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Theoretical investigation on the promotion of second harmonic generation from chalcopyrite family A(I)GaS(2) to A(II)Ga(2)S(4)
The chalcopyrite structure is a rich source for the exploration of new IR materials. However, not all of the compounds with a chalcopyrite-type structure exhibit satisfactory optical properties, which may originate from their different microstructure features. In this work, we selected four classica...
Autores principales: | , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
The Royal Society of Chemistry
2019
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9076573/ https://www.ncbi.nlm.nih.gov/pubmed/35541577 http://dx.doi.org/10.1039/c9ra09109b |
Sumario: | The chalcopyrite structure is a rich source for the exploration of new IR materials. However, not all of the compounds with a chalcopyrite-type structure exhibit satisfactory optical properties, which may originate from their different microstructure features. In this work, we selected four classical chalcopyrite materials, A(I)GaS(2) (A(I) = Ag, Cu) with normal structures and A(II)Ga(2)S(4) (A(II) = Zn, Hg) with defect structures, to study their electronic structures, optical properties including the contribution of ions and ion groups to their band gaps, SHG responses and birefringences by the first-principles method. The results uncover that the different band gaps are mainly caused by the d orbitals of A* (A* = A(I), A(II))-site atoms and dp hybridizations between the A*-site and S atoms. In addition, the more powerful covalent bonds of A(II)–S and Ga–S in the A(II)Ga(2)S(4) lead to the larger SHG responses of ZnGa(2)S(4) and HgGa(2)S(4). For the birefringences, the sizes of the A*-site atoms make sense, namely larger size will lead to higher distortion of tetrahedra, then result in large birefringences. All the above analyses conclude that the A*-site atoms in the chalcopyrite structures play a modulation role in determining the optical properties. |
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