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纯态和掺杂态Ba6Ti2Nb8O30钨青铜的结构与光谱性质

Structural and spectroscopic properties of pure and doped Ba6Ti2Nb8O30 tungsten bronze.

作者信息

Massarotti V, Capsoni D, Bini M, Azzoni C B, Mozzati M C, Galinetto P, Chiodelli G

机构信息

Dipartimento di Chimica Fisica, M. Rolla dell'Università, viale Taramelli 16, 27100 Pavia, Italy.

出版信息

J Phys Chem B. 2006 Sep 14;110(36):17798-805. doi: 10.1021/jp063382p.

Abstract

Pure and doped Ba(6)Ti(2)Nb(8)O(30) (BTN), obtained by substituting M = Cr, Mn, or Fe on the Ti site (Ba(6)Ti(2-x) M(x)Nb(8)O(30), x = 0.06 and 0.18) and Y and Fe on the Ba and Ti sites, respectively (Ba(6-x)Y(x)Ti(2-x)Fe(x)Nb(8)O(30), x= 0.18), are synthesized. The influence of cation doping on the local structure, the cation oxidation state, and the possible defect formation able to maintain the charge neutrality are investigated by spectroscopic (electron paramagnetic resonance (EPR) and micro-Raman), structural (X-ray powder diffraction) and transport (impedance spectroscopy, thermoelectric power) measurements, in the temperature range of 300-1200 K in air and N(2) flow. Starting from the valence state of the doping ions (Fe(3+), Cr(3+), and Mn(2+)), determined by EPR, and from thermoelectric power measurements, evidencing a negative charge transport, different charge-compensating defect equilibria, based on the creation of positive electron holes or oxygen vacancies and electrons, are discussed to interpret the conductivity results.

摘要

通过在Ti位点上用M = Cr、Mn或Fe进行替代(Ba(6)Ti(2 - x)M(x)Nb(8)O(30),x = 0.06和0.18)以及分别在Ba和Ti位点上用Y和Fe进行替代(Ba(6 - x)Y(x)Ti(2 - x)Fe(x)Nb(8)O(30),x = 0.18),合成了纯的和掺杂的Ba(6)Ti(2)Nb(8)O(30)(BTN)。在300 - 1200 K的温度范围内,于空气和N(2)气流中,通过光谱测量(电子顺磁共振(EPR)和显微拉曼光谱)、结构测量(X射线粉末衍射)以及输运测量(阻抗谱、热电功率),研究了阳离子掺杂对局部结构、阳离子氧化态以及能够保持电荷中性的可能缺陷形成的影响。从由EPR确定的掺杂离子(Fe(3+)、Cr(3+)和Mn(2+))的价态出发,以及从热电功率测量结果(表明存在负电荷传输)出发,基于正电子空穴或氧空位以及电子的产生,讨论了不同的电荷补偿缺陷平衡,以解释电导率结果。

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