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μSR 研究磁电阻钌铜钙钛矿 RuSr2Nd(1.8-x)Y0.2Ce(x)Cu2O(10-δ)(x = 0.95 和 0.80)。

A μSR study of the magnetoresistive ruthenocuprates RuSr2Nd(1.8-x)Y0.2Ce(x)Cu2O(10-δ) (x = 0.95 and 0.80).

机构信息

Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen, UK.

出版信息

J Phys Condens Matter. 2011 Sep 14;23(36):365704. doi: 10.1088/0953-8984/23/36/365704. Epub 2011 Aug 25.

DOI:10.1088/0953-8984/23/36/365704
PMID:21865639
Abstract

Zero field muon spin relaxation (ZF-μSR) has been used to study the magnetic properties of the underdoped giant magnetoresistive ruthenocuprates RuSr(2)Nd(1.8-x)Y (0.2)Ce(x)Cu(2)O(10-δ) (x = 0.95, 0.80). The magnetoresistance (MR) is defined so that MR = ((ρ(H)-ρ(0))/ρ(0)) and the giant magnetoresistive ruthenocuprates RuSr(2)Nd(1.8-x)Y(0.2)Ce(x)Cu(2)O(10-δ) exhibit a large reduction in electronic resistivity upon application of a magnetic field. The ZF-μSR results show a gradual loss of initial asymmetry A(0) at the ruthenium spin transition temperature, T(Ru). At the same time the electronic relaxation rate, λ, shows a gradual increase with decreasing temperature below T(Ru). These results have been interpreted as evidence for Cu spin cluster formation below T(Ru). These magnetically ordered clusters grow as the temperature is decreased thus causing the initial asymmetry to decrease slowly. Giant magnetoresistance is observed over a wide temperature range in the materials studied and the magnitude increases as the temperature is reduced from T(Ru) to 4 K which suggests a relation between Cu spin cluster size and |-MR|.

摘要

零场μ子自旋弛豫(ZF-μSR)已被用于研究欠掺杂巨磁电阻钌铜酸盐 RuSr(2)Nd(1.8-x)Y(0.2)Ce(x)Cu(2)O(10-δ)(x = 0.95、0.80)的磁性。磁电阻(MR)的定义为 MR = ((ρ(H)-ρ(0))/ρ(0)),巨磁电阻钌铜酸盐 RuSr(2)Nd(1.8-x)Y(0.2)Ce(x)Cu(2)O(10-δ) 在施加磁场时电子电阻率会大幅降低。ZF-μSR 结果表明,在钌自旋转变温度 T(Ru)处,初始不对称性 A(0)逐渐消失。与此同时,电子弛豫率 λ 在低于 T(Ru)的温度下逐渐增加。这些结果被解释为在 T(Ru)以下形成 Cu 自旋团簇的证据。随着温度的降低,这些磁性有序团簇会生长,从而导致初始不对称性缓慢降低。在所研究的材料中,巨磁电阻在很宽的温度范围内都有观察到,并且随着温度从 T(Ru)降低到 4 K,其幅度增加,这表明 Cu 自旋簇尺寸与 |-MR| 之间存在关系。

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