Growth, structure, and temperature dependent emission processes in emerging metal hexachloride scintillators Cs2HfCl6 and Cs2ZrCl6

被引:14
作者
Mykhaylyk, V [1 ]
Nagorny, S. S. [2 ,3 ,4 ]
Nahorna, V. V. [2 ,5 ]
Wang, P. [2 ,5 ]
Frogley, M. D. [1 ]
Swiderski, L. [6 ]
Kolomiets, V [7 ]
Vasylechko, L. [8 ]
机构
[1] Diamond Light Source, Harwell Campus, Didcot OX11 0DE, Oxon, England
[2] Queens Univ, Arthur B McDonald Canadian Astroparticle Phys Res, Kingston, ON K7L 3N6, Canada
[3] Queens Univ, Dept Phys, Kingston, ON K7L 3N6, Canada
[4] Queens Univ, Dept Engn Phys & Astron, Kingston, ON K7L 3N6, Canada
[5] Queens Univ, Chem Dept, Kingston, ON K7L 3N6, Canada
[6] Natl Ctr Nucl Res, Soltana 7, PL-05900 Otwock, Poland
[7] Franko Natl Univ Lviv, Phys Dept 1, 50 Dragomanova Str, UA-79005 Lvov, Ukraine
[8] Lviv Polytech Natl Univ, 12 Bandera Str, UA-79013 Lvov, Ukraine
基金
新加坡国家研究基金会; 加拿大创新基金会;
关键词
LUMINESCENCE; CRYSTALS; PHOTOLUMINESCENCE; PROGRESS;
D O I
10.1039/d2dt00223j
中图分类号
O61 [无机化学];
学科分类号
070301 ; 081704 ;
摘要
Crystals of metal hexachlorides Cs2MCl6 (M = Hf or Zr) have recently emerged as promising materials for scintillation applications due to their excellent energy resolution. In this work, we investigated the crystal structure and scintillation properties of Cs2HfCl6 and Cs2ZrCl6 crystals in the broad temperature range from 9 to 300 K. X-ray diffraction data confirmed the same cubic structure (space group Fm3m) for Cs2HfCl6 and Cs2ZrCl6 over the entire examined temperature range. The room temperature scintillation light yield of Cs2HfCl6 excited with a Cs-137 gamma-source is measured to be 24 800 photons per MeV, while Cs2ZrCl6 exhibits 33 900 photons per MeV resulting in energy resolutions of 5.3% and 4.5%, respectively. The alpha-to-beta ratio determined at room temperature for 5.5 MeV alpha-particles from an Am-241 source is equal to 0.39 for Cs2HfCl6 and 0.35 for Cs2ZrCl6. The measurements of scintillation decay curves revealed complex kinetics due to delayed recombination processes. A tangible enhancement of the scintillation yield with heating is observed in the 125-150 K range. This effect is a manifestation of negative thermal quenching explained by thermal activation of trapped carriers. A model of the emission centre is proposed that consistently explains the observed changes of emission intensity with temperature in the crystals under study.
引用
收藏
页码:6944 / 6954
页数:11
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