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arXiv 1407.0563nucl-ex
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在反射不对称区域边界处的Laser光谱学

Laser spectroscopy of francium isotopes at the borders of the region of reflection asymmetry

I. Budinčević, J. Billowes, M. L. Bissell, T. E. Cocolios, R. P. de Groote, S. De Schepper, V. N. Fedosseev, K. T. Flanagan, S. Franchoo, R. F. Garcia Ruiz, H. … 展开作者

I. Budinčević, J. Billowes, M. L. Bissell, T. E. Cocolios, R. P. de Groote, S. De Schepper, V. N. Fedosseev, K. T. Flanagan, S. Franchoo, R. F. Garcia Ruiz, H. Heylen, K. M. Lynch, B. A. Marsh, G. Neyens, T. J. Procter, R. E. Rossel, S. Rothe, I. Strashnov, H. H. Stroke, K. D. A. Wendt

摘要:

利用欧洲核子研究中心(CERN)ISOLDE新安装的共线共振电离光谱(CRIS)束线测量了富中子$^{218m,219,229,231}\text{Fr}$同位素的磁偶极矩和均方电荷半径的变化,探测了$7s~^{2}S_{1/2}$到$8p~^{2}P_{3/2}$的原子跃迁。$^{218m,219}\text{Fr}$和$^{229,231}\text{Fr}$的$δ\langle r^{2}\rangle^{A,221}$值遵循观察到的超过$N~=~126$的电荷半径的增加斜率。讨论了该丰中子区的电荷半径奇偶错列,表明$^{220}\text{Fr}$有弱的反奇偶错列,而$^{228}\text{Fr}$有正常的错列.这表明这两种同位素都位于一个反向交错区域的边界,这与反射不对称的形状有关。$g(^{219}\text{Fr}) = +0.69(1)$值支持基态的$π1h_{9/2}$壳模型配置。$g(^{229,231}\text{Fr})$值支持试探性的$I^π(^{229,231}\text{Fr}) = (1/2^{+})$自旋,并指向$πs_{1/2}^{-1}$入侵者基态配置。

英文摘要:

The magnetic dipole moments and changes in mean-square charge radii of the neutron-rich $^{218m,219,229,231}\text{Fr}$ isotopes were measured with the newly-installed Collinear Resonance Ionization Spectroscopy (CRIS) beam line at ISOLDE, CERN, probing the $7s~^{2}S_{1/2}$ to $8p~^{2}P_{3/2}$ atomic transition. The $δ\langle r^{2}\rangle^{A,221}$ values for $^{218m,219}\text{Fr}$ and $^{229,231}\text{Fr}$ follow the observed increasing slope of the charge radii beyond $N~=~126$. The charge radii odd-even staggering in this neutron-rich region is discussed, showing that $^{220}\text{Fr}$ has a weakly inverted odd-even staggering while $^{228}\text{Fr}$ has normal staggering. This suggests that both isotopes reside at the borders of a region of inverted staggering, which has been associated with reflection-asymmetric shapes. The $g(^{219}\text{Fr}) = +0.69(1)$ value supports a $π1h_{9/2}$ shell model configuration for the ground state. The $g(^{229,231}\text{Fr})$ values support the tentative $I^π(^{229,231}\text{Fr}) = (1/2^{+})$ spin, and point to a $πs_{1/2}^{-1}$ intruder ground state configuration.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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