Dec 4, 2024
9:30am - 9:45am
Sheraton, Third Floor, Huntington
Himani Mishra1,Shuxiang Zhou1,Linu Malakkal1,Amey Khanolkar1,David Hurley1,Marat Khafizov2
Idaho National Laboratory1,The Ohio State University2
Himani Mishra1,Shuxiang Zhou1,Linu Malakkal1,Amey Khanolkar1,David Hurley1,Marat Khafizov2
Idaho National Laboratory1,The Ohio State University2
Experiments suggest that ThO<sub>2</sub> is an optical insulator with a bandgap between 5.0-6.0 eV and the introduction of oxygen vacancy results in an emergence of new optical absorption peak in the visible region of the electromagnetic spectrum. Using a fully ab-initio methodology, we demonstrate how oxygen vacancies effect opto-electronic properties of ThO<sub>2</sub>. The bare energies were calculated using density functional theory, whereas G<sub>0</sub>W<sub>0</sub> many-body perturbation theory was utilized to extract the excited-state energies. A coupled electron-hole Bethe-Salpeter equation (BSE) was solved with quasi-particle correction from G<sub>0</sub>W<sub>0 </sub>calculation revealing the optical signatures of both pristine ThO<sub>2 </sub>and ThO<sub>2 </sub>containing oxygen vacancies at two different concentrations. Our G<sub>0</sub>W<sub>0 </sub>calculations reveal that oxygen vacancy at concentration of 1.6 at% reduces the bandgap from 6.6 eV for pristine ThO<sub>2 </sub>to 1.06 eV. Consequently, the optical response changes, showing emergence of a new peak at 1.0 eV in the presence of oxygen vacancies, compared to 4.54 eV peak observed in pristine ThO<sub>2</sub> which aligns well with the experimental observations. Furthermore, we investigated the neutral and charged vacancies (+2 charge) within ThO<sub>2</sub> in the G<sub>0</sub>W<sub>0 </sub>+ BSE framework. This comprehensive study of the excited state physics provides valuable insights in to defect physics within ThO<sub>2</sub> and serves as a platform for tuning opto-electronic and transport properties in these materials.