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The FM has a much smaller cross-sectional area (A) compared to the device.
Thus, the Schottky diode shows much faster switching under pulsed UV illumination as compared to the device with ohmic contacts on both the sides.
This explains the better sensitivity and faster switching of the photocurrent in the Schottky barrier devices as compared to the device with ohmic contact on both sides.
And it has been reported that the perovskite solar cells based on Li-doped TiO2 produce higher performances compared to the device based on un-doped TiO2 [16].
It is also observed that the presence of the NiO buffer layer decreased the leakage current and showed higher series resistance compared to the device based on only n-ZnO/p-GaN heterojunction.
Apart from the geometry, the main difference of this sample compared to the device presented in Ref. [27] is the higher root mean square variation of the height (r h) on the island.
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The fabricated DSSCs with the GZO/TiO2 glasses showed an enhanced conversion efficiency of 4.02% compared to the devices with the normal GZO glasses (3.36%).
The uniaxially strained pMOSFETs achieve a 24% reduction in ΔR total/ΔL G slope i.e. R ch, compared to the devices without uniaxial compressive strain.
The uniaxially strained pMOSFETs exhibit a smaller ΔR total/ΔL G slope, indicating higher channel μ eff compared to the devices without uniaxial compressive strain.
Compared to the devices without interlayer, all the devices exhibit significant improvements of the device parameters by reducing the work function of indium tin oxide (ITO) cathode.
Significant improvement in harvesting photo-generated currents and low series resistances were observed which lead to higher power conversion efficiencies compared to the devices without ZnO CNT.
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