Single-Neutron Adding on $^{34}$S

A. N. Kuchera, C. R. Hoffman, G. Ryan, I. B. D'Amato, O. M. Guarinello, P. S. Kielb, R. Aggarwal, S. Ajayi, A. L. Conley, I. Conroy, P. D. Cottle, J. C. Esparza, S. Genty, K. Hanselman, M. Heinze, D. Houlihan, B. Kelly, M. I. Khawaja, E. Lopez-Saavedra, G. W. McCann, A. B. Morelock, L. A. Riley, A. Sandrik, V. Sitaraman, M. Spieker, C. Wibisono, I. Wiedenhover
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Abstract

Purpose: Single-neutron adding data was collected in order to determine the distribution of the single-neutron strength of the $0f_{7/2}$, $1p_{3/2}$, $1p_{1/2}$ and $0f_{5/2}$ orbitals outside of $Z=16, N=18$, $^{34}$S. Methods: The $^{34}$S($d$,$p$)$^{35}$S reaction has been measured at 8 MeV/u to investigate cross sections to excited states in $^{35}$S. Outgoing proton yields and momenta were analyzed by the Super-Enge Split-Pole Spectrograph in conjunction with the CeBrA demonstrator located at the John D. Fox Laboratory at Florida State University. Angular distributions were compared with Distorted Wave Born Approximation calculations in order to extract single-neutron spectroscopic overlaps. Results: Spectroscopic overlaps and strengths were determined for states in $^{35}$S up through 6~MeV in excitation energy. Each orbital was observed to have fragmented strength where a single level carried the majority. The single-neutron centroids of the $0f_{7/2}$, $1p_{3/2}$, $1p_{1/2}$ and $0f_{5/2}$ orbitals were determined to be $2360^{+90}_{-40}$~keV, $3280^{+80}_{-50}$~keV, $4780^{+60}_{-40}$~keV, and $\gtrsim7500$~keV, respectively. Conclusion: A previous discrepancy in the literature with respect to distribution of the neutron $1p_{1/2}$ strength was resolved. The integration of the normalized spectroscopic strengths, up to 5.1~MeV in excitation energy, revealed fully-vacant occupancies for the $0f_{7/2}$, $1p_{3/2}$, and $1p_{1/2}$ orbitals, as expected. The spacing in the single-neutron energies highlighted a reduction in the traditional $N=28$ shell-gap, relative to both the $1p$ spin-orbit energy difference ($N=32$) and the lower limit on the $N=34$ shell spacing.
^{34}$S上的单中子加法
目的:收集单中子添加数据,以确定 $0f_{7/2}$、$1p_{3/2}$、$1p_{1/2}$ 和 $0f_{5/2}$ 轨道在 $Z=16、N=18$、$^{34}$S 以外的单中子强度分布。方法:在 8 MeV/uto 下测量了 $^{34}$S($d$,$p$)$^{35}$S 反应,研究了 $^{35}$S 激发态的截面。利用位于佛罗里达州立大学约翰-D-福克斯实验室的超级-恩格分极摄谱仪和 CeBrA 演示器分析了出射质子量和质子矩。将角度分布与扭曲波博恩近似计算进行了比较,以提取单中子谱重叠。结果:测定了激发能量高达 6~MeV 的 $^{35}$S 状态的光谱重叠和强度。观察到每个轨道都有碎裂强度,其中单级占大多数。测定的 $0f_{7/2}$、$1p_{3/2}$、$1p_{1/2}$ 和 $0f_{5/2}$ 轨道的单中子中心分别为 $2360^{+90}_{-40}$~keV、$3280^{+80}_{-50}$~keV、$4780^{+60}_{-40}$~keV 和 $\gtrsim7500$~keV。结论解决了以前文献中关于中子1p_{1/2}$强度分布的差异问题。对激发能量高达 5.1~MeV 的归一化光谱强度的积分显示,0f_{7/2}$、1p_{3/2}$ 和 1p_{1/2}$ 轨道完全空位。单中子能量间距显示,相对于 1p 自旋轨道能量差(N=32)和 N=34 的壳间距下限,传统的 N=28 的壳间隙有所减小。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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