2023
DOI: 10.1016/j.apsusc.2023.156983
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Phenethylammonium iodide modulated SnO2 electron selective layer for high performance, self-powered metal halide perovskite photodetector

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Cited by 12 publications
(7 citation statements)
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“…Therein, i n is derived from a fast Fourier transform of the acquired dark current as a function of time at 0 V, as illustrated in Figure S21. In the frequency range below 250 Hz, the i n – f curve for PDs is primarily dominated by flicker noise (1/ f noise) . Above 250 Hz, the i n values remain constant and show little frequency dependence, as for the 14-FABA-modified PDs, the constant i n value is ∼2.05 × 10 –12 A/Hz 1/2 .…”
Section: Resultsmentioning
confidence: 99%
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“…Therein, i n is derived from a fast Fourier transform of the acquired dark current as a function of time at 0 V, as illustrated in Figure S21. In the frequency range below 250 Hz, the i n – f curve for PDs is primarily dominated by flicker noise (1/ f noise) . Above 250 Hz, the i n values remain constant and show little frequency dependence, as for the 14-FABA-modified PDs, the constant i n value is ∼2.05 × 10 –12 A/Hz 1/2 .…”
Section: Resultsmentioning
confidence: 99%
“…The tests on the noise current spectrum of perovskite devices modified with 14-FABA were also conducted to further confirm the validity of the D *. According to the work of Wang et al, the D * values can be obtained by following the formula: D * = R A B i n , where A , B , and i n are the effective photoactive area, bandwidth, and i n , respectively. Therein, i n is derived from a fast Fourier transform of the acquired dark current as a function of time at 0 V, as illustrated in Figure S21.…”
Section: Resultsmentioning
confidence: 99%
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“…This D * value is larger than or comparable to those of previously reported self-powered n–i–p-type perovskite-based PDs (Table ). ,,, …”
Section: Resultsmentioning
confidence: 99%