Ce同位素的恒星s过程中子俘获截面

R. N. Sahoo, M. Paul, Y. Kashiv, M. Tessler, M. Friedman, S. Halfon, A. Kreisel, A. Shor, L. Weissman
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摘要

根据观测和理论模型,特别是中子--神奇的 $^{140}$Ce 同位素,铈的恒星丰度是当前人们高度关注的问题。在球状星团中观测到的铈丰度与$s-$过程恒星模型存在很大差异,这表明实验核反应速率可能存在不确定性。在这项工作中,测量了稳定铈同位素$^{136}$Ce、$^{138}$Ce、$^{140}$Ce和$^{142}$Ce的恒星中子俘获截面。利用$^{7}$Li($p,n$)反应,在$kT = 34.2$ keV条件下用准马克斯韦尔中子辐照了$^{nat}$Ce样品。在索雷克应用研究加速器设施(Soreq Applied Research Accelerator Facility,SARAF),用能量(1.92 MeV)略高于阈值的毫安质子束辐照液态锂靶(LiLiT),产生了强度为10^{10}$ n/s的3-5倍的中子场。使用屏蔽式高纯锗探测器测量了^{nat}$铈中子俘获产物的活度。提取了相对于$^{197}$Au(n,$\gamma$)反应的横截面,并得出了铈同位素的麦克斯韦平均横截面(MACS)。从该实验中提取的MACS值与之前的测量值基本一致,并显示$^{140}$Ce的MACS值比最近的实验值小大约15%。
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Stellar s-process neutron capture cross section of Ce isotopes
Stellar abundances of cerium are of high current interest based both on observations and theoretical models, especially with regard to the neutron--magic $^{140}$Ce isotope. A large discrepancy of $s-$process stellar models relative to cerium abundance observed in globular clusters was highlighted, pointing to possible uncertainties in experimental nuclear reaction rates. In this work, the stellar neutron capture cross section of the stable cerium isotopes $^{136}$Ce, $^{138}$Ce, $^{140}$Ce, and $^{142}$Ce, were re-measured. A $^{nat}$Ce sample was irradiated with quasi-Maxwellian neutrons at $kT = 34.2$ keV using the $^{7}$Li($p,n$) reaction. The neutron field with an intensity of $3-5 \times 10^{10}$ n/s was produced by irradiating the liquid-lithium target (LiLiT) with a mA proton beam at an energy (1.92 MeV) just above the threshold at Soreq Applied Research Accelerator Facility (SARAF). The activities of the $^{nat}$Ce neutron capture products were measured using a shielded High Purity Germanium detector. Cross sections were extracted relative to that of the $^{197}$Au(n,$\gamma$) reaction and the Maxwellian-averaged cross section (MACS) of the Ce isotopes were derived. The MACS values extracted from this experiment are generally consistent with previous measurements and show for $^{140}$Ce a value $\approx 15$\% smaller than most recent experimental values.
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