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High-Pressure Behavior and Disorder for Ag(2)ZnSnS(4) and Ag(2)CdSnS(4)
[Image: see text] We carried out first-principles calculations to simulate Ag(2)ZnSnS(4) and Ag(2)CdSnS(4) and calculated enthalpies of different plausible structural models (kesterite-type, stannite-type, wurtzkesterite-type, wurtzstannite-type, and GeSb-type) to identify low- and high-pressure pha...
Autores principales: | , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical Society
2021
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8529692/ https://www.ncbi.nlm.nih.gov/pubmed/34693159 http://dx.doi.org/10.1021/acsomega.1c04290 |
Sumario: | [Image: see text] We carried out first-principles calculations to simulate Ag(2)ZnSnS(4) and Ag(2)CdSnS(4) and calculated enthalpies of different plausible structural models (kesterite-type, stannite-type, wurtzkesterite-type, wurtzstannite-type, and GeSb-type) to identify low- and high-pressure phases. For Ag(2)ZnSnS(4), we predict the following transition: kesterite-type→[8.2GPa]→ GeSb-type. At the transition pressure, the electronic structure changes from semiconducting to metallic. For Ag(2)CdSnS(4), we cannot decide which of the experimentally observed structures (kesterite-type or wurtzkesterite-type) is the ground-state structure because their energy difference is too small. At 4.7 GPa, however, we predict a transition to the GeSb-type structure with metallic character for both structures. Regarding the sensitivity of the material to disorder, a major drawback for solar cell applications, Ag(2)CdSnS(4) behaves similar to Cu(2)ZnSnS(4), both showing a high tendency to cationic disorder. In contrast, the disordered structures in Ag(2)ZnSnS(4) are much higher in energy, and therefore, the material is less affected by disorder. |
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