Growth Mechanisms of All-Vacuum Deposited (FA/Cs)SnI3 Perovskites via Sequential Evaporation
Joey Pu-Chou Lin a, Roland Scheer a, Paul Pistor b
a Martin-Luther-University Halle-Wittenberg, Institute of Physics, Germany, Halle 06099, Germany
b Center for Nanoscience and Sustainable Technologies (CNATS). Department of Physical, Chemical and Natural Systems, Universidad Pablo de Olavide, Sevilla, Spain
Proceedings of Perovskite Semiconductors: From Fundamental Properties to Devices (PerFunPro)
Konstanz, Germany, 2025 September 8th - 10th
Organizers: Lukas Schmidt-Mende, Vladimir Dyakonov and Selina Olthof
Poster, Joey Pu-Chou Lin, 042
Publication date: 16th July 2025

Lead-free tin halide perovskites, particularly formamidinium tin iodide (FASnI3) and cesium tin iodide (CsSnI3), represent a promising class of materials for sustainable photovoltaics due to their optimal bandgaps for tandem solar cell integration and their reduced environmental impact. The fabrication of uniform, compact, and defect-free thin films with precise stoichiometry is essential for achieving high device performance and long-term stability. Although solution-processing remains widely used at the laboratory scale, vacuum-based sequential physical vapor deposition (PVD) offers a solvent-free, industrially scalable alternative with superior control over film composition, thickness, and crystallization.

 

In this study, we investigate the growth dynamics of FASnI3 and CsSnI3 thin films via all-vacuum sequential deposition using in situ X-ray diffraction (XRD) to monitor real-time phase evolution during deposition and annealing. By comparing different precursor stacking orders, we explore how interdiffusion kinetics and crystallization behavior influence film morphology and stability.

 

For FASnI3, two sequential deposition routes—FAI/SnI2 and SnI2/FAI—were examined. In both cases, initial perovskite formation was detected during deposition at room temperature, indicating rapid interfacial reactivity. FAI emerged as the primary diffusing species since post-annealing morphology varied significantly. The FAI/SnI2 route producing perovskite at 160 °C exhibited notable voids and non-uniformity. In contrast, the SnI2/FAI route yielded dense, void-free films. From this difference, we conclude that FAI is the main diffusing species. Nonetheless, both configurations showed thermal degradation above 180 °C, revealing the intrinsic thermal instability of FASnI3.

 

For CsSnI3, sequential deposition routes of CsI/SnI2 and SnI2/CsI were studied. The CsI/SnI2 configuration required annealing above 100 °C to initiate 1:1:3 perovskite formation, but ultimately formed uniform, dense films upon annealing between 180–240 °C. The SnI2/CsI sequence, in contrast, led to immediate perovskite formation upon CsI deposition at room temperature but produced films with prominent cavities after annealing. These results confirm that here SnI2 is the main mobile species. Its inward diffusion into CsI yields controlled reaction fronts, whereas outward diffusion from SnI2 layers can lead to void formation. Additionally, both sequences transiently exhibited the Cs2SnI6 phase and decomposed thermally above 240 °C, reverting to CsI.

 

Our findings establish that precursor stacking order is a critical factor governing crystallization pathways, phase purity, and film quality in all-vacuum deposited tin perovskites. Optimal sequences—SnI2/FAI for FASnI3 and CsI/SnI2 for CsSnI3—minimize residual precursors and suppress morphological defects. Given the observed thermal vulnerabilities, we also studied Cs-alloying in FASnI3 and found complete mixed A-cation perovskite formation.

 

Keywords: halide perovskites, physical vapor deposition, in situ X-ray diffraction, formamidinium tin iodide, cesium tin iodide, diffusion model, perovskite solar cells.

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