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arXiv 1408.5985nucl-exnucl-th
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$^{89,90}$ Y中的壳体间隙降低水平密度

Shell-gap reduced level densities in $^{89,90}$Y

M. Guttormsen, A. C. Larsen, F. L. Bello Garrote, Y. Byun, T. K. Eriksen, F. Giacoppo, A. Görgen, T. W. Hagen, M. Klintefjord, H. T. Nyhus, T. Renstrøm, S. J. R… 展开作者

M. Guttormsen, A. C. Larsen, F. L. Bello Garrote, Y. Byun, T. K. Eriksen, F. Giacoppo, A. Görgen, T. W. Hagen, M. Klintefjord, H. T. Nyhus, T. Renstrøm, S. J. Rose, E. Sahin, S. Siem, T. Tornyi, G. M. Tveten, A. Voinov

摘要:

利用来自$^{89}$ Y($p,p' γ$)$^{89}$ Y和$^{89}$ Y($d,p γ$)$^{90}$ Y反应的粒子- $γ$符合来获得作为激发能的函数的$γ$ -射线光谱.利用奥斯陆方法从粒子- $γ$符合矩阵中提取能级密度。的$N=50$壳封闭的能级密度的影响进行了讨论的组合准粒子模型的框架内。

英文摘要:

Particle-$γ$ coincidences from the $^{89}$Y($p,p' γ$)$^{89}$Y and $^{89}$Y($d,p γ$)$^{90}$Y reactions were utilized to obtain $γ$-ray spectra as function of excitation energy. The Oslo method was used to extract the level density from the particle-$γ$ coincidence matrices. The impact of the $N=50$ shell closure on the level densities is discussed within the framework of a combinatorial quasi-particle model.

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