This study examines the specific characteristics of Raman scattering observed in ZnSnN2 samples produced via magnetron co-sputtering. The spectra demonstrate a high degree of similarity to the phonon density of states. This phenomenon is caused by the presence of SnZn substitutional defects, which disrupt the ideal crystal structure and generate so-called defect-induced Raman modes across the entire first Brillouin zone. An increase in the elemental content of Sn leads to a decrease in the intensity of the 230 cm⁻1 and 660 cm⁻1 peaks and to their broadening. This suggests an intensification of the disorder within the cation sublattice. Following annealing at 450 °C in a vacuum, an increase in the intensity of the peaks at 450 cm⁻1 and 560 cm⁻1, as well as the Boson peak, was observed. We attribute these changes to the increased formation of Zn–N–Sn bonds within the film structure due to the ordering of the anion (nitrogen) sublattice. However, zinc and tin atoms still occupy random positions in their sublattices, contributing to the overall increase in structural disorder.

Raman spectroscopy study of disorder in cation sublattice of nonstoichiometric and annealed ZnSnN2

Baratta M.;De Filpo G.;
2024-01-01

Abstract

This study examines the specific characteristics of Raman scattering observed in ZnSnN2 samples produced via magnetron co-sputtering. The spectra demonstrate a high degree of similarity to the phonon density of states. This phenomenon is caused by the presence of SnZn substitutional defects, which disrupt the ideal crystal structure and generate so-called defect-induced Raman modes across the entire first Brillouin zone. An increase in the elemental content of Sn leads to a decrease in the intensity of the 230 cm⁻1 and 660 cm⁻1 peaks and to their broadening. This suggests an intensification of the disorder within the cation sublattice. Following annealing at 450 °C in a vacuum, an increase in the intensity of the peaks at 450 cm⁻1 and 560 cm⁻1, as well as the Boson peak, was observed. We attribute these changes to the increased formation of Zn–N–Sn bonds within the film structure due to the ordering of the anion (nitrogen) sublattice. However, zinc and tin atoms still occupy random positions in their sublattices, contributing to the overall increase in structural disorder.
2024
Charge carrier density
Defect-induced Raman scattering
Disorder
Raman spectroscopy
Solar cell
Substitutional defects
Zinc tin nitride
File in questo prodotto:
Non ci sono file associati a questo prodotto.

I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.

Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.11770/377618
 Attenzione

Attenzione! I dati visualizzati non sono stati sottoposti a validazione da parte dell'ateneo

Citazioni
  • ???jsp.display-item.citation.pmc??? ND
  • Scopus 0
  • ???jsp.display-item.citation.isi??? 0
social impact