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arXiv 0811.4404cond-mat.str-el
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YTiO_3中偶极激活光学声子的椭圆偏振研究和晶格动力学计算

Dipole-active optical phonons in YTiO_3: ellipsometry study and lattice-dynamics calculations

N. N. Kovaleva, A. V. Boris, L. Capogna, J. L. Gavartin, P. Popovich, P. Yordanov, A. Maljuk, A. M. Stoneham, B. Keimer

摘要:

利用椭圆偏振光谱法对正交晶系(Pbnm)YTiO_3单晶的三个主晶向进行了声子频率测量,准确地提取了各向异性复介电响应。我们确定了所有25个红外激活声子模式允许对称性,7B_1u,9B_2u和9B_3u,沿c-,b-和a-轴,分别极化。从复介电函数\tilde ε(ω)及其逆-1/ \tilde ε(ω)的经典色散分析中,我们定义了横向(TO)和纵向(LO)声子模的谐振频率、宽度和振子强度。我们计算了B_1u、B_2u和B_3u简正模的本征频率和本征矢量,并通过比较它们的频率和振子强度与目前晶格动力学研究的结果,建议了在我们的椭圆偏振光谱中观察到的TO声子模的归属。在此基础上,我们估算了YTiO_3晶格中原子的动态有效电荷。我们发现,在一般情况下,YTiO_3晶格中的动态有效电荷是典型的钙钛矿氧化物家族。与铁电BaTiO_3相比,氧的动态有效电荷与沿c轴的位移有关,并没有显示出异常大的值。同时,Y和ab面氧的动态有效电荷表现出各向异性,表明沿a轴的强杂化。

英文摘要:

The anisotropic complex dielectric response was accurately extracted from spectroscopic ellipsometry measurements at phonon frequencies for the three principal crystallographic directions of an orthorhombic (Pbnm) YTiO_3 single crystal. We identify all twenty five infrared-active phonon modes allowed by symmetry, 7B_1u, 9B_2u, and 9B_3u, polarized along the c-, b-, and a-axis, respectively. From a classical dispersion analysis of the complex dielectric functions \tildeε(ω) and their inverses -1/\tildeε(ω) we define the resonant frequencies, widths, and oscillator strengths of the transverse (TO) and longitudinal (LO) phonon modes. We calculate eigenfrequencies and eigenvectors of B_1u, B_2u, and B_3u normal modes and suggest assignments of the TO phonon modes observed in our ellipsometry spectra by comparing their frequencies and oscillator strengths with those resulting from the present lattice-dynamics study. Based on these assignments, we estimate dynamical effective charges of the atoms in the YTiO_3 lattice. We find that, in general, the dynamical effective charges in YTiO_3 lattice are typical for a family of perovskite oxides. By contrast to a ferroelectric BaTiO_3, the dynamical effective charge of oxygen related to a displacement along the c-axis does not show the anomalously large value. At the same time, the dynamical effective charges of Y and ab-plane oxygen exhibit anisotropy, indicating strong hybridization along the a-axis.

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