Abstract

Tin-based perovskite material is the best choice to replace heavy metal element lead during the last several years. Cs2SnI6 with Sn4+ is a fascinating optoelectronic material, which is a more air-stable composite cesium tin halide peroxide variant from CsSnI3. However, the optoelectronic performance between N and P type of Cs2SnI6 varies considerably. Herein, we synthesized uniform Cs2SnI6 by modified two-step method, which thermal evaporated CsI firstly, and followed annealing in the SnI4 and I2 vapor at 150 °C resulted in uniform Cs2SnI6 films. SnF4 is used as a dopant source to improve the optoelectronic properties of Cs2SnI6 films. Results indicate that good crystallinity was obtained for all films and the doped films underwent a crystalline plane meritocracy transition. The doped films had a flat, non-porous morphology with large grains. The high transmittance of the doped films in the infrared region led to the avoidance of self-generated thermal decomposition. With the help of F−, the films became more conductive and had higher carrier mobility. DFT calculations showed that doping with F reduced the surface energy of (004), resulted in a preferred orientation transition in the crystal of Cs2SnI6. Fluorine doped double layer perovskite materials would have a broader application prospect.

Highlights

  • Tin-based perovskite material is the best choice to replace heavy metal element lead during the last several years. ­Cs2SnI6 with ­Sn4+ is a fascinating optoelectronic material, which is a more air-stable composite cesium tin halide peroxide variant from ­CsSnI3

  • We found C­ s2SnI6 is a more air-stable composite cesium tin halide peroxide variant from C­ sSnI36

  • Regarding the preferred orientation transition, it may be related to the change of the crystal plane energy and surface energy by the doping of F­ −

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Summary

Introduction

Tin-based perovskite material is the best choice to replace heavy metal element lead during the last several years. ­Cs2SnI6 with ­Sn4+ is a fascinating optoelectronic material, which is a more air-stable composite cesium tin halide peroxide variant from ­CsSnI3. The structure and properties of ­Cs2SnI6 thin films with the amount of doping were observed, measured, and analyzed the influence of ­F− doping. The peak at 23.9748° was attributed to ­Cs2SnF6 phase (011) plane (PDF #070-0141) in F doped films.

Results
Conclusion

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