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The η-NS (%) was not studied for the double-side coated waveguide. For the double-side coated waveguide, the most effective charge generation portion is the top surface of the waveguide that directly faces the sunlight, while the sunlight is largely attenuated once it penetrates through the ZnO NWs, the ITO layer, and the waveguide to reach the bottom surface of the waveguide. The electrons/holes generated at the the top surface cannot be collected since the top Pt counterelectrode is removed to allow the light to reach the solar cell. The photon generated electrons/holes can only be collected for the bottom surface, at which the incident light is significantly attenuated with consideration of the scattering and adsorption of the top surface layer. This attenuation results the low-energy conversion efficiency for the NS configuration and the high EEF.
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