Ultrafast self-trapping of photoexcited carriers sets the upper limit on antimony trisulfide photovoltaic devices

Antimony trisulfide (Sb 2 S 3 ) is considered to be a promising photovoltaic material; however, the performance is yet to be satisfactory. Poor power conversion efficiency and large open circuit voltage loss have been usually ascribed to interface and bulk extrinsic defects By performing a spectrosc...

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Published inNature communications Vol. 10; no. 1; pp. 4540 - 8
Main Authors Yang, Zhaoliang, Wang, Xiaomin, Chen, Yuzhong, Zheng, Zhenfa, Chen, Zeng, Xu, Wenqi, Liu, Weimin, Yang, Yang (Michael), Zhao, Jin, Chen, Tao, Zhu, Haiming
Format Journal Article
LanguageEnglish
Published London Nature Publishing Group UK 04.10.2019
Nature Publishing Group
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Summary:Antimony trisulfide (Sb 2 S 3 ) is considered to be a promising photovoltaic material; however, the performance is yet to be satisfactory. Poor power conversion efficiency and large open circuit voltage loss have been usually ascribed to interface and bulk extrinsic defects By performing a spectroscopy study on Sb 2 S 3 polycrystalline films and single crystal, we show commonly existed characteristics including redshifted photoluminescence with 0.6 eV Stokes shift, and a few picosecond carrier trapping without saturation at carrier density as high as approximately 10 20  cm −3 . These features, together with polarized trap emission from Sb 2 S 3 single crystal, strongly suggest that photoexcited carriers in Sb 2 S 3 are intrinsically self-trapped by lattice deformation, instead of by extrinsic defects. The proposed self-trapping explains spectroscopic results and rationalizes the large open circuit voltage loss and near-unity carrier collection efficiency in Sb 2 S 3 thin film solar cells. Self-trapping sets the upper limit on maximum open circuit voltage (approximately 0.8 V) and thus power conversion efficiency (approximately 16 %) for Sb 2 S 3 solar cells. Antimony trisulfide has a proper bandgap of 1.7 eV for making solar cells but the devices suffer from severe voltage loss. Here Yang et al. propose that the photoexcited carriers are self-trapped by lattice deformation, which places a thermodynamic limit of only 0.8 V for the open circuit voltage.
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ISSN:2041-1723
2041-1723
DOI:10.1038/s41467-019-12445-6