7 and 1.2 × 105, respectively. In contrast, the filled factor (FF) does not seem to depend on post-growth heat treatment. The chlorine doping of CdTe NGs and the related GB passivation following the CdCl2 heat treatment are thus beneficial for the photovoltaic properties. The best photovoltaic properties only result in a photo-conversion efficiency of about 0.01%: this is fairly low as compared to the photo-conversion efficiency of 4.74% for ZnO/CdSe [65], 4.15% for ZnO/CdS/CdSe [66], and 4.17% for ZnO/In2S3/CuInS2 NW arrays [67].

However, it has widely been reported that the photovoltaic properties of ZnO/CdTe core-shell NW arrays are poor [22, 24, 25, 27, 29, 32]. The low V OC may originate from the occurrence of cracks in the CuSCN thick layer acting as the hole-collecting layer, which could also increase the series resistance [32]. In contrast, the J SC depends, in addition to the incident spectral flux density, RG-7388 datasheet on the EQE, which is the MK5108 supplier number of collected charge carriers divided by the number of incident photons. The EQE for the annealed ZnO/CdTe core-shell NW arrays is about 2% above the bandgap energy of 1.5 eV for CdTe, as shown in Figure  8. Basically, the EQE is

equal to the internal quantum efficiency (IQE) multiplied by the light-harvesting efficiency. Still, the light-harvesting efficiency see more is fairly high in ZnO/CdTe core-shell NW arrays, as revealed in Figure  7a: the light-harvesting efficiency is typically larger than 90% at the energy of 2.36 eV (i.e., the wavelength of 525 nm at the maximum of the solar irradiance). This is in agreement with the systematic optical simulations of the ideal J SC by RCWA, which have emphasized the large

absorption capability of ZnO/CdTe core-shell NW arrays [20]. As a consequence, the low J SC and EQE arise from the poor IQE: this indicates that most of the photo-generated charge carriers in CdTe NGs is lost. The location where the charge carriers are photo-generated is given in Figure  7b, by the maps of the polychromatic radial optical generation rate. Interestingly, most of the charge carriers are actually photo-generated in the CdTe shell, owing to its bandgap energy of 1.5 eV in contrast to the wide bandgap energy of ZnO and CuSCN. A smaller proportion of PAK6 the incident light is still absorbed in the ZnO NWs, especially for lower wavelength. More importantly, the optical generation rate is significantly decreased from the bottom to the top of the ZnO/CdTe core-shell NW arrays, as shown in Figure  7b. The vast majority of charge carriers is even photo-generated at the extreme bottom of the ZnO/CdTe core-shell NW arrays inside the CdTe shell. It is expected that the main critical point for these solar cells is related to the collection of the photo-generated charge carriers. The absence of structural relationship (i.e.