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二氧化钛(TiO2)作为一种性能优良的光催化剂已经受到越来越多的关注. 本研究采用密度泛函理论的第一性原理和广义梯度近似+U方法,对锐钛矿结构TiO2晶体三种可能的(Nb, N) 共掺杂TiO2的几何结构、形成能、能带结构、电子密度和光吸收系数进行了研究, 并与单掺杂(Nb/N)体系进行了对比.对掺杂后体系的几何结构进行的计算表明杂质原子掺入后晶格发生了不同程度的畸变.此外, (Nb, N)共掺杂体系与纯TiO2相比,其禁带宽度和吸收边较小.同时,与N掺杂TiO2相比, N的2p态在共掺杂情形下变为完全占据, 从而减少了电子空穴对的复合.而且共掺杂体系的形成能比N单掺杂体系低,因而更加稳定. 因此, (Nb, N)共掺杂可以很好地提升锐钛矿型TiO2在可见光波段的光催化性能.Titanium dioxide (TiO2), as a kind of excellent photocatalyst, has been widely researched and applied. The geometry structures, band structures, densities of states and absorption coefficients of three possible (Nb, N) co-doped anatase are studied by the density functional theory based on GGA+U method, and the results are compared with those of the single doped (Nb/N) anatase. It is shown that the introduction of dopants leads to the lattice distortion. Besides, compared with undoped TiO2, (Nb, N) co-doped TiO2 has small band gap and absorption edge, and the level of N 2p state changes from partially occupied to occupied, which reduces the recombination of electron-hole pairs. In addition, the smaller formation energy of co-doped anatase indicates that it is more stable than the N doped anatase. Therefore, (Nb, N) co-doping anatase is a kind of stable photocatalyst and it has better photocatalytic performance in visible light band than pure TiO2.
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Keywords:
- electronic structure /
- density functional theory /
- anatase /
- co-doped
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[1] Fujishima A, Honda K 1972 Nature 238 37
[2] Fujishima A, Rao T N 2000 J. Photoch Photobio C 1 1
[3] Diebold U 2003 Surf. Sci. Rep. 48 53
[4] Asahi R, Morikawa T, Ohwaki T, Aoki K, Taga Y 2001 Science 293 269
[5] Livraghi S, Chierotti M R, Giamello E, Magnacca G, Paganini M C, Cappelletti G, Bianchi C L 2008 J. Phys. Chem. C 112 17244
[6] Sun H, Bai Y, Jin W, Xu N 2008 Sol. Energy Mater. Sol. Cells 92 76
[7] Hu S, Wang A, Li X, Lowe H 2010 J. Phys. Chem. Solids 71 156
[8] Yin Y, Zhang W, Chen S, Yu S 2009 Mater. Chem. Phys. 113 982
[9] Mi L, Zhang Y, Wang P N 2008 Chem. Phys. Lett. 458 341
[10] Chen X, Burda C 2008 J. Am. Chem. Soc. 130 5018
[11] Stengl V, Bakardjieva S 2010 J. Phys. Chem. C 114 19308
[12] Kurtoglu M E, Longenbach T, Sohlberg K, Gogotsi Y 2011 J. Phys. Chem. C 115 17392
[13] Zhu W, Qiu X, Iancu V, Chen X Q, Pan H, Wang W, Dimitrijevic N M, Rajh T, Meyer III H M, Paranthaman M P, Stocks G M, Weitering H H, Gu B, Eres G, Zhang Z 2009 Phys. Rev. Lett. 103 226401
[14] Long R, English N J 2010 Chem. Mater. 22 1616
[15] Khan M, Xu J, Chen N, Cao W 2012 J. Alloys Compd. 513 539
[16] Liu X D, Jiang E Y, Li Z Q, Song Q G 2008 Appl. Phys. Lett. 92 252104
[17] Furubayashi Y, Hitosugi T, Yamamoto Y, Inaba K, Kinoda G, Hirose Y, Shimada T, Hasegawa T 2005 Appl. Phys. Lett. 86 252101
[18] Furubayashi Y, Hitosugi T, Hasegawa T 2006 Appl. Phys. Lett. 88 226103
[19] Zhang S X, Kundaliya D C, Yi W, Dhar S, Young S Y, Salamanca-Riba L G, Ogale S B, Vispute R D, Venkatesan T 2007 J. Appl. Phys. 102 013701
[20] Kresse G, Furthmüller J 1996 Phys. Rev. B 54 11
[21] Yang K, Dai Y, Huang B 2008 Chem. Phys. Lett. 456 71
[22] Anisimov V I, Aryasetiawan F, Lichtenstein A I 1997 J. Phys. Condens. Matter 9 767
[23] Zhang S B 2002 J. Phys. Condens. Matter 14 881
[24] Sun J, Wang H T, He J, Tian Y 2005 Phys. Rev. B 71 125132
[25] Burdett J K, Hughbanks T, Miller G J, Richardson J W, Smith J V 1987 J. Am. Chem. Soc. 109 3639
[26] Czoska A M, Livraghi S, Chiesa M, Giamello E, Agnoli S, Granozzi G, Finazzi E, Valentin C D, Pacchioni G 2008 J. Phys. Chem. C 112 8951
[27] Zhang S X, Kundaliya D C, Yi W, Dhar S, Young S Y, Salamanca-Riba L G, Ogale S B, Vispute R D, Venkatesan T 2007 J. Appl. Phys. 102 013701
[28] Irie H, Watanabe Y, Hashimoto K 2003 J. Phys. Chem. B 107 5483
[29] Valentin C D, Pacchioni G, Selloni A, Livraghi S, Giamello E 2005 J. Phys. Chem. B 109 11414
[30] Valentin C D, Finazzi E, Pacchioni G, Selloni A, Livraghi S, Paganini M C, Giamello E 2007 Chem. Phys. 339 44
[31] Nakano Y, Morikawa T, Ohwaki T 2005 Appl. Phys. Lett. 86 132104
[32] Shi W, Chen Q, Xu Y, Wu D, Huo C 2011 Appl. Surf. Sci. 257 3000
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