Abstract

Since single junction c-Si solar cells are reaching their practical efficiency limit. Perovskite/c-Si tandem solar cells hold the promise of achieving greater than 30% efficiencies. In this regard, optical simulations can deliver guidelines for reducing the parasitic absorption losses and increasing the photocurrent density of the tandem solar cells. In this work, an optical study of 2, 3 and 4 terminal perovskite/c-Si tandem solar cells with c-Si solar bottom cells passivated by high thermal-budget poly-Si, poly-SiOx and poly-SiCx is performed to evaluate their optical performance with respect to the conventional tandem solar cells employing silicon heterojunction bottom cells. The parasitic absorption in these carrier selective passivating contacts has been quantified. It is shown that they enable greater than 20mA/cm2 matched implied photocurrent density in un-encapsulated 2T tandem architecture along with being compatible with high temperature production processes. For studying the performance of such tandem devices in real-world irradiance conditions and for different locations of the world, the effect of solar spectrum and angle of incidence on their optical performance is studied. Passing from mono-facial to bi-facial tandem solar cells, the photocurrent density in the bottom cell can be increased, requiring again optical optimization. Here, we analyse the effect of albedo, perovskite thickness and band gap as well as geographical location on the optical performance of these bi-facial perovskite/c-Si tandem solar cells. Our optical study shows that bi-facial 2T tandems, that also convert light incident from the rear, require radically thicker perovskite layers to match the additional current from the c-Si bottom cell. For typical perovskite bandgap and albedo values, even doubling the perovskite thickness is not sufficient. In this respect, lower bandgap perovskites are very interesting for application not only in bi-facial 2T tandems but also in related 3T and 4T tandems.

Highlights

  • Crystalline silicon (c-Si) solar cells dominate the photovoltaic market due to their relatively high efficiency, low manufacturing costs and long-term stability

  • We found that the influence of tunnel recombination junction (TRJ) layers for all cases of c-Si bottom cells on the optical performance of 3T tandem devices was negligible and due to the decoupling of Jph between top and bottom cells

  • In 2T tandem configuration high temperature Carrier-selective passivating contacts (CSPCs) such as poly-Si, poly-SiOx and poly-SiCx can achieve matched photocurrent density greater than 20 mA/cm2 and around 19.5 mA/cm2 without encapsulation and with encapsulation, respectively. These values are slightly lower than those of a 2T tandem based on silicon heterojunction (SHJ) bottom cell because of the high doping-driven free carrier absorption in high-thermal budget CSPCs

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Summary

Introduction

Crystalline silicon (c-Si) solar cells dominate the photovoltaic market due to their relatively high efficiency, low manufacturing costs and long-term stability. Perovskite/perovskite [3,4,5,6] and perovskite/c-Si [7,8,9,10,11,12,13,14,15,16,17,18,19,20,21,22,23,24,25,26] tandem solar cells are gaining lot of attention in this regard This is because perovskite solar cells have a sharp optical edge, a long diffusion length, a tuneable bandgap range and a good short wavelength response [27,28,29,30]. Widespread industrial c-Si solar cells are compatible with high temperature processes such as impurity gettering, thermal oxidation, dopants

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