Monteagudo B, Marqués F M, Gibelin J, Orr N A, Corsi A, Kubota Y, Casal J, Gómez-Camacho J, Authelet G, Baba H, Caesar C, Calvet D, Delbart A, Dozono M, Feng J, Flavigny F, Gheller J-M, Giganon A, Gillibert A, Hasegawa K, Isobe T, Kanaya Y, Kawakami S, Kim D, Kiyokawa Y, Kobayashi M, Kobayashi N, Kobayashi T, Kondo Y, Korkulu Z, Koyama S, Lapoux V, Maeda Y, Motobayashi T, Miyazaki T, Nakamura T, Nakatsuka N, Nishio Y, Obertelli A, Ohkura A, Ota S, Otsu H, Ozaki T, Panin V, Paschalis S, Pollacco E C, Reichert S, Rousse J-Y, Saito A T, Sakaguchi S, Sako M, Santamaria C, Sasano M, Sato H, Shikata M, Shimizu Y, Shindo Y, Stuhl L, Sumikama T, Sun Y L, Tabata M, Togano Y, Tsubota J, Uesaka T, Yang Z H, Yasuda J, Yoneda K, Zenihiro J
LPC Caen, ENSICAEN, CNRS/IN2P3, Université de Caen, Normandie Université, 14050 Caen, France.
FRIB, Michigan State University, East Lansing, Michigan 48824, USA.
Phys Rev Lett. 2024 Feb 23;132(8):082501. doi: 10.1103/PhysRevLett.132.082501.
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.
通过从高能(^{17}B)束流中敲除质子,对中子数最多的铍同位素(^{16}Be)的结构和衰变进行了研究。首次观测到两个相对较窄的共振峰,其能量分别比双中子衰变阈值高(0.84(3))和(2.15(5))兆电子伏,宽度分别为(0.32(8))和(0.95(15))兆电子伏。这些共振峰被确定为基态((J^{\pi}=0^{+}))和第一激发态((2^{+})),激发能(E_{x}=1.31(6))兆电子伏。由此推导出(^{16}Be)的质量过剩为(56.93(13))兆电子伏,比之前唯一一次测量结果的束缚能约高(0.5)兆电子伏。观测到这两个态均通过直接双中子发射衰变。将衰变过程中波函数的演化作为一个真正的三体过程进行的计算,再现了两个能级的中子 - 中子能谱的主要特征,表明基态呈现出很强的空间紧凑双中子成分,而(2^{+})能级的中子 - 中子分布则更为弥散。