过渡金属Fe或Ag掺杂K2Ti6O13的电子结构和光学性质

本文利用基于密度泛函理论（DFT）的第一性原理计算研究了它们的电子结构和光学性质.光学性质的计算结果和实验相一致.结果表明，Fe或Ag掺杂后，K₂Ti₆O₁₃的带隙中出现了杂质带且其带隙值变小，因而使掺杂后的K₂Ti₆O₁₃的吸收边发生红移并实现了其对可见光吸收.其中杂质带主要由Fe 3d态或Ag 4d态与Ti 3d态和O 2p态杂化而成.对于Fe掺杂的K₂Ti₆O₁₃，杂质带位于带隙中间，因此可以作为电子从价带跃迁到导带的桥梁.对于Ag掺杂的K₂Ti₆O₁₃，杂质带位于价带顶附近为受主能级，可以降低光生载流子的复合概率.实验和计算研究表明，通过Fe或Ag的掺杂可以实现了K₂Ti₆O₁₃对可见光的吸收，这对进一步研究K₂Ti₆O₁₃的光学性质具有重要意义.

Electronic Structure and Optical Properties of K2Ti6O13 Doped with Transition Metal Fe or Ag

Based on the experimental study of the optical properties of K₂Ti₆O₁₃ doped with Fe or Ag, their electronic structures and optical properties are studied by the first-principles method based on the density functional theory (DFT). The calculated optical properties are consistent with the experiment results. K₂Ti₆O₁₃ doped with substitutional Fe or Ag has isolated impurity bands mainly stemming from the hybridization by the Fe 3d states or Ag 4d states with Ti 3d states and O 2p states and the band gap becomes narrower, the absorption edge of K₂Ti₆O₁₃ thus has a clear red shift and the absorption of visible light can be realized after doping. For Fe-doped K₂Ti₆O₁₃, the impurity bands are in the middle of the band gap, suggesting that they can be used as a bridge for valence band electrons transition to the conduction band. For Ag-doped K₂Ti₆O₁₃, the impurity bands form a shallow acceptor above the valence band and can reduce the recombination rate of photoexcited carriers. The experimental and calculated results are significant for the development of K₂Ti₆O₁₃ materials that have absorption under visible light.