Semiconducting and magnetic properties of La/sub 0.67/Ca/sub 0.33/Mn/sub 1-x/Dy/sub x/O/sub 3/ ceramics

S. A. Halim, S. Koh, S. P. Chow, E. Saion, H. Mansor, W.Y.W. Daud
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Abstract

Electrical resistivity measurements of La/sub 0.67/Ca/sub 0.33/Mn/sub 1-x/Dy/sub x/O/sub 3/, x=0 to 0.12, ceramics have been studied using a standard four point probe technique, while the magnetic behaviour has been studied using AC susceptibility techniques. The transport properties show the transition from semiconducting to metallic conductivity at T/sub p/ and paramagnetic-ferromagnetic transitions, T/sub c/, were observed in the /spl chi/-temperature curves for all samples. The existence of metallic conductivity, T/sub p/, and ferromagnetism, T/sub c/, were found to be linearly correlated. This phenomenon of coexistence is due to the double exchange interaction of two electrons in Mn/sup 3+/-O/sup 2-/-Mn/sup 4+/ and Mn/sup 4+/-O/sup 2-/-Mn/sup 3+/ configuration which brings the system below T/sub c/ into a metallic state. Hence, it is observed that the Curie temperature T/sub c/ is closely related to the sharp decrease in electrical resistivity of the samples. However, both transition temperatures shift to lower temperatures as dysprosium doping increases, indicating the loss of ferromagnetic order and transport properties. As for the transport properties, the semiconductor model ln(/spl sigma/)/spl sim/(E/sub g//2kT) was used to explain the conduction mechanism of perovskite manganites above T/sub p/. It was concluded that the total conductivity /spl sigma//sub tot/ consists of the intrinsic and extrinsic components such that /spl sigma//sub tot/=/spl sigma//sub int/+/spl sigma//sub ext/. The energy gap decreases initially from 0.11 eV to a minimum value of 0.06 eV at x=0.03 and increases again to 0.08 eV at the composition of x=0.12 for the extrinsic region.
La/sub 0.67/Ca/sub 0.33/Mn/sub 1-x/Dy/sub x/O/sub 3/陶瓷的半导体和磁性能
使用标准四点探针技术研究了La/sub 0.67/Ca/sub 0.33/Mn/sub 1-x/Dy/sub x/O/sub 3/, x=0至0.12,陶瓷的电阻率测量,同时使用交流磁化率技术研究了磁性行为。输运性质显示在T/sub p/处从半导体到金属电导率的转变,并且在/spl chi/-温度曲线上观察到顺磁-铁磁转变T/sub c/。金属电导率T/sub p/与铁磁性T/sub c/呈线性相关。这种共存现象是由于两个电子在Mn/sup 3+/- o /sup 2-/-Mn/sup 4+/和Mn/sup 4+/- o /sup 2-/-Mn/sup 3+/构型中的双重交换相互作用,使T/sub c/以下的体系进入金属态。由此可见,居里温度T/sub c/与试样电阻率的急剧下降密切相关。然而,随着镝掺杂的增加,这两个转变温度都向更低的温度转移,表明铁磁有序和输运性质的损失。在输运性质方面,采用半导体模型ln(/spl sigma/)/spl sim/(E/sub g//2kT)来解释钙钛矿型锰矿在T/sub p/以上的传导机理。结果表明:总电导率/spl sigma//sub - tot/由内禀分量和外禀分量组成,因此/spl sigma//sub - tot/=/spl sigma//sub - int/+/spl sigma//sub - ext/。当x=0.03时,能隙从0.11 eV减小到最小值0.06 eV,当x=0.12时,能隙再次增大到0.08 eV。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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