Chemistry and Physics of Materials Unit, Jawaharlal Nehru Centre for Advanced Scientific Research, Jakkur PO, Bangalore-560064, India.
J Phys Condens Matter. 2013 Aug 28;25(34):345901. doi: 10.1088/0953-8984/25/34/345901.
BaTiO3, with both nitrogen and fluorine substituted for oxygen, has been prepared and the properties of the doped material with the composition BaTiO2:8N0:1F0:1 have been studied. The color of the sample changes to light green on doping, accompanying a broad visible absorption band with its edge at 2.5 eV. The first-order ferroelectric transition changes to a broad transition on doping along with a decrease in the dielectric constant. We have examined the local structure, electronic structure and polar lattice dynamical properties of N and F co-substituted BaTiO3 using first-principles density functional theory-based calculations and derived the mechanism of the diffuse ferroelectric transition observed here with a broad peak in the temperature-dependent dielectric response. The calculated Born charges clearly reveal a strong disparity in the interaction of N, O and F with Ti: N being the most ferro-active, with a highly anomalous charge, and F being the least active, with an almost nominal charge. This originates from an electronic structure in which the top-most valence band is constituted of the 2p states of N, while the electronic states of F lie deep in the energy band, resulting in a local structure with short covalent Ti–N and long ionic Ti–F bonds. Disorder in these hetero ferro-active anions leads to a relaxor-like diffuse phase transition and a reduction in polarization. Calculations confirm the reduction of 0.65 eV in the bandgap of BaTiO3, which changes from indirect to direct type.
BaTiO3 中的氧被氮和氟取代,已经制备出这种掺杂材料,其组成是 BaTiO2:8N0:1F0:1。掺杂后,样品的颜色变为浅绿色,同时出现一个宽的可见吸收带,其边缘在 2.5 eV 处。一级铁电相变在掺杂后转变为宽转变,介电常数降低。我们使用基于第一性原理密度泛函理论的计算方法研究了 N 和 F 共取代 BaTiO3 的局域结构、电子结构和极性晶格动力学性质,并从温度相关介电响应的宽峰中得出了观察到的弥散铁电转变的机制。计算得到的 Born 电荷清楚地表明,N、O 和 F 与 Ti 的相互作用存在很大差异:N 是最具铁活性的,具有非常反常的电荷,而 F 是最不活跃的,几乎具有标称电荷。这源于电子结构,其中最上面的价带由 N 的 2p 态构成,而 F 的电子态位于能带深处,导致具有短共价 Ti-N 和长离子 Ti-F 键的局域结构。这些杂 ferro 活性阴离子的无序导致弛豫型弥散相变和极化的降低。计算证实 BaTiO3 的能带隙从间接类型减少到直接类型,减少了 0.65 eV。