Author Affiliations
1College of Materials and Chemical Engineering, Hainan University, Haikou 570228, China2College of Materials Science and Engineering, Hunan University, Changsha 410082, Chinashow less
Fig. 1. The 2 × 2 × 1 supercell structure of various supercell models (the red, grey and blue balls represent O, Ti and Ce atoms, respectively; the imaginary red circle shows the position of oxygen vacancy): (a) Pure anatase TiO2; (b) Ce-TiO2; (c) OV-TiO2; (d) Ce/OV-TiO2.
2 × 2 × 1的超胞结构图(红色球为O, 灰色球为Ti, 蓝色球表示Ce原子的掺杂位置, 红色虚圆圈表示OV的位置) (a) Pure TiO2; (b) Ce-TiO2; (c) OV-TiO2; (d) Ce/OV-TiO2
Fig. 2. Band structure of anatase TiO2 before and after doping (the dashed lines represent the Fermi level, EF): (a) Pure TiO2; (b) Ce-doped TiO2; (c) OV-TiO2; (d) Ce/OV-TiO2.
纯TiO2和Ce/OV掺杂TiO2的能带结构图(图中虚线代表费米能级EF) (a) Pure TiO2; (b) Ce-TiO2; (c) OV-TiO2; (d) Ce/OV-TiO2
Fig. 3. Comparison of partial density of states of anatase TiO2 before and after doping (the dashed lines represent the Fermi level, EF): (a) Pure TiO2; (b) Ce-doped TiO2; (c) OV-TiO2; (d) Ce/OV-TiO2.
纯TiO2和Ce/OV掺杂TiO2的态密度图(图中虚线代表费米能级EF) (a) Pure TiO2; (b) Ce-TiO2; (c) OV-TiO2; (d) Ce/OV-TiO2
Fig. 4. Calculated band energy positions of pure TiO2, Ce-TiO2, OV-TiO2, Ce/OV-TiO2 (the energy scale is indicated by the normal hydrogen electrode in electron volts as a reference; the short thick lines and fine red lines represent the band energy positions of TiO2 by neglecting and considering the impurity levels, respectively).
Ce/OV掺杂锐钛矿相TiO2的能带带边位置示意图(图中各带边位置的电位均以NHE的电位为参考零点, 粗黑线代表忽略杂质能级时的带边位置, 细红线代表考虑杂质能级时的带边位置)
Fig. 5. Absorption spectra of pure and different doping TiO2 models (inset is the expanded absorption spectra in the visible region).
Ce/OV掺杂锐钛矿TiO2的光吸收谱(插图为可见光区光吸收谱的放大图)
参量 | GGA | GGA + U | LDA | LDA + U | Experiment | Theory | Error% | 注: dap, deq分别表示Ti—O长键和短键的键长; 误差指LDA + U方法相对于实验值的误差.
| a/nm
| 0.3791 | 0.3897 | 0.3745 | 0.3806 | 0.3785[26] | 0.3831[29] | 0.5548 | b/nm
| 0.3791 | 0.3897 | 0.3745 | 0.3806 | 0.3785[26] | 0.3831[29] | 0.5548 | c/nm
| 0.9805 | 0.9925 | 0.9447 | 0.9674 | 0.9514[26] | 0.9631[29] | 1.6817 | c/a | 2.5860 | 2.5470 | 2.5230 | 2.5410 | 2.5140[26] | 2.5140[29] | 1.0739 | u | 0.2050 | 0.2050 | 0.2080 | 0.2070 | — | 0.2050[29] | — | dap/nm
| 0.2011 | 0.2031 | 0.1966 | 0.2005 | 0.1980[27] | 0.1973[29] | 1.2626 | deq/nm
| 0.1946 | 0.2000 | 0.1914 | 0.1948 | 0.1934[28] | 0.1930[29] | 0.7238 | Eg/eV
| 2.18 | 3.18 | 2.16 | 3.12 | 3.32[24] | 3.23[29] | — |
|
Table 1. Lattice parameters and band gap width of pure anatase TiO2 calculated at the GGA, GGA + U, LDA and LDA + U levels of theory.
采用GGA, GGA + U, LDA及LDA + U方法计算得到的纯锐钛矿相TiO2的晶格参数和带隙宽度
参量 | Ce-TiO2 | | OV-TiO2 | | Ce/OV-TiO2 | This work | Experiment | Other theory | | This work | | This work | 注: dap, deq分别表示Ce-TiO2, Ce/OV-TiO2中Ce—O长键和短键的键长, 对于OV-TiO2则表示Ti—O长键和短键的平均键长.
| a/nm
| 0.3822 | 0.3789[25] | 0.3980[31] | | 0.3789 | | 0.3827 | b/nm
| 0.3833 | — | 0.3980[31] | | 0.3793 | | 0.3798 | c/nm
| 0.9956 | 0.9509[25] | 0.9757[31] | | 0.9824 | | 1.0090 | dap/nm
| 0.2225 | — | 0.2273[32] | | 0.2012 | | 0.2233 | deq/nm
| 0.2183 | — | 0.2119[32] | | 0.1946 | | 0.2252 |
|
Table 2. Lattice parameters of Ce/OV single and co-doped anatase TiO2 after the structure relaxation.
Ce/OV单(共)掺杂锐钛矿相TiO2弛豫后的晶胞参数
Model | Ef/eV
| | q/e
| p/Debye
| Ti-rich | O-rich | | O | Ti | Ce | Pure TiO2 | — | — | | −0.720 | 1.440 | — | 0.0000 | Ce-TiO2 | 10.42 | 1.16 | | −0.719 | 1.405 | 1.920 | 0.0168 | OV-TiO2 | 1.02 | 5.65 | | −0.727 | 1.412 | — | 0.0668 | Ce/OV-TiO2 | −15.84 | −20.48 | | −0.725 | 1.373 | 1.920 | 0.0251 |
|
Table 3. Defect formation energy, average net charges and average dipole moment of Ce/OV doped TiO2 supercell after the structure relaxation.
Ce/OV掺杂锐钛矿相TiO2的缺陷形成能(Ef)、平均净电荷(q)和平均偶极矩(p)