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Abstract:
The structures of N=7 and N=8 isotones in Be-F mass range are investigated in the framework of the single-particle shell model. Different from the traditional potential terms, the l2 coupling is included in the average nuclear potential. Calculations give a unified description for the structures of all studied nuclei. The neutron s-p level inversion in 11Be and proton s-d level inversion in 16F are simultaneously reproduced. In addition, the neutron halo structures in 11Be(2s1/2) and 11Be(1p1/2) are obtained. The proton halo in the first-excited state of 17F is also discussed.
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References
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[1]
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. Talmi I, Unna I. Phys. Rev. Lett., 1960, 4: 4692. Fortune H T. Phys. Rev. C, 1995, 52: 22613. LIU Z H, BAO J D. Chin. Phys. Lett., 2004, 21: 4574. Tanihata I et al. Nucl. Phys. A, 1995, 583: 7695. CHEN B Q, MA Z Y. Chin. Phys. Lett., 2001, 18: 15616. PEI J C, XU F R, Stevenson P D. Nucl. Phys. A, 2006,765: 297. GUO Y Q, REN Z Z. HEP NP, 2007, 31: 3618. Descouvemont P. Nucl. Phys. A, 1997, 615: 2619. REN Z Z et al. Z. Phys. A, 1997, 357: 13710. Bohr A, Mottelson B R. Nuclear Structure (Vol. I). Sin-gapore: World Scienti c Publishing Co. Pte. Ltd., 1998.144-149, 235-24011. CHENG Tan-Sheng, ZHONG Yu-Shu. Nuclear physics oflow and medium energy. Beijing: Press of Beijing Univer-sity, 1997. 313 12. Audi G et al. Nucl. Phys. A, 2003, 729: 313. Audi G, Wapstra A H, Thibault C. Nucl. Phys. A, 2003,729: 33714. Morlock R et al. Phys. Rev. Lett., 1997, 79: 383715. REN Z Z, Amand Faessler, Bobyk A. Phys. Rev. C, 1998,57: 275216. Ajzenberg-Selove F. Nucl. Phys. A, 1990, 506: 1; Nucl.Phys. A, 1991, 523: 1 |
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