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arXiv 1202.4873physics.atom-phnucl-th
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$^{12}$ Be的核电荷半径

Nuclear Charge Radius of $^{12}$Be

Andreas Krieger, Klaus Blaum, Mark L. Bissell, Nadja Frömmgen, Christopher Geppert, Michael Hammen, Kim Kreim, Magdalena Kowalska, Jörg Krämer, Thomas Neff, Rai… 展开作者

Andreas Krieger, Klaus Blaum, Mark L. Bissell, Nadja Frömmgen, Christopher Geppert, Michael Hammen, Kim Kreim, Magdalena Kowalska, Jörg Krämer, Thomas Neff, Rainer Neugart, Gerda Neyens, Wilfried Nörtershäuser, Christian Novotny, Rodolfo Sanchez, Deyan T. Yordanov

摘要:

利用共线激光光谱技术对Be离子$^{+}$中的$2s_{1/2}\rightarrow 2p_{1/2, 3/2}$跃迁进行了精确测定。与单中子晕同位素$^{11}$ Be的$δ<r_{\rm c}^2>^{10,11} = 0.49(5) \fm^{2}$相比,从$^{10}$ Be到$^{12}$ Be的均方电荷半径增加了$δ<r_{\rm c}^2>^{10,12} = 0.69(5) \fm^{2}$。费米分子动力学方法的计算表明,$^{12}$ Be的结构对电荷半径有很强的敏感性。实验电荷半径与N=8壳层闭合的破裂一致。

英文摘要:

The nuclear charge radius of $^{12}$Be was precisely determined using the technique of collinear laser spectroscopy on the $2s_{1/2}\rightarrow 2p_{1/2, 3/2}$ transition in the Be$^{+}$ ion. The mean square charge radius increases from $^{10}$Be to $^{12}$Be by $δ<r_{\rm c}^2>^{10,12} = 0.69(5) \fm^{2}$ compared to $δ<r_{\rm c}^2>^{10,11} = 0.49(5) \fm^{2}$ for the one-neutron halo isotope $^{11}$Be. Calculations in the fermionic molecular dynamics approach show a strong sensitivity of the charge radius to the structure of $^{12}$Be. The experimental charge radius is consistent with a breakdown of the N=8 shell closure.

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