Efficient collection of incoming photons and photo-generated carriers in Si nanostructure array solar cells Yunae Cho, Eunah Kim, and Dong-Wook Kim* Department of Physics, Ewha Womans University, Korea * corresponding author: dwkim@ewha.ac.kr Joondong Kim Department of Electrical Engineering, Incheon National University, Korea Abstract- Si nanostructure array enables much improved broadband and omnidirectional optical absorption, compared with conventional light trapping strategies. We achieved a very high photocurrent density of 36.94 mAcm-2 from our nanoconical frustum array crystalline Si (c-Si) solar cells. Optical simulation studies showed that the expected photocurrent of 10-m-thick nanostructured cells could slightly exceed the Lambertian limit with the help of remarkable antireflection (AR) effects and efficient carrier collection capability. There have been intensive research efforts to realize high efficiency Si nanostructure array solar cells, since the nanostructured Si wafers can significantly lower the optical reflection in broad wavelength range. The remarkable AR effects are originated from graded refractive index, multiple reflection, and Mie resonance.1,2 The measured photovoltaic (PV) performance of nanostructured cells, however, often cannot surpass that of conventional cells, despite their substantially enhanced optical absorption. This suggests that the collection capability of photo-generated carriers as well as the absorption of incoming light should be carefully considered for the nanostructured solar cells. In this work, we performed comparative experimental and simulation studies of hexagonal nanoconical frustum array solar cells to provide insight into improving performance of the nanostructured Si PV devices. The power conversion efficiency of the nano-patterned cell was 15.8%, much higher than that of the flat cell, 14.3%. The optical simulations showed that the optical gain of the nano-patterned cells maintained, as the absorber thickness was reduced to 10 m. The expected photocurrent of the 10 μm thick cell even slightly exceeded the Lambertian limit, due to the increase in absorption for light having a wavelength of >1 μm. The optical benefits of the nanostructure array, in particular the substrate-coupled Mie resonance, also caused strong concentration of light near the top surface of the nano-patterned cells. As a result, the highest photon density was expected to reside near the p–n junction, where the built-in potential readily separates the electron–hole pairs. This would enable very efficient carrier collection, only if proper surface passivation could suppress electrical loss. REFERENCES 1. Kim, J. et al., “Transparent conductor-embedding nanocones for selective emitters: optical and electrical improvements of Si solar cells,” Sci. Rep. Vol. 5, 9256, 2015. 2. Cho, Y. et al., “Wafer-scale nanoconical frustum array crystalline silicon solar cells: promising candidates for ultrathin device applications,” Nanoscale Vol. 6, 9568-9573, 2014.