论文标题

$^{159} $ tb(n,$γ$)横截面的测量

Measurement of the $^{159}$Tb(n, $γ$) cross section at the CSNS Back-n facility

论文作者

Zhang, S., Li, G., Jiang, W., Wang, D. X., Ren, J., Li, E. T., Huang, M., Tang, J. Y., Ruan, X. C., Wang, H. W., Li, Z. H., Chen, Y. S., Liu, L. X., Li, X. X., Fan, Q. W., Fan, R. R., Hu, X. R., Wang, J. C., Li, X., Niu, 1D. D., Song, N., Gu, M.

论文摘要

在$ \ $ 160左右的质量数的恒星(n,$γ$)的横截面数据对慢速中子捕获过程的主要组成部分中的核合成至关重要,在慢速中子捕获过程的主要成分中,这发生在热脉动渐近的巨型分支(TP-agb)中。 $^{159} $ tb的(n,$γ$)横截面的新测量是使用C $ _6 $ _6 $ _6 $ _6 $检测器系统在中国中国剥离中子中子梁线(后N)的后面流媒体中子中子源(CSN),并使用1 ev到1 mev的中子能量。通过此捕获测量,据报道,实验性共振捕获核高达1.2 KEV中子能量。 Maxwellian-averaged cross sections (MACS) were derived from the measured $^{159}$Tb (n, $γ$) cross sections at $kT$ = 5 $\sim$ 100 keV and are in good agreement with the recommended data of KADoNiS-v0.3 and JEFF-3.3, while KADoNiS-v1.0 and ENDF-VIII.0 significantly overestimate the present MACS up to 40 $ \%$和20 $ \%$。还使用恒星进化代码台面进行了S过程的核合成敏感测试。在MESA模拟中,ENDF/B-VIII.0.0和目前的测量率在$^{159} $ tb(n,$γ$)$^{160} $ tb之间,观察到了$ \ $ 160的大量变化。

The stellar (n, $γ$) cross section data for the mass numbers around A $\approx$ 160 are of key importance to nucleosynthesis in the main component of the slow neutron capture process, which occur in the thermally pulsing asymptotic giant branch (TP--AGB). The new measurement of (n, $γ$) cross sections for $^{159}$Tb was performed using the C$_6$D$_6$ detector system at the back streaming white neutron beam line (Back-n) of the China spallation neutron source (CSNS) with neutron energies ranging from 1 eV to 1 MeV. Experimental resonance capture kernels were reported up to 1.2 keV neutron energy with this capture measurement. Maxwellian-averaged cross sections (MACS) were derived from the measured $^{159}$Tb (n, $γ$) cross sections at $kT$ = 5 $\sim$ 100 keV and are in good agreement with the recommended data of KADoNiS-v0.3 and JEFF-3.3, while KADoNiS-v1.0 and ENDF-VIII.0 significantly overestimate the present MACS up to 40$\%$ and 20$\%$, respectively. A sensitive test of the s-process nucleosynthesis was also performed with the stellar evolution code MESA. Significant changes in abundances around A $\approx$ 160 were observed between the ENDF/B-VIII.0 and present measured rate of $^{159}$Tb(n, $γ$)$^{160}$Tb in the MESA simulation.

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