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N=8 Shell Breaking in Be12 from a Single-Particle Perspective

J. Chen1,2,*, B. P. Kay2, D. K. Sharp3, L. P. Gaffney4, S. J. Freeman3,5, S. M. Wang6,7, J. G. Li8,9,10, P. T. MacGregor3,5, C. R. Hoffman2 et al. (ISOLDE Collaboration)

C. R. Hoffman2, Y. Ayyad11, P. A. Butler4, S. Carollo12,13, A. Ceulemans14, D. J. Clarke3, A. J. Dolan4, C. Everett4, Z. Favier5, K. Garrett3, J. Geng15, H. Jayatissa2, M. Labiche16, I. Lazarus16, W. P. Liu1, Y. F. Niu15, B. Olaizola5,17, J. Ojala4, C. A. A. Page18,5, R. D. Page4, O. Poleshchuk14, R. Raabe14, M. R. Xie8,9, C. X. Yuan19, Z. Yue18,5, and Y. N. Zhang19 (ISOLDE Collaboration)

  • *Contact author: chenjie@sustech.edu.cn

Phys. Rev. Lett. 136, 222501 – Published 2 June, 2026

DOI: https://doi.org/10.1103/3vts-dwst

Abstract

Experimental observations of the low-lying states in Be12 and their accurate modeling play an essential role in understanding the disappearance of the N=8 magic number. Long-standing experimental ambiguities have been clarified using an one-neutron adding (d, p) reaction on Be11 using the ISOLDE Solenoidal Spectrometer at CERN’s HIE-ISOLDE facility. The single-particle energies of 1s1/2, 0d5/2, and 0p1/2 orbitals in Be12 have been determined from the extracted spectroscopic factors. A significant reduction between the separation of 1s1/2 and 0p1/2 orbitals is found in comparison with the carbon isotones, highlighting the breakdown of the N=8 shell. These observations serve as an important test of different effects incorporated in theoretical models. It is found that two synergistic mechanisms, core deformation and weak binding, are responsible for the N=8 shell breaking and the exotic near-threshold phenomena observed in Be12, including the narrow unnatural-parity resonance 01− and the possible halolike nature of the 02+ isomer.

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