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Shell model calculations have been carried out for 90Nb nucleus with the model space in which the valence protons occupy the f5/2, p3/2, p1/2, and g9/2 orbitals and the valence neutrons occupy the p1/2, g9/2, d5/2, and g7/2 orbitals. According to the calculated results, the negative parity is from the contribution of the proton of the f5/2, p3/2, and p1/2 orbits. The moderate spin states of 90Nb are mainly due to the excitation of protons from the f5/2 and p3/2 orbits to the p1/2 and g9/2 orbits across the Z = 38 subshell closure, and the high spin states arise from the excitation of a single neutron from the g9/2 orbit into the d5/2 orbit across the N = 50 shell closure.
Słowa kluczowe
Czasopismo
Rocznik
Tom
Strony
113--116
Opis fizyczny
Bibliogr. 15 poz., rys.
Twórcy
autor
- School of Physics and Electronic Engineering of An Qing Normal University No. 1318, Jixian North Road, Anqing city Anhui, 246133, P. R. China
autor
- College of Physics of Jilin University No. 2699 Qianjin Street, Changchun city Jilin, 130012, P. R. China
autor
- College of Physics of Jilin University No. 2699 Qianjin Street, Changchun city Jilin, 130012, P. R. China
autor
- School of Physics of Sun Yat-sen University No. 135, Xingang Xi Road, Guangzhou city Gungdong, 510275, P. R. China
Bibliografia
- 1. Pattabiraman, N. S., Chintalapudi, S. N., Ghugre, S. S., Tirumala Rao, B. V., Raju, M. L. N., Seshi Reddy, T., Joshi, P. K., Palit, R., & Jain, H. C. (2002). Level structure of 92 Mo at high angular momentum: Evidence for Z=38, N=50 core excitation. Phys. Rev. C, 65, 044324. https://doi.org/10.1103/Phys-RevC.65.044324.
- 2. Rainovski, G., Schwengner, R., Schilling, K. D., Wagner, A., Jungclaus, A., Galindo, E., Thelen, O., Napoli, D. R., Ur, C. A., de Angelis, G., Axiotis, M., Gadea, A., Marginean, N., Martinez, T., & Kröll, Th. (2002). High-spin structure of the spherical nucleus 90Y. Phys. Rev. C, 65, 044327. https://doi.org/10.1103/PhysRevC.65.044327.
- 3. Roth, H. A., Arnell, S. E., Foltescu, D., Skeppstedt, Ö., Blomqvist, J., Nilsson, A., Kuroyanagi, T., Mitarai, S., & Nyberg, J. (1994). Gaps in the yrast level structure of the N=50 isotones 93Tc, 94Ru, and 95Rh at high angular momentum. Phys. Rev. C, 50(3), 1330.https://doi.org/10.1103/PhysRevC.50.1330.
- 4. Stefanova, E. A., Schwengner, R., Rainovski, G., Schilling, K. D., Wagner, A., Dönau, F., Galindo, E., Jungclaus, A., Lieb, K. P., Thelen, O., Eberth, J., Napoli, D. R., Ur, C. A., de Angelis, G., Axiotis, M., Gadea, A., Marginean, N., Martinez, T., Kröll, Th., & Kutsarova, T. (2001). Structure of high-spin states in 89Sr and 90Sr. Phys. Rev. C, 63, 064315. https://doi.org/10.1103/PhysRevC.63.064315.
- 5. Ghugre, S. S., Naguleswaran, S., Bhowmik, R. K., Garg, U., Patel, S. B., Reviol, W., & Walpe, J. C. (1995). High-spin states in 94Tc and the shell-model interpretation. Phys. Rev. C, 51, 2809. https://doi.org/10.1103/PhysRevC.51.2809.
- 6. Wu, Yi-Heng., Lu, Jing-Bin., Luo, Peng-Wei., Li, Guang-Sheng., Li, Hong-Wei., Wu, Xiao-Guang., He, Chuang-Ye., Zheng, Yun., Ma, Ke-Yan., Yang, Dong., Li, Cong-Bo., Hu, Shi-Peng., Liu, Jia-Jian., Wang, Jin-Long., Yao, Shun-He., Chen, Qi-Ming., & Zhong, Jian. (2014). High-spin states in the odd-odd nucleus 92Nb. Chin. Phys. Lett., 31(4), 042101. https://doi.org/10.1088/0256-307X/31/4/042102.
- 7. Luo, P. W., Wu, X. G., Sun, H. B., Li, G. S., He, C. Y., Zheng, Y., Li, C. B., Hu, S. P., Wu, Y. H., Li, H. W.,Liu, J. J., Wang, J. L., Yao, S. H., & Edwards, S. A.(2014). High-spin level structure of the semi-magic nucleus 91Nb. Phys. Rev. C, 89(3), 034318. https://doi.org/10.1103/PhysRevC.89.034318.
- 8. Arnell, S. E., Foltescu, D., Roth, H. A., Skeppstedt,Ö., Blomqvist, J., Nilsson, A., Kuroyanagi, T., Mitarai, S., & Nyberg, J. (1994). Yrast level structure of the neutron defi cient N=49 isotones 92Tc, 93Ru, 94Rh, and 95Pd up to high angular momentum. Phys. Rev. C, 49(1), 51. https://doi.org/10.1103/PhysRevC.49.51.
- 9. Zhao, Guang-yi., Li, Guang-sheng., Wu, Xiao-guang., Liu, Xiang-an., Wen, Shu-xian., Lu, Jing-bin., Yuan, Guan-jun., & Yang, Chun-xiang. (1999). Structure of high spin states in 87Zr. Chin. Phys. Lett.,16(5), 345.
- 10. He, Chuang-Ye., Cui, Xing-Zhu., Zhu, Li-Hua., Wu, Xiao-Guang., Li, Guang-Sheng., Liu, Ying., Wang, Zhi-Min., Wen, Shu-Xian., Sun, Hui-Bin., Ma, Rui-Gang., & Yang, Chun-Xiang. (2010). Shell structures in 91Nb. Chin. Phys. Lett., 27, 102104. https://doi.org/10.1088/0256-307X/27/10/102104.
- 11. Ray, S., Pattabiraman, N. S., Goswami, R., Ghugre, S. S., Sinha, A. K., & Garg, U. (2004). Experimental study of nuclear structure of 91Mo at high spin. Phys. Rev. C, 69(5), 054314. https://doi.org/10.1103/Phys-RevC.69.054314.
- 12. Cui, X. Z., Zhu, L. H., Wu, X. G., Wang, Z. M., He,C. Y., Liu, Y., Li, G. S., Wen, S. X., Zhang, Z. L., Meng, R., Ma, R. G., Luo, P., Zheng, Y., Ndontchueng, M. M., Huo, J. D., & Yang, C. X. (2005). High-spin states and shell structure of the odd-odd nucleus 90Nb.Phys. Rev. C, 72(4), 044322. https://doi.org/10.1103/PhysRevC.72.044322.
- 13. Brown, B. A., & Rae, W. D. M. (2007). NuShell@MSU. MSU-NSCL Report (unpublished). Michigan State University, National Superconducting Cyclotron Laboratory.
- 14. Chang-hua, Zhang., Shun-jin, Wang., & Jin-nan, Gu. (1999). Shell model studies of nuclei with A=92–98.Phys. Rev. C, 60(5), 054316. https://doi.org/10.1103/PhysRevC.60.054316.
- 15. Ghugre, S. S., & Datta, S. K. (1995). Shell model study of the high spin states in the N=50 isotones 92Mo, 93Tc, 94Ru, and 95Rh. Phys. Rev. C, 52(4), 1881. https://doi.org/10.1103/PhysRevC.52.1881
Uwagi
Opracowanie rekordu w ramach umowy 509/P-DUN/2018 ze środków MNiSW przeznaczonych na działalność upowszechniającą naukę (2019).
Typ dokumentu
Bibliografia
Identyfikator YADDA
bwmeta1.element.baztech-15ca4a4f-8791-4658-a02a-8ea9ccca3db1