Ultrafast self-trapping of photoexcited carriers sets the upper limit on antimony trisulfide photovoltaic devices.
basic_science · Level V
Where this comes from
- Record sourced from PubMed, PMID 31586054.
- Also identified by DOI 10.1038/s41467-019-12445-6 and PMC identifier 6778121.
- Licence recorded as CC BY.
- The licence permits redistribution, so the abstract is shown in full and the full text is available from the publisher.
Abstract
Antimony trisulfide (Sb<sub>2</sub>S<sub>3</sub>) 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<sub>2</sub>S<sub>3</sub> 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<sup>20</sup> cm<sup>-3</sup>. These features, together with polarized trap emission from Sb<sub>2</sub>S<sub>3</sub> single crystal, strongly suggest that photoexcited carriers in Sb<sub>2</sub>S<sub>3</sub> 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<sub>2</sub>S<sub>3</sub> 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<sub>2</sub>S<sub>3</sub> solar cells.