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Nuclear charge radius of $^{12}$Be

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 $\delta <r_{\rm c}^2>^{10,12} =...

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Detalles Bibliográficos
Autores principales: Krieger, A., Blaum, K., Bissell, M.L., Frommgen, N., Geppert, Ch., Hammen, M., Kreim, K., Kowalska, M., Kramer, J., Neff, T., Neugart, R., Neyens, G., Nortershauser, W., Novotny, Ch., Sanchez, R., Yordanov, D.T.
Lenguaje:eng
Publicado: 2012
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevLett.108.142501
http://cds.cern.ch/record/1426421
Descripción
Sumario: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 $\delta <r_{\rm c}^2>^{10,12} = 0.69(5)$ fm$^{2}$ compared to $\delta <r_{\rm c}^2>^{10,11} = 0.49(5)$ 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.