M. Zaman , M.A. Rehman , I. Zeba , M. Shakil , S.S.A. Gillani
{"title":"压力影响下钙钛矿型TlSrF3光电性能的增强:DFT视角","authors":"M. Zaman , M.A. Rehman , I. Zeba , M. Shakil , S.S.A. Gillani","doi":"10.1016/j.cocom.2025.e01075","DOIUrl":null,"url":null,"abstract":"<div><div>This research aims to thoroughly assess TlSrF<sub>3</sub>'s mechanical, elastic, anisotropic, electronic, and optical properties between 0 GPa and 400 GPa of pressure. There is a drop in lattice parameters, but the structure remains cubic and no phase transition occurs by applying external pressure ranging from 0 to 400 GPa. Through arithematic computation of several mechanical and elastic characteristics, it is determined that the material is stable mechanically at different pressures except 0 GPa, 320 GPa, 360 GPa and 400 GPa. Poisson's ratio, Pugh/Frantsevich ratio, Kleinman's parameter and Cauchy pressure have all demonstrated the metallic bond nature, the material's elasticity and high-pressure persistence. Phonon dispersion curve confirms the dynamical stability of TlSrF<sub>3</sub> at 400 GPa. The elasticity, resistance to plastic deformation, anisotropy of elasticity and volume changes under pressure of metallic bonded materials are all determined by these parameters, which guarantee high-pressure persistence. Our material shows anisotropic behaviour at different anisotropy factors. When the electronic band structure (BS) is taken into account, from 0 to 40 GPa there is a minor increase in band gap from 4.229 eV to 4.254 eV. A shift from broad bandgap semiconductor (4.254 eV) to metal (0 eV) is observed from 40 GPa to 400 GPa. The electronic BS has been examined by the estimation of the partial, elemental and total densities of states, respectively. The real and imaginary conductivity, refractive index n(ω), extinction coefficient k(ω), loss function L(ω), absorption I(ω), reflectivity R(ω) and real/imaginary dielectric functions have been computed to emphasize the material's applicability further. As pressure is applied, the static values of <span><math><mrow><msub><mi>ε</mi><mn>1</mn></msub><mrow><mo>(</mo><mi>ω</mi><mo>)</mo></mrow></mrow></math></span> and n(ω) rise. This is an ideal material for UV filters since its absorbance spectra are in the UV area. Its excellent conductivity, reflectance, absorbance and refractive index make it an ideal element for optoelectronic devices.</div></div>","PeriodicalId":46322,"journal":{"name":"Computational Condensed Matter","volume":"44 ","pages":"Article e01075"},"PeriodicalIF":3.9000,"publicationDate":"2025-06-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Enhanced optoelectronic properties of perovskite type TlSrF3 under the influence of pressure: A DFT perspective\",\"authors\":\"M. Zaman , M.A. Rehman , I. Zeba , M. Shakil , S.S.A. Gillani\",\"doi\":\"10.1016/j.cocom.2025.e01075\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>This research aims to thoroughly assess TlSrF<sub>3</sub>'s mechanical, elastic, anisotropic, electronic, and optical properties between 0 GPa and 400 GPa of pressure. There is a drop in lattice parameters, but the structure remains cubic and no phase transition occurs by applying external pressure ranging from 0 to 400 GPa. Through arithematic computation of several mechanical and elastic characteristics, it is determined that the material is stable mechanically at different pressures except 0 GPa, 320 GPa, 360 GPa and 400 GPa. Poisson's ratio, Pugh/Frantsevich ratio, Kleinman's parameter and Cauchy pressure have all demonstrated the metallic bond nature, the material's elasticity and high-pressure persistence. Phonon dispersion curve confirms the dynamical stability of TlSrF<sub>3</sub> at 400 GPa. The elasticity, resistance to plastic deformation, anisotropy of elasticity and volume changes under pressure of metallic bonded materials are all determined by these parameters, which guarantee high-pressure persistence. Our material shows anisotropic behaviour at different anisotropy factors. When the electronic band structure (BS) is taken into account, from 0 to 40 GPa there is a minor increase in band gap from 4.229 eV to 4.254 eV. A shift from broad bandgap semiconductor (4.254 eV) to metal (0 eV) is observed from 40 GPa to 400 GPa. The electronic BS has been examined by the estimation of the partial, elemental and total densities of states, respectively. The real and imaginary conductivity, refractive index n(ω), extinction coefficient k(ω), loss function L(ω), absorption I(ω), reflectivity R(ω) and real/imaginary dielectric functions have been computed to emphasize the material's applicability further. As pressure is applied, the static values of <span><math><mrow><msub><mi>ε</mi><mn>1</mn></msub><mrow><mo>(</mo><mi>ω</mi><mo>)</mo></mrow></mrow></math></span> and n(ω) rise. This is an ideal material for UV filters since its absorbance spectra are in the UV area. Its excellent conductivity, reflectance, absorbance and refractive index make it an ideal element for optoelectronic devices.</div></div>\",\"PeriodicalId\":46322,\"journal\":{\"name\":\"Computational Condensed Matter\",\"volume\":\"44 \",\"pages\":\"Article e01075\"},\"PeriodicalIF\":3.9000,\"publicationDate\":\"2025-06-06\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Computational Condensed Matter\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S2352214325000747\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"PHYSICS, CONDENSED MATTER\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Computational Condensed Matter","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S2352214325000747","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"PHYSICS, CONDENSED MATTER","Score":null,"Total":0}
Enhanced optoelectronic properties of perovskite type TlSrF3 under the influence of pressure: A DFT perspective
This research aims to thoroughly assess TlSrF3's mechanical, elastic, anisotropic, electronic, and optical properties between 0 GPa and 400 GPa of pressure. There is a drop in lattice parameters, but the structure remains cubic and no phase transition occurs by applying external pressure ranging from 0 to 400 GPa. Through arithematic computation of several mechanical and elastic characteristics, it is determined that the material is stable mechanically at different pressures except 0 GPa, 320 GPa, 360 GPa and 400 GPa. Poisson's ratio, Pugh/Frantsevich ratio, Kleinman's parameter and Cauchy pressure have all demonstrated the metallic bond nature, the material's elasticity and high-pressure persistence. Phonon dispersion curve confirms the dynamical stability of TlSrF3 at 400 GPa. The elasticity, resistance to plastic deformation, anisotropy of elasticity and volume changes under pressure of metallic bonded materials are all determined by these parameters, which guarantee high-pressure persistence. Our material shows anisotropic behaviour at different anisotropy factors. When the electronic band structure (BS) is taken into account, from 0 to 40 GPa there is a minor increase in band gap from 4.229 eV to 4.254 eV. A shift from broad bandgap semiconductor (4.254 eV) to metal (0 eV) is observed from 40 GPa to 400 GPa. The electronic BS has been examined by the estimation of the partial, elemental and total densities of states, respectively. The real and imaginary conductivity, refractive index n(ω), extinction coefficient k(ω), loss function L(ω), absorption I(ω), reflectivity R(ω) and real/imaginary dielectric functions have been computed to emphasize the material's applicability further. As pressure is applied, the static values of and n(ω) rise. This is an ideal material for UV filters since its absorbance spectra are in the UV area. Its excellent conductivity, reflectance, absorbance and refractive index make it an ideal element for optoelectronic devices.