Mass, Spectroscopy, and Two-Neutron Decay of ^{16}Be.

B Monteagudo,F M Marqués, J Gibelin,N A Orr, A Corsi,Y Kubota, J Casal, J Gómez-Camacho, G Authelet, H Baba, C Caesar, D Calvet, A Delbart,M Dozono,J Feng,F Flavigny,J-M Gheller, A Giganon, A Gillibert, K Hasegawa, T Isobe, Y Kanaya, S Kawakami,D Kim, Y Kiyokawa,M Kobayashi,N Kobayashi,T Kobayashi, Y Kondo, Z Korkulu, S Koyama, V Lapoux, Y Maeda, T Motobayashi, T Miyazaki,T Nakamura, N Nakatsuka, Y Nishio, A Obertelli, A Ohkura, S Ota,H Otsu, T Ozaki, V Panin, S Paschalis,E C Pollacco, S Reichert,J-Y Rousse,A T Saito, S Sakaguchi, M Sako, C Santamaria, M Sasano,H Sato, M Shikata, Y Shimizu, Y Shindo, L Stuhl,T Sumikama,Y L Sun, M Tabata,Y Togano, J Tsubota, T Uesaka,Z H Yang, J Yasuda, K Yoneda, J Zenihiro

Physical review letters(2024)

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摘要
The structure and decay of the most neutron-rich beryllium isotope, ^{16}Be, has been investigated following proton knockout from a high-energy ^{17}B beam. Two relatively narrow resonances were observed for the first time, with energies of 0.84(3) and 2.15(5) MeV above the two-neutron decay threshold and widths of 0.32(8) and 0.95(15) MeV, respectively. These were assigned to be the ground (J^{π}=0^{+}) and first excited (2^{+}) state, with E_{x}=1.31(6)  MeV. The mass excess of ^{16}Be was thus deduced to be 56.93(13) MeV, some 0.5 MeV more bound than the only previous measurement. Both states were observed to decay by direct two-neutron emission. Calculations incorporating the evolution of the wave function during the decay as a genuine three-body process reproduced the principal characteristics of the neutron-neutron energy spectra for both levels, indicating that the ground state exhibits a strong spatially compact dineutron component, while the 2^{+} level presents a far more diffuse neutron-neutron distribution.
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