{"title":"Composition-driven Mott transition within SrTi 1−x V x O3","authors":"A D N James, M Aichhorn, J Laverock","doi":"10.1088/2516-1075/ad29ab","DOIUrl":null,"url":null,"abstract":"The last few decades has seen the rapid growth of interest in the bulk perovskite-type transition metal oxides SrVO<sub>3</sub> and SrTiO<sub>3</sub>. The electronic configuration of these perovskites differs by one electron associated to the transition metal species which gives rise to the drastically different electronic properties. Therefore, it is natural to look into how the electronic structure transitions between these bulk structures by using doping. Measurements of the substitutional doped SrTi<inline-formula>\n<tex-math><?CDATA $_{{1-x}}$?></tex-math>\n<mml:math overflow=\"scroll\"><mml:msub><mml:mi> </mml:mi><mml:mrow><mml:mrow><mml:mn>1</mml:mn><mml:mo>−</mml:mo><mml:mi>x</mml:mi></mml:mrow></mml:mrow></mml:msub></mml:math>\n<inline-graphic xlink:href=\"estad29abieqn3.gif\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula>V<inline-formula>\n<tex-math><?CDATA $_{{{x}}}$?></tex-math>\n<mml:math overflow=\"scroll\"><mml:msub><mml:mi></mml:mi><mml:mrow><mml:mrow><mml:mrow><mml:mi>x</mml:mi></mml:mrow></mml:mrow></mml:mrow></mml:msub></mml:math>\n<inline-graphic xlink:href=\"estad29abieqn4.gif\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula>O<sub>3</sub> shows an metal–insulator transition (MIT) as a function of doping. By using supercell density functional theory with dynamical mean field theory (DFT+DMFT), we show that the MIT is indeed the result of the combination of local electron correlation effects (Mott physics) within the <inline-formula>\n<tex-math><?CDATA $t_{{\\mathrm{2g}}}$?></tex-math>\n<mml:math overflow=\"scroll\"><mml:msub><mml:mi>t</mml:mi><mml:mrow><mml:mrow><mml:mrow><mml:mn>2</mml:mn><mml:mi mathvariant=\"normal\">g</mml:mi></mml:mrow></mml:mrow></mml:mrow></mml:msub></mml:math>\n<inline-graphic xlink:href=\"estad29abieqn5.gif\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula> orbitals and the atomic site configuration of the transition metals which may indicate dependence on site disorder. SrTi<inline-formula>\n<tex-math><?CDATA $_{{1-x}}$?></tex-math>\n<mml:math overflow=\"scroll\"><mml:msub><mml:mi> </mml:mi><mml:mrow><mml:mrow><mml:mn>1</mml:mn><mml:mo>−</mml:mo><mml:mi>x</mml:mi></mml:mrow></mml:mrow></mml:msub></mml:math>\n<inline-graphic xlink:href=\"estad29abieqn6.gif\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula>V<inline-formula>\n<tex-math><?CDATA $_{{{x}}}$?></tex-math>\n<mml:math overflow=\"scroll\"><mml:msub><mml:mi></mml:mi><mml:mrow><mml:mrow><mml:mrow><mml:mi>x</mml:mi></mml:mrow></mml:mrow></mml:mrow></mml:msub></mml:math>\n<inline-graphic xlink:href=\"estad29abieqn7.gif\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula>O<sub>3</sub> may be an ideal candidate for benchmarking cutting-edge Mott–Anderson models of real systems. We show that applying an effective external perturbation on SrTi<inline-formula>\n<tex-math><?CDATA $_{{1-x}}$?></tex-math>\n<mml:math overflow=\"scroll\"><mml:msub><mml:mi> </mml:mi><mml:mrow><mml:mrow><mml:mn>1</mml:mn><mml:mo>−</mml:mo><mml:mi>x</mml:mi></mml:mrow></mml:mrow></mml:msub></mml:math>\n<inline-graphic xlink:href=\"estad29abieqn8.gif\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula>V<inline-formula>\n<tex-math><?CDATA $_{{{x}}}$?></tex-math>\n<mml:math overflow=\"scroll\"><mml:msub><mml:mi></mml:mi><mml:mrow><mml:mrow><mml:mrow><mml:mi>x</mml:mi></mml:mrow></mml:mrow></mml:mrow></mml:msub></mml:math>\n<inline-graphic xlink:href=\"estad29abieqn9.gif\" xlink:type=\"simple\"></inline-graphic>\n</inline-formula>O<sub>3</sub> can switch the system between the insulating and metallic phase, meaning this is a bulk system with the potential use in Mott electronic devices.","PeriodicalId":42419,"journal":{"name":"Electronic Structure","volume":null,"pages":null},"PeriodicalIF":2.9000,"publicationDate":"2024-03-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Electronic Structure","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1088/2516-1075/ad29ab","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"CHEMISTRY, PHYSICAL","Score":null,"Total":0}
引用次数: 0
Abstract
The last few decades has seen the rapid growth of interest in the bulk perovskite-type transition metal oxides SrVO3 and SrTiO3. The electronic configuration of these perovskites differs by one electron associated to the transition metal species which gives rise to the drastically different electronic properties. Therefore, it is natural to look into how the electronic structure transitions between these bulk structures by using doping. Measurements of the substitutional doped SrTi1−xVxO3 shows an metal–insulator transition (MIT) as a function of doping. By using supercell density functional theory with dynamical mean field theory (DFT+DMFT), we show that the MIT is indeed the result of the combination of local electron correlation effects (Mott physics) within the t2g orbitals and the atomic site configuration of the transition metals which may indicate dependence on site disorder. SrTi1−xVxO3 may be an ideal candidate for benchmarking cutting-edge Mott–Anderson models of real systems. We show that applying an effective external perturbation on SrTi1−xVxO3 can switch the system between the insulating and metallic phase, meaning this is a bulk system with the potential use in Mott electronic devices.