Abstract

Differential and angle-integrated cross sections for the 10^{10}B(n,αn, α)7^{7}Li, 10^{10}B(n,αn, α0_{0})7^{7}Li and 10^{10}B(n,αn, α1_{1})7^{7}Li∗^{*} reactions have been measured at CSNS Back-n white neutron source. Two enriched (90%) 10^{10}B samples 5.0 cm in diameter and ~85.0 μμg/cm2^{2} in thickness each with an aluminum backing were prepared, and back-to-back mounted at the sample holder. The charged particles were detected using the silicon-detector array of the Light-charged Particle Detector Array (LPDA) system. The neutron energy En_{n} was determined by TOF (time-of-flight) method, and the valid αα events were extracted from the En_{n}-Amplitude two-dimensional spectrum. With 15 silicon detectors, the differential cross sections of αα-particles were measured from 19.2° to 160.8°. Fitted with the Legendre polynomial series, the (n,αn, α) cross sections were obtained through integration. The absolute cross sections were normalized using the standard cross sections of the 10^{10}B(n,αn, α)7^{7}Li reaction in the 0.3 - 0.5 MeV neutron energy region. The measurement neutron energy range for the 10^{10}B(n,αn, α)7^{7}Li reaction is 1.0 eV ≤\le En < 2.5 MeV (67 energy points), and for the 10^{10}B(n,αn, α0_{0})7^{7}Li and 10^{10}B(n,αn, α1_{1})7^{7}Li∗^{*} reactions is 1.0 eV ≤\le En < 1.0 MeV (59 energy points). The present results have been analyzed by the resonance reaction mechanism and the level structure of the 11^{11}B compound system, and compared with existing measurements and evaluations.

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