结晶学
物理
兴奋剂
刚玉
材料科学
凝聚态物理
化学
冶金
作者
Mario Okawa,D. Takegami,Denise S. Christovam,Miguel Ferreira-Carvalho,Chang‐Yang Kuo,Chien‐Te Chen,T. Miyoshino,K. Takasu,Taichi Okuda,C. F. Chang,L. H. Tjeng,T. Mizokawa
出处
期刊:Physical review
[American Physical Society]
日期:2023-11-07
卷期号:108 (19)
标识
DOI:10.1103/physrevb.108.195108
摘要
Corundum oxide ${\mathrm{Ti}}_{2}{\mathrm{O}}_{3}$ shows the metal-insulator transition around 400--600 K accompanying the nearest ${\mathrm{Ti}}^{3+}\text{\ensuremath{-}}{\mathrm{Ti}}^{3+}$ bond (${a}_{1g}{a}_{1g}$ singlet state) formation along the $c$ axis. In order to clarify the hole-doping effect for the ${a}_{1g}{a}_{1g}$ singlet bond in ${\mathrm{Ti}}_{2}{\mathrm{O}}_{3}$, we investigated Ti $3d$ orbital anisotropy between corundum-type ${\mathrm{Ti}}_{2}{\mathrm{O}}_{3}$ and ilmenite-type ${\mathrm{MgTiO}}_{3}$ using linear dichroism of soft x-ray absorption spectroscopy of the Ti ${L}_{2,3}$ edge. From the linear dichroic spectral weight in ${\mathrm{Mg}}_{y}{\mathrm{Ti}}_{2\ensuremath{-}y}{\mathrm{O}}_{3}$, we confirmed that the ${a}_{1g}{a}_{1g}$ state is dominant not only in $y=0.01$ (almost ${\mathrm{Ti}}_{2}{\mathrm{O}}_{3}$), but also in $y=0.29$, indicating that the Ti-Ti bond survives against a certain level of hole doping. In $y=0.63$ corresponding to 46% hole doping per Ti, the $3d$ orbital symmetry changes from ${a}_{1g}$ to ${e}_{g}^{\ensuremath{\pi}}$.
科研通智能强力驱动
Strongly Powered by AbleSci AI