L A Winslow, Y Efremenko,H J Karwowski,D M Markoff, W Tornow,T O'Donnell,J A Detwiler, S Enomoto, M P Decowski, J Menéndez, R Dvornický,F Šimkovic

Physical review letters(2019)

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摘要
We present a precision analysis of the ^{136}Xe two-neutrino ββ electron spectrum above 0.8 MeV, based on high-statistics data obtained with the KamLAND-Zen experiment. An improved formalism for the two-neutrino ββ rate allows us to measure the ratio of the leading and subleading 2νββ nuclear matrix elements (NMEs), ξ_{31}^{2ν}=-0.26_{-0.25}^{+0.31}. Theoretical predictions from the nuclear shell model and the majority of the quasiparticle random-phase approximation (QRPA) calculations are consistent with the experimental limit. However, part of the ξ_{31}^{2ν} range allowed by the QRPA is excluded by the present measurement at the 90% confidence level. Our analysis reveals that predicted ξ_{31}^{2ν} values are sensitive to the quenching of NMEs and the competing contributions from low- and high-energy states in the intermediate nucleus. Because these aspects are also at play in neutrinoless ββ decay, ξ_{31}^{2ν} provides new insights toward reliable neutrinoless ββ NMEs.
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