The dark and photocurrent values were 7.35 and 22.89 μA, respectively, which clearly indicate a threefold increase in the dark current value. JNK animal study Figure 4 I – V curves of the area-selective deposited ZnO nanorods in dark and UV light environments. The sensor mechanism is based on Equations (1) to (3) [35, 36]; the reactions on the ZnO nanorod surface during UV illumination can be explained as follows: when the adsorbed
oxygen OSI-906 purchase molecules capture the electron from the conduction band, a negative space charge layer is created, which results in enhanced resistivity . (1) When the photon energy is greater than the bandgap energy (Eg), the incident radiation is adsorbed in the ZnO nanorod UV sensor, which results in electron–hole pairs. (2) The positively charge holes that were created due to the photogeneration neutralize the chemisorbed oxygen that was responsible for higher resistance that revealed conductivity increment, and as a consequence, the photocurrent increases. where O2 is the oxygen molecule, e – is the free electron and the photogenerated electron in the conduction band, is the adsorbed oxygen, hv is the photon energy of the UV light, and h + is the photogenerated hole in the valence band. After the UV light is switched
on, the number of oxygen molecules on the ZnO nanorod surface rapidly reaches the maximum value in response to the ultraviolet light . When the ultraviolet selleck chemical light is switched off, the oxygen molecules are reabsorbed
on the ZnO nanorod surface. Thus, the sensor reverts to its initial mode . An important parameter used to evaluate the suitability of the sensor for UV-sensing applications is spectral responsivity as a function of different wavelengths. This parameter yields the internal photoconductive gain. Generally, the sensor responsivity can be calculated as  (3) where λ, q, h, c, and η show the wavelength, electron charge, Planck’s constant, light velocity, external quantum efficiency, and internal gain of the sensor. As see more shown in Figure 5, the sensor responsivity shows a linear behavior below the bandgap UV region (300 to 370 nm) and a sharp cutoff with a decrease of two to three orders of magnitude at approximately 370 nm. The maximum responsivity of our sensor at an applied bias of 5 V was 2 A/W, which is higher than the values reported in the literature [41–43]. Figure 5 Spectral responsivity of area-selective deposited ZnO nanorods between the microgap electrodes. Another important parameter for UV sensor is the current-to-time (I-t) response in the switched on/off states of UV light. Figure 6 shows the I-t response curves at different voltages of area-selective deposited ZnO nanorods on microgap electrodes with UV illumination. The rise time was 72 s, whereas the decay time was 110 s.