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钙钛矿型钛酸盐金属带绝缘体转变中电子输运和热电功率因子的关联及声子效应

Correlation and phonon effects for the electronic transport and thermoelectric power factors in the metal-band-insulator crossover of perovskite-type titanates.

作者信息

Onoda Masashige, Goto Ikuo

出版信息

J Phys Condens Matter. 2009 Oct 28;21(43):435603. doi: 10.1088/0953-8984/21/43/435603. Epub 2009 Oct 8.

Abstract

The structural and electronic properties in the metal-band-insulator crossover of the perovskite-type oxygen deficient system SrTiO(3-δ/2) and the Sr-rare-earth element substituted systems Sr(1-x)Ce(x)TiO(3-δ(n)/2) and Sr(1-x)La(x)TiO(3-δ(n)/2), δ(n) being the nominal value, are explored in order to clarify the transport mechanisms and to determine the thermoelectric power factors, through measurements of the x-ray diffraction, electrical resistivity, thermoelectric power, Hall coefficient and magnetic susceptibility. The metallic transport for SrTiO(3-δ/2) with δ≤0.2 and that for Sr(1-x)Ce(x)TiO(3-δ(n)/2) and Sr(1-x)La(x)TiO(3-δ(n)/2) with x≈0.02 and δ(n) = 0 are explained successfully on the basis of scattering by electron correlations, acoustic phonons with the Debye temperature 4 × 10(2) K and polar optical phonons with the Einstein temperature of the order of 10(3) K. The composition dependences of the carrier concentrations of Sr(1-x)Ce(x)TiO(3-δ(n)/2) and Sr(1-x)La(x)TiO(3-δ(n)/2) with δ(n) = 0 are explained in terms of a one-band model, while those of SrTiO(3-δ/2) with δ>0 are explained in terms of a two-band model, as suggested in part previously. For all of the systems, the effective mass ratio of the transport is about 3 and a thermoelectric power factor is found to have a power of -2/3 in the carrier concentration. The factor over 10(-3)  W m(-1) K(-2) at 300 K is obtained for SrTiO(2.97) with the smallest δ in this work.

摘要

为了阐明输运机制并确定热电功率因子,通过对x射线衍射、电阻率、热电功率、霍尔系数和磁化率的测量,研究了钙钛矿型缺氧体系SrTiO(3 - δ/2)以及Sr - 稀土元素取代体系Sr(1 - x)Ce(x)TiO(3 - δ(n)/2)和Sr(1 - x)La(x)TiO(3 - δ(n)/2)(其中δ(n)为标称值)在金属 - 能带 - 绝缘体转变中的结构和电子性质。基于电子关联散射、德拜温度为4×10²K的声学声子以及爱因斯坦温度约为10³K的极性光学声子,成功解释了δ≤0.2时SrTiO(3 - δ/2)以及x≈0.02且δ(n) = 0时Sr(1 - x)Ce(x)TiO(3 - δ(n)/2)和Sr(1 - x)La(x)TiO(3 - δ(n)/2)的金属输运。对于δ(n) = 0的Sr(1 - x)Ce(x)TiO(3 - δ(n)/2)和Sr(1 - x)La(x)TiO(3 - δ(n)/2),其载流子浓度的成分依赖性用单带模型解释,而对于δ>0的SrTiO(3 - δ/2),如之前部分所建议的,用双带模型解释。对于所有体系,输运的有效质量比约为3,并且发现热电功率因子在载流子浓度上具有-2/3的幂次。在本工作中,对于δ最小的SrTiO(2.97),在300K时获得了超过10⁻³W m⁻¹K⁻²的因子。

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