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Charge Transport and Defects in Sulfur-Deficient Chalcogenide Perovskite BaZrS3

Garima Aggarwal1,*,†, Adeem Saeed Mirza2,‡, Stefania Riva3,‡, Corrado Comparotto1, Robert J. W. Frost4, Soham Mukherjee3, Monica Morales-Masis2, Håkan Rensmo3, and Jonathan Staaf Scragg1

  • 1Division of Solar Cell Technology, Department of Materials Science and Engineering, Uppsala University, 75237 Uppsala, Sweden
  • 2MESA+ Institute for Nanotechnology, University of Twente, 7500 AE Enschede, The Netherlands
  • 3Division of X-Ray Photon Science, Department of Physics and Astronomy, Uppsala University, Box 516, SE-75120 Uppsala, Sweden
  • 4Division of Applied Nuclear Physics, Department of Physics and Astronomy, Uppsala University, Box 516, 75120 Uppsala, Sweden

  • *Contact author: garima.agrawalsk@gmail.com
  • †Now at Waaree Energies Limited, Mumbai, India
  • ‡These authors contributed equally to this work.

PRX Energy 4, 033001 – Published 10 July, 2025

DOI: https://doi.org/10.1103/t7ns-99dk

Abstract

Exploring the conduction mechanism in the chalcogenide perovskite BaZrS3 is of significant interest due to its potential suitability as a top absorber layer in silicon-based tandem solar cells and other optoelectronic applications. Theoretical and experimental studies anticipate native ambipolar doping in BaZrS3, although experimental validation remains limited. This study reveals a transition from highly insulating behavior to n-type conductivity (approximately 100 S/cm) in BaZrS3 thin films through annealing in an S-poor environment. BaZrS3 thin films are synthesized via a two-step process: co-sputtering of Ba-Zr followed by sulfurization at 600∘C, and subsequent annealing in high vacuum. Ultraviolet-visible spectroscopy measurements reveal a red shift of approximately 100 meV in the band gap concurrent with sample-color darkening after vacuum annealing. The increase in defect density from the order of 1017 to 1021cm−3 with vacuum annealing, coupled with the low activation energy (approximately 8 meV), and the n-type character of the defects, strongly suggests that sulfur vacancies (VS) are responsible for the n-type doping, in agreement with theoretical predictions. Temperature-dependent Hall measurement shows that phonon scattering governs charge transport at room temperature in BaZrS3 films and that S vacancies are shallow donor defects acting as a weak impurity metal. The shift of the valence-band maximum (VBM) with respect to the Fermi level, quantified by hard x-ray photoelectron spectroscopy (Ga Kα, 9.25 keV), further corroborates the induced n type of conductivity in annealed samples. Our findings indicate that vacuum annealing induces VS defects that dominate charge transport, resulting in n-type conductivity in BaZrS3 under S-poor conditions. These discoveries will inform important design choices, such as selecting appropriate contact materials, for integrating BaZrS3 into solar cell structures or other devices.

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