2021
DOI: 10.1039/d0tc05148a
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Radiation hardness and abnormal photoresponse dynamics of the CH3NH3PbI3 perovskite photodetector

Abstract: Schematic diagram of the perovskite photodetector under proton irradiation and the degradation mechanism of the functional layer after irradiation.

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Cited by 12 publications
(18 citation statements)
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“…Similar behavior has been previously observed in organic–inorganic hybrid perovskite photodetectors and attributed to irradiation‐induced defect formation. [ 40 ] Another possible reason may be related to the pile‐up effects leading to severe recombination of the photogenerated carriers due to their small mobilities as shown in Figure 3d.…”
Section: Resultsmentioning
confidence: 99%
“…Similar behavior has been previously observed in organic–inorganic hybrid perovskite photodetectors and attributed to irradiation‐induced defect formation. [ 40 ] Another possible reason may be related to the pile‐up effects leading to severe recombination of the photogenerated carriers due to their small mobilities as shown in Figure 3d.…”
Section: Resultsmentioning
confidence: 99%
“…6 The presence of large Z-elements (Pb, I, Br, Cs) in the compositions of HP, high density (>3.8 g cm −3 ) 7 and large carrier drift lengths (the μτ products) 8 demonstrates the high potential of HP for use in radiation detectors. Promising results for radiation tolerance under X-rays 9 and proton fluence 10 have been demonstrated for solar cells with HP-based absorbers. Moreover, the hybrid nature of the chemical compositions with organic–inorganic cations (CH 3 NH 3 PbI 3 , etc. )…”
Section: Introductionmentioning
confidence: 99%
“…It is noteworthy that conventional CH 3 NH 3 PbI 3 perovskite photodiodes exhibited a 60% drop in EQE after the same irradiation fluence of 150 keV protons under a steady low‐intensity beam. [ 19 ] This indicates that the photodiodes made of the high‐performance multicomponent Cs 0.04 Rb 0.04 (FA 0.65 MA 0.35 ) 0.92 Pb(I 0.85 Br 0.14 Cl 0.01 ) 3 perovskite material exhibit a higher radiation resistance even under intense short‐pulse proton irradiation (see Table S1, Supporting Information for more details). Optical properties of the perovskite, Spiro‐OMeTAD and SnO 2 functional layers remain unchanged under proton irradiation with the accumulated fluence up to 10 13 protons cm −2 .…”
Section: Resultsmentioning
confidence: 99%
“…This is due to the formation of shallow traps in the perovskite active layer, which possess a long recharge time . [ 15,16,19 ]…”
Section: Resultsmentioning
confidence: 99%
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