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采用基于密度泛函理论(DFT)的第一性原理计算研究了 (Ba0.5Sr0.5)TiO3 (BST) 晶体在高压下的电子结构及能带变化行为. 研究结果发现,随着压强的增加,BST能带间隙先增加,在压强为55 GPa时达到最大值,然后减小,这些有趣的结果将有助于开发与设计新的BST铁电器件. 进一步地,通过电子态密度和密度分布图的研究分析可知:在低压区域(0P55 GPa),带隙的增加是由于费米能级附近导带反键态的形成和价带成键态的形成共同作用的结果. 在高压区域(P55 GPa),则是出现的离域现象占主导(电子的离域作用超过键态的作用),从而使带隙减小.The high-pressure behaviors of crystalline (Ba0.5Sr0.5)TiO3 (BST) are investigated, using the first-principles calculations based on the density functional theory. The results show that as pressure increases, the band gap of BST first increases and peaks at around 55 GPa, and then gradually decreases. The analysis of density of states shows that in the low-pressure region (0P55 GPa), the increase in band gap is due to the formation of anti-bonding states and bonding states in the conduction band and valence band, respectively. In the high-pressure region (P55 GPa), the delocalization phenomenon in dominant due to the fact that the delocaligation action exceeds the force of bonding state and anti-bonding state, which results in the decrease of the band gap.
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Keywords:
- (Ba0.5Sr0.5)TiO3 (BST) /
- high-pressure /
- first-principle /
- band gap
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[1] Akbas M A, Davies P K 1998 J. Am. Ceram. Soc. 81 670
[2] [3] Walizer L, Lisenkov S, Bellaiche L 2006 Phys. Rev. B 73 144105
[4] Bao P, Jackson T J, Wang X, Lancaster M J 2008 J. Phys. D-Appl. Phys. 41 063001
[5] [6] Ma Y M, Eremets M, Oganov A R, Xie Y, Trojan I, Medvedev S, Lyakhov A O, Valle M, Prakapenka V 2009 Nature 458 182
[7] [8] Guennou M, Bouvier P, Kreisel J, Machon D 2010 Phys. Rev. B 81 134101
[9] [10] [11] Ganesh P, Cohen R E 2009 J. Phys. Condes. Matter 21 064225
[12] Stengel M, Vanderbilt D, Spaldin N A 2009 Nat. Mater. 8 392
[13] [14] He J P, Lu W Z, Wang X H 2009 Ferroelectrics 388 172
[15] [16] Zhu W H, Xiao H M 2010 Struct. Chem. 21 657
[17] [18] [19] Zhu W H, Zhang X W, Zhu W, Xiao H M 2008 Phys. Chem. Chem. Phys. 10 7318
[20] [21] Zhu J L, Jin C Q, Cao W W, Wang X H 2008 Appl. Phys. Lett. 92 242901
[22] [23] Tse J S, Klug D D, Patchkovskii S, Ma Y M, Dewhurst J K 2006 J. Phys. Chem. B 110 3721
[24] Lemanov V V, Smirnova E P, Syrnikov P P, Tarakanov E A 1996 Phys. Rev. B 54 3151
[25] [26] [27] Menoret C, Kiat J M, Dkhil B, Dunlop M, Dammak H, Hernandez O 2002 Phys. Rev. B 65 224104
[28] [29] Ostapchuk T, Petzelt J, Hlinka J, Bovtun V, Kuzel P, Ponomareva I, Lisenkov S, Bellaiche L, Tkach A, Vilarinho P 2009 J. Phys. Condes. Matter 21 474215
[30] Wang Y X 2005 Solid State Commun. 135 290
[31] [32] Wang Y X 2008 Phys. Status Solidi B-Basic Solid State Phys. 245 1147
[33] [34] [35] Guennou M, Bouvier P, Krikler B, Kreisel J, Haumont R, Garbarino G 2010 Phys. Rev. B 82 054115
[36] Yang L, Ma Y M, Iitaka T, Tse J S, Stahl K, Ohishi Y, Wang Y, Zhang R W, Liu J F, Mao H K, Jiang J Z 2006 Phys. Rev. B 74 245209
[37] [38] [39] Xiao W S, Tan D Y, Xiong X L, Liu J, Xu J A 2010 Proc. Natl. Acad. Sci. USA 107 14026
[40] [41] Kresse G, Furthmuller J 1996 Phys. Rev. B 54 11169
[42] Vanderbilt D 1990 Phys. Rev. B 41 7892
[43] [44] Perdew J P, Burke K, Ernzerhof M 1996 Phys. Rev. Lett. 77 3865
[45] [46] Ceperley D M, Alder B J 1980 Phys. Rev. Lett. 45 566
[47] [48] Seo S S A, Lee H N 2009 Appl. Phys. Lett. 94 232904
[49] [50] Johnston K, Huang X Y, Neaton J B, Rabe K M 2005 Phys. Rev. B 71 100103
[51] [52] Jia C H, Chen Y H, Zhou X L, Yang A L, Zheng G L, Liu X L, Yang S Y, Wang Z G 2010 Appl. Phys. A-Mater. Sci. Process. 99 511
[53] [54] Wang J, Xiang J H, Duo S W, Li W K, Li M S, Bai L Y 2009 J. Mater. Sci. Mater. Electron. 20 319
[55] [56] [57] Chen W K, Cheng C M, Huang J Y, Hsieh W F, Tseng T Y 2000 J. Phys. Chem. Solids 61 969
[58] [59] Cohen R E 1992 Nature 358 136
[60] [61] Zhu W, Zhang X, Xiao H 2008 Phys. Chem. Chem. Phys. 10 7318
[62] Blochl P E 1994 Phys. Rev. B 50 17953
[63] [64] Wei X, Xu G, Ren Z H, Wang Y G, Shen G, Han G R 2008 J. Cryst. Growth 310 4132
[65] [66] [67] Todorova M, Reuter K, Scheffler M 2004 J. Phys. Chem. B 108 14477
[68] [69] Morgan B J, Watson G W 2010 J. Phys. Chem. C 114 2321
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