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. 2015 May 15;27(25):3760–3766. doi: 10.1002/adma.201500889

Figure 2.

Figure 2

a) Photocurrent ΔI versus V s at T = 300 K and V g = 0 V under light illumination with a focused laser beam of power P, 102 P, 103 P, and 104 P (P = 0.5 nW, λ = 633 nm). The inset shows the photocurrent map indicating that ΔI arises primarily from the InSe layer between the two graphene electrodes, g1 and g2. b) Photoconductivity spectra at T = 300 K and V s = 2 V with unfocused light and power P ≈ 10 pW. The inset shows a color map of ΔI versus V g and V s with a laser at λ = 633 nm. c) Temporal dependence of the photocurrent (V g = 0 V, V s = 1 V, and λ = 633 nm). The dashed line shows the modulation of the laser beam at frequency f = 100 Hz.