However, solar cells made from ZnO/CdTe epitaxy-free planar layers have already reached the photo-conversion efficiency of 12.3%, which clearly indicates that the combination of ZnO with CdTe can work for photovoltaic devices [18]. It is also worth noticing that dye-sensitized solar cells made from identical ZnO NWs can lead to the photo-conversion efficiency as high as 4.7%, which somehow points out that the electron conduction in ZnO NWs and collection from

FTO top-side contact are not the limiting physical processes [11]. Instead, the poor collection MNK inhibitor of the holes from the CuSCN/Au back-side contact is presumably expected to be critical. The holes that are mainly photo-generated at the extreme bottom of the ZnO/CdTe core-shell NW arrays inside the CdTe shell just like the electrons are much farther from the Au back-side contact than the electrons from the FTO top-side contact. The Selleckchem SC79 poor collection of the holes may be due to (i) the low conductivity of the CuSCN layer and (ii) the CdTe/CuSCN band alignment. The diffusion of copper in the CdTe shell may occur as well, but the deposition of the

CuSCN layer is achieved at the low growth temperature of 100°C. Eventually, light-soaking effects occur in the annealed ZnO/CdTe core-shell NW arrays, as selleck screening library revealed in Figure  6b. After 2 min of AM 1.5G standard illuminations, the J SC increased from 0.35 to 0.45 mA/cm2 while slightly reducing the V OC. The relative decrease in the V OC can be related to an increase in the solar cell temperature, which was not monitored. However, the increase in the J SC is too high to be only due to solar cell temperature effects. Metastable effects in p-CdTe/n-CdS heterojunction solar cells or modules have already been reported, originating from copper diffusion from the back-side contact [69, 70]. Here, light-soaking effects are more likely associated with the saturation of trap centers in CdTe NGs, leading to the increase in the J SC through Forskolin in vitro the collection of more electrons and holes [71]. Figure 6 Photovoltaic

properties. (a) J(V) characteristics of the as-grown and annealed ZnO/CdTe core-shell NW arrays at 300°C and 450°C for 1 h, under dark conditions (dashed lines) and AM 1.5G standard illumination conditions (solid lines). (b) J(V) characteristics of annealed ZnO/CdTe core-shell NW arrays at 450°C for 1 h under dark conditions (dashed line) and AM 1.5G standard illumination conditions (solid lines). The illumination is performed for a varying time (i.e., light-soaking effects). Figure 7 Light-harvesting efficiency and polychromatic radial optical generation rate. (a) Light-harvesting efficiency (LHE) of the as-grown and annealed ZnO/CdTe core-shell NW arrays at 300°C and 450°C for 1 h, respectively.