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arXiv 1702.03352astro-ph.SRnucl-ex
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用AMS测量恒星$^{58}$ Ni $(n,γ)^{59}$ Ni截面

Measurement of the stellar $^{58}$Ni$(n,γ)^{59}$Ni cross section with AMS

Peter Ludwig, Georg Rugel, Iris Dillmann, Thomas Faestermann, Leticia Fimiani, Karin Hain, Gunther Korschinek, Johannes Lachner, Mikhail Poutivtsev, Klaus Knie,… 展开作者

Peter Ludwig, Georg Rugel, Iris Dillmann, Thomas Faestermann, Leticia Fimiani, Karin Hain, Gunther Korschinek, Johannes Lachner, Mikhail Poutivtsev, Klaus Knie, Michael Heil, Franz Käppeler, Anton Wallner

摘要:

结合活化技术和加速器质谱(AMS)测量$^{58}$ Ni $(n,γ)^{59}$ Ni截面。中子活化是在卡尔斯鲁厄3.7 MV的范德格拉夫加速器上进行的,使用的是由$^7$ Li($p,n$)$^7$ Be反应产生的$kT=25$ keV的准恒星中子谱。随后的AMS测量是在位于加尔兴的迈尔-莱布尼茨实验室的14 MV串列加速器上使用充气分析磁铁系统(GAMS)进行的。测量了三个单独的样品,得到在$\langleσ\rangle_{30\text{keV}}$ = 30.4(23)$^{syst}$(9)$^{stat}$ mbarn的$kT=30$ keV下的麦克斯韦平均截面。该值略低于最近发表的两个使用飞行时间(TOF)方法的测量值,但在不确定性范围内一致。我们的新结果还解决了旧TOF测量值与我们以前的值之间的巨大差异。

英文摘要:

The $^{58}$Ni$(n,γ)^{59}$Ni cross section was measured with a combination of the activation technique and accelerator mass spectrometry (AMS). The neutron activations were performed at the Karlsruhe 3.7 MV Van de Graaff accelerator using the quasi-stellar neutron spectrum at $kT=25$ keV produced by the $^7$Li($p,n$)$^7$Be reaction. The subsequent AMS measurements were carried out at the 14 MV tandem accelerator of the Maier-Leibnitz-Laboratory in Garching using the Gas-filled Analyzing Magnet System (GAMS). Three individual samples were measured, yielding a Maxwellian-averaged cross section at $kT=30$ keV of $\langleσ\rangle_{30\text{keV}}$= 30.4 (23)$^{syst}$(9)$^{stat}$ mbarn. This value is slightly lower than two recently published measurements using the time-of-flight (TOF) method, but agrees within the uncertainties. Our new results also resolve the large discrepancy between older TOF measurements and our previous value.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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