JPhys Energy (Jan 2023)

Elucidating the local structure of V substitutes in In2S3 as potential intermediate band material by x-ray absorption spectroscopy and first principles calculations

  • Elaheh Ghorbani,
  • Martin Schiller,
  • Hans H Falk,
  • Leonard A Wägele,
  • Stefanie Eckner,
  • Francesco d’Acapito,
  • Roland Scheer,
  • Karsten Albe,
  • Claudia S Schnohr

DOI
https://doi.org/10.1088/2515-7655/acd95b
Journal volume & issue
Vol. 5, no. 3
p. 035003

Abstract

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Vanadium doped indium sulphide, In _2 S _3 :V, is studied as a potential absorber material for intermediate band (IB) solar cells. Based on electronic considerations, it is usually assumed that V occupies octahedrally coordinated In sites, although geometrical considerations would favour tetrahedral In sites. In this study, we therefore combined experimental x-ray diffraction and x-ray absorption spectroscopy with ab initio theoretical calculations of both $\mathrm{\alpha}$ and $\mathrm{\beta}$ phase to elucidate the incorporation of V in In _2 S _3 :V thin films grown with different V content and different growth temperatures. Comparing shape and position of the measured and calculated x-ray absorption edge of V, comparing experimentally determined and calculated V–S bond lengths, and evaluating the calculated heat of solution of V on different lattice sites all indicate that V is incorporated on octahedral rather than tetrahedral sites in the In _2 S _3 matrix. For this material system, the electronic benefit of octahedral coordination thus outweighs the mechanical stress of the associated lattice relaxation. Finally, we studied the electronic structure of V-substituted $\mathrm{\alpha}$ - $\mathrm{In_2S_3}$ using hybrid density functional calculations and find that for a concentration of 1.9 at %, V on octahedrally coordinated In sites forms an empty IB isolated from valence band and conduction band (CB). By increasing the V content to 3.8 at %, however, the gap between IB and CB closes, which results in a reduction of the band gap. This differs from the electronic structure calculated for $\mathrm{\beta}$ - $\mathrm{In_2S_3}$ :V and clearly demonstrates that both crystal structure and V incorporation site affect the resulting electronic material properties.

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