Assignment for Vibrational Spectra of BaTiO3 Ferroelectric Ceramic Based on the First-Principles Calculation

被引:33
作者
An Wei [1 ]
Liu Tian-Hui [2 ,3 ]
Wang Chun-Hai [2 ]
Diao Chuan-Ling [2 ]
Luo Neng-Neng [2 ]
Liu Yong [2 ,3 ]
Qi Ze-Ming [4 ]
Shao Tao [4 ]
Wang Yu-Yin [4 ]
Jiao Huan [3 ]
Tian Guang-Shan [1 ]
Jing Xi-Ping [2 ]
机构
[1] Peking Univ, Sch Phys, Beijing 100871, Peoples R China
[2] Peking Univ, Coll Chem & Mol Engn, State Key Lab Rare Earth Mat Chem & Applicat, Beijing 100871, Peoples R China
[3] Shaanxi Normal Univ, Coll Chem & Chem Engn, Key Lab Macromol Sci Shaanxi Prov, Xian 710119, Peoples R China
[4] Univ Sci & Technol China, Natl Synchrotron Radiat Lab, Hefei 230029, Peoples R China
基金
中国国家自然科学基金;
关键词
First-principles calculation; Raman mode; IR mode; Dielectric property; INFRARED REFLECTION SPECTRA; MICROWAVE DIELECTRIC-PROPERTIES; TEMPERATURE-DEPENDENCE; BARIUM-TITANATE; RAMAN; PARTICLES; MODES; SPECTROSCOPY;
D O I
10.3866/PKU.WHXB201504144
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
A BaTiO3 ceramic was synthesized using a conventional solid-state reaction, and sintered at 1400 degrees C for 4 h. The pure tetragonal phase was confirmed by Rietveld refinement of the X-ray diffraction data. The Raman spectrum and the far infrared (FIR) reflective spectrum were obtained and analyzed using Lorentz fitting and the four-parameter semi-quantum model fitting, respectively. The Raman and FIR spectra were assigned based on first-principles calculations, and consideration of the splitting of the transverse optical modes and longitudinal optical modes. All the vibrational modes were represented by linear combinations of the symmetry coordinates deduced by group theory analysis. Among the 12 optical modes, the Raman-active-only mode, B-1, can be viewed as the wing-flapping vibration of the O4-O5 plane perpendicular to the z-axis in the O-6 octahedron. The A(1)((1)) mode and the E-(1) soft mode are split by the triply degenerate F-1u mode of cubic BaTiO3, resulting in the ferroelectric property of tetragonal BaTiO3. The appearance of the A(1)((1)) mode leads to crystal polarization along the z-axis and the E-(1) mode causes the large permittivity. These two modes can be described as vibration of the Ti atom against the O-6 octahedral cage along the z-axis [A(1)((1))] and on the xy-plane [E-(1)].
引用
收藏
页码:1059 / 1068
页数:10
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