Sensitivity and Detection Limit of Spectroscopic‐Grade Perovskite CsPbBr3 Crystal for Hard X‐Ray Detection

作者:He Yihui; Hadar Ido; De Siena Michael C.; Klepov Vladislav V.; Pan Lei; Chung Duck Young; Kanatzidis Mercouri G.
来源:Advanced Functional Materials, 2022, 32(24): 2112925.
DOI:10.1002/ADFM.202112925

摘要

Spectroscopic‐grade single crystal detectors can register the energies of individual X‐ray interactions enabling photon‐counting systems with superior resolution over traditional photoconductive X‐ray detection systems. Current technical challenges have limited the preparation of perovskite semiconductors for energy‐discrimination X‐ray photon‐counting detection. Here, this work reports the deployment of a spectroscopic‐grade CsPbBr3 Schottky detector under reverse bias for continuum hard X‐ray detection in both the photocurrent and spectroscopic schemes. High surface barriers of ≈1 eV are formed by depositing solid bismuth and gold contacts. The spectroscopic response under a hard X‐ray source is assessed in resolving the characteristic X‐ray peak. The methodology in enhancing X‐ray sensitivity by controlling the X‐ray energies and flux, and voltage, is described. The X‐ray sensitivity varies between a few tens to over 8000 μC Gyair?1 cm?2. The detectable dose rate of the CsPbBr3 detectors is as low as 0.02 nGyair s?1 in the energy discrimination configuration. Finally, the unbiased CsPbBr3 device forms a spontaneous contact potential difference of about 0.7 V enabling high quality of the CsPbBr3 single crystals to operate in “passive” self‐powered X‐ray detection mode and the X‐ray sensitivity is estimated as 14 μC Gyair?1 cm?2. The great potential of spectroscopic‐grade CsPbBr3 devices for X‐ray photon‐counting systems is anticipated in this work.(#br)The ability of the perovskite CsPbBr3 spectroscopic‐grade detector for continuum hard X‐ray detection in energy‐discrimination configuration (single photon mode), as well as in photoconductive modes is comparatively demonstrated. Blocking contacts are used to achieve energy determination of the incident X‐ray photons and to achieve a low detectable dose rate limit of 0.02 nGyair s?1.