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Optical Analysis of Planar Multicrystalline Perovskite Solar Cells
Author(s) -
van Eerden Maarten,
Jaysankar Manoj,
Hadipour Afshin,
Merckx Tamara,
Schermer John J.,
Aernouts Tom,
Poortmans Jef,
Paetzold Ulrich W.
Publication year - 2017
Publication title -
advanced optical materials
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 2.89
H-Index - 91
ISSN - 2195-1071
DOI - 10.1002/adom.201700151
Subject(s) - materials science , perovskite (structure) , opacity , planar , absorption (acoustics) , optoelectronics , stack (abstract data type) , ellipsometry , layer (electronics) , solar cell , halide , band gap , scattering , optics , thin film , crystallography , nanotechnology , inorganic chemistry , composite material , chemistry , computer graphics (images) , computer science , programming language , physics
Organometal halide perovskites are attracting strong interest as light‐harvesting absorber materials in single‐ and multijunction solar cells. In order to advance the technology, careful optical design of the device architecture and elaborate analysis of optical losses are essential. In this work, a detailed optical analysis of semitransparent and opaque planar CH 3 NH 3 PbI 3 solar cells is reported. Using a combination of variable‐angle spectroscopic ellipsometry and spectrophotometry data, the complex refractive indices of all involved materials in the device architecture are accurately determined, taking the underlying layer stack explicitly into account. The optical properties of partial and complete layer stacks of solar cells, comprising CH 3 NH 3 PbI 3 films with different CH 3 NH 3 PbI 3 surface topography roughnesses, are simulated using the transfer‐matrix method. Very good agreement between simulated and experimental data is demonstrated. Sub‐bandgap absorption is observed in CH 3 NH 3 PbI 3 layer stacks, which is by means of a ray‐tracing model shown to be related to diffuse scattering at the multicrystalline CH 3 NH 3 PbI 3 /air interface. Finally, the optical losses of all layers are discriminated for opaque and semitransparent CH 3 NH 3 PbI 3 solar cells and four‐terminal perovskite/Si tandem solar cells.

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