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Measurement of the 159Tb(n, ?) cross section at the CSNS Back-n facility

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PHYSICAL REVIEW C
卷 107, 期 4, 页码 -

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AMER PHYSICAL SOC
DOI: 10.1103/PhysRevC.107.045809

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The (n, gamma) cross section data for 159Tb was measured using the C6D6 detector system at the China spallation neutron source. The derived Maxwellian-averaged cross sections (MACS), based on the measured data, are in good agreement with KADoNiS-v0.3 and JEFF-3.3, but over-estimate significantly in KADoNiS-v1.0 and ENDF-VIII.0. The stellar evolution simulation using the obtained rate of 159Tb(n, gamma) 160Tb shows significant changes in abundances around A approximate to 160 compared to ENDF/B-VIII.0.
The stellar (n, gamma) cross section data for the mass numbers around A approximate to 160 are of key importance to nucle-osynthesis in the main component of the slow neutron capture process, which occurs in the thermally pulsing asymptotic giant branch (TP-AGB). The new measurement of (n, gamma) cross sections for 159Tb was performed using the C6D6 detector system at the back streaming white neutron beam line (Back-n) of the China spallation neutron source with neutron energies ranging from 1 eV to 1 MeV. Experimental resonance capture kernels are reported up to 1.2 keV neutron energy with this capture measurement. Maxwellian-averaged cross sections (MACS) are derived from the measured 159Tb(n, gamma) cross sections at kT = 5-100 keV , 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 over-estimate the present MACS up to 40% and 20%, respectively. A sensitive test of the s-process nucleosynthesis is also performed with the stellar evolution code MESA. Significant changes in abundances around A approximate to 160 are observed between the ENDF/B-VIII.0 and present measured rate of 159Tb(n, gamma) 160Tb in the MESA simulation.

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