TY - JOUR
T1 - Single-Crystal Perovskite Solar Cells Exhibit Close to Half A Millimeter Electron-Diffusion Length
AU - Turedi, Bekir
AU - Lintangpradipto, Muhammad N.
AU - Sandberg, Oskar J.
AU - Yazmaciyan, Aren
AU - Matt, Gebhard J.
AU - Alsalloum, Abdullah Y.
AU - Almasabi, Khulud
AU - Sakhatskyi, Kostiantyn
AU - Yakunin, Sergii
AU - Zheng, Xiaopeng
AU - Naphade, Rounak
AU - Nematulloev, Saidkhodzha
AU - Yeddu, Vishal
AU - Baran, Derya
AU - Armin, Ardalan
AU - Saidaminov, Makhsud I.
AU - Kovalenko, Maksym V.
AU - Mohammed, Omar F.
AU - Bakr, Osman M.
N1 - Funding Information:
The authors acknowledge funding support from King Abdullah University of Science and Technology (KAUST). The work at Eidgenössiche Technische Hochschule Zürich (ETH Zürich) was financially supported by the Swiss Innovation Agency (Innosuisse) under grant agreement 46894.1 IP‐ENG and by ETH Zürich through the ETH+ Project SynMatLab: Laboratory for Multiscale Materials Synthesis. The work at the University of Victoria was supported in part by the Natural Sciences and Engineering Research Council (NSERC) of Canada.
Publisher Copyright:
© 2022 Wiley-VCH GmbH.
PY - 2022/11/24
Y1 - 2022/11/24
N2 - Single-crystal halide perovskites exhibit photogenerated-carriers of high mobility and long lifetime, making them excellent candidates for applications demanding thick semiconductors, such as ionizing radiation detectors, nuclear batteries, and concentrated photovoltaics. However, charge collection depreciates with increasing thickness; therefore, tens to hundreds of volts of external bias is required to extract charges from a thick perovskite layer, leading to a considerable amount of dark current and fast degradation of perovskite absorbers. However, extending the carrier-diffusion length can mitigate many of the anticipated issues preventing the practical utilization of perovskites in the abovementioned applications. Here, single-crystal perovskite solar cells that are up to 400 times thicker than state-of-the-art perovskite polycrystalline films are fabricated, yet retain high charge-collection efficiency in the absence of an external bias. Cells with thicknesses of 110, 214, and 290 µm display power conversion efficiencies (PCEs) of 20.0, 18.4, and 14.7%, respectively. The remarkable persistence of high PCEs, despite the increase in thickness, is a result of a long electron-diffusion length in those cells, which was estimated, from the thickness-dependent short-circuit current, to be ≈0.45 mm under 1 sun illumination. These results pave the way for adapting perovskite devices to optoelectronic applications in which a thick active layer is essential.
AB - Single-crystal halide perovskites exhibit photogenerated-carriers of high mobility and long lifetime, making them excellent candidates for applications demanding thick semiconductors, such as ionizing radiation detectors, nuclear batteries, and concentrated photovoltaics. However, charge collection depreciates with increasing thickness; therefore, tens to hundreds of volts of external bias is required to extract charges from a thick perovskite layer, leading to a considerable amount of dark current and fast degradation of perovskite absorbers. However, extending the carrier-diffusion length can mitigate many of the anticipated issues preventing the practical utilization of perovskites in the abovementioned applications. Here, single-crystal perovskite solar cells that are up to 400 times thicker than state-of-the-art perovskite polycrystalline films are fabricated, yet retain high charge-collection efficiency in the absence of an external bias. Cells with thicknesses of 110, 214, and 290 µm display power conversion efficiencies (PCEs) of 20.0, 18.4, and 14.7%, respectively. The remarkable persistence of high PCEs, despite the increase in thickness, is a result of a long electron-diffusion length in those cells, which was estimated, from the thickness-dependent short-circuit current, to be ≈0.45 mm under 1 sun illumination. These results pave the way for adapting perovskite devices to optoelectronic applications in which a thick active layer is essential.
KW - diffusion length
KW - perovskites
KW - single crystals
KW - solar cells
KW - thickness-control
UR - http://www.scopus.com/inward/record.url?scp=85140037337&partnerID=8YFLogxK
U2 - 10.1002/adma.202202390
DO - 10.1002/adma.202202390
M3 - Article
C2 - 36069995
AN - SCOPUS:85140037337
SN - 0935-9648
VL - 34
JO - Advanced Materials
JF - Advanced Materials
IS - 47
M1 - 2202390
ER -