2021
DOI: 10.1016/j.jmst.2021.01.020
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High-performance and broadband photodetection of bicrystalline (GaN)1-(ZnO) solid solution nanowires via crystal defect engineering

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Cited by 10 publications
(2 citation statements)
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“…In addition, the InGaN NR based PD exhibits a weak photoresponse in the wavelength range of 450 to 650 nm due to the existence of defect states whose defect level serves as carrier transition energy level. 30 To further analyze the dependence of photocurrent and light power density, the time-dependent photocurrent under different light power densities from 70 μW/cm 2 to 15.5 mW/cm 2 and zero bias are shown in Figure 3f. The relationship of transient photocurrent and pulse light power density is shown in Figure S9, and the fitting factor is calculated to be 0.79, and the change of the power-law dependence indicates a complex recombination process of carriers through trap states.…”
Section: Resultsmentioning
confidence: 99%
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“…In addition, the InGaN NR based PD exhibits a weak photoresponse in the wavelength range of 450 to 650 nm due to the existence of defect states whose defect level serves as carrier transition energy level. 30 To further analyze the dependence of photocurrent and light power density, the time-dependent photocurrent under different light power densities from 70 μW/cm 2 to 15.5 mW/cm 2 and zero bias are shown in Figure 3f. The relationship of transient photocurrent and pulse light power density is shown in Figure S9, and the fitting factor is calculated to be 0.79, and the change of the power-law dependence indicates a complex recombination process of carriers through trap states.…”
Section: Resultsmentioning
confidence: 99%
“…Moreover, the InGaN NR/PEDOT:PSS PD and InGaN NR/PEDOT:PSS@Ag NW PD exhibit a higher responsivity in the ultraviolet region, and the main reason is that the PEDOT:PSS material increases ultraviolet absorption as demonstrated by the absorption spectrum (Figure c). In addition, the InGaN NR based PD exhibits a weak photoresponse in the wavelength range of 450 to 650 nm due to the existence of defect states whose defect level serves as carrier transition energy level . To further analyze the dependence of photocurrent and light power density, the time-dependent photocurrent under different light power densities from 70 μW/cm 2 to 15.5 mW/cm 2 and zero bias are shown in Figure f.…”
Section: Resultsmentioning
confidence: 99%