首页> 外文期刊>Journal of Applied Physics >Thermopower peak in phase transition region of (1-x)La_(2/3)Ca_(1/3)MnO_(3)/(x)yttria-stabilized zirconia
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Thermopower peak in phase transition region of (1-x)La_(2/3)Ca_(1/3)MnO_(3)/(x)yttria-stabilized zirconia

机译:(1-x)La_(2/3)Ca_(1/3)MnO_(3)/(x)氧化钇稳定氧化锆相变区的热功率峰值

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摘要

The thermoelectric power (TEP) and the electrical resistivity of the intergranular magnetoresistance composite (1-x)La_(2/3)Ca_(1/3)MnO_(3)/(x)yttria-stabilized zirconia (YSZ) (LCMO/YSZ) with x=0, 0.75, 1.25, 4.5, 13, 15, and 80 of YSZ have been measured from 300 down to 77 K. A pronounced TEP peak appears during phase transition for samples with x>0, while it is not observed for x=0. We suggest that this is due to the magnetic structure variation induced by lattice strain which is a result of the LCMO/YSZ boundary layers. The transition width in the temperature derived from dχ/dT, with χ the ac magnetic susceptibility, supports this interpretation.
机译:在300至77 K测量了x=0%、0.75%、1.25%、4.5%、13%、15%和80%的晶间磁阻复合材料(1-x)La_(2/3)Ca_(1/3)MnO_(3)/(x)钇稳定氧化锆(YSZ)(LCMO/YSZ)的热电功率(TEP)和电阻率。对于x>0的样品,在相变期间会出现明显的TEP峰,而在x=0时则没有观察到。我们认为这是由于LCMO/YSZ边界层引起的晶格应变引起的磁结构变化。由dχ/dT得出的温度转变宽度,χ为交流磁化率,支持这种解释。

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