DocumentCode :
10477
Title :
Fast Neutron Detection With {\\rm Cs}_{2} {\\rm LiYCl}_{6}
Author :
Glodo, J. ; Shirwadkar, U. ; Hawrami, R. ; Achtzehn, T. ; Andrews, H.R. ; Clifford, E.T.H. ; Ing, H. ; Kovaltchouk, V.D. ; Smith, Martin B. ; Shah, K.S.
Author_Institution :
Radiat. Monitoring Devices, Watertown, MA, USA
Volume :
60
Issue :
2
fYear :
2013
fDate :
Apr-13
Firstpage :
864
Lastpage :
870
Abstract :
This paper discusses our initial investigation of fast neutron detection with a Cs2LiYCl6 (CLYC) scintillator. CLYC has been already developed for dual mode detectors (thermal neutrons and gamma rays). Described are results collected under mono-energetic irradiation from a Van de Graaff generator and a continuous irradiation from a 252Cf source. There are two reactions in which fast neutrons are captured 35Cl(n,p)35S and 6Li(n,t)α; both have been observed. They produce a proton and a pair of α/t particles, respectively. The response to mono-energetic fast neutrons due to the 35Cl(n,p) reaction produces a peak and due to the 6Li(n,t) reaction a continuum in the energy spectra. The relation between the peak (continuum) position and the excitation energy is linear within evaluated energy range. This allows for fast neutron spectroscopy. The α/β ratios for both reactions were found to be different and somewhat dependent on the excitation energy. The decay times under the proton excitation slightly differ from these under the α/t excitation, while both are significantly different from the gamma ray excited curves. This is important for pulse shape discrimination. Using continuous excitation from 252Cf initial efficiency was estimated for the 35Cl(n,p) reaction. For a 1-inch right cylinder crystal the measured intrinsic efficiency is at least 0.06%, while calculated is 0.5%. The discrepancy is due to experimental inaccuracies. The relative detection efficiency scales linearly with the volume. A convolution of the theoretical 252Cf fast neutron distribution and the 35Cl(n,p) cross-section curve was found to match the experimental data.
Keywords :
gamma-ray detection; neutron detection; neutron spectroscopy; neutron-nucleus reactions; nuclei with mass number 20 to 38; nuclei with mass number 6 to 19; pulse shaping circuits; radioactive sources; solid scintillation detectors; van de Graaff accelerators; 252Cf; 252Cf fast neutron distribution; 252Cf source; 35Cl(n,p)35S; 6Li(n,t)alpha; CLYC scintillator; Cs2LiYCl6; Van de Graaff generator; continuous irradiation; cylinder crystal; energy spectra; excitation energy; fast neutron detection; fast neutron spectroscopy; gamma ray detectors; gamma ray excited curves; intrinsic efficiency; monoenergetic fast neutron; monoenergetic irradiation; peak continuum position; proton excitation; proton production; pulse shape discrimination; relative detection efficiency scales; thermal neutrons detector; Crystals; Detectors; Ions; Neutrons; Particle beams; Protons; Radiation effects; $^{35}{rm Cl}({rm n, p})$ reaction; ${rm Cs}_{2}{rm LiYCl}_{6}$; CLYC; elpasolite crystals; fast neutrons; neutron detectors; radiation detectors;
fLanguage :
English
Journal_Title :
Nuclear Science, IEEE Transactions on
Publisher :
ieee
ISSN :
0018-9499
Type :
jour
DOI :
10.1109/TNS.2012.2227499
Filename :
6410458
Link To Document :
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