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Probing the magnetic state by linear and non linear ac magnetic susceptibility measurements in under doped manganite Nd0.8Sr0.2MnO3

机译:通过线性和非线性交流磁探测磁状态   掺杂锰氧化物Nd0.8sr0.2mnO3的磁化率测定

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摘要

We have thoroughly investigated the entire magnetic states of under dopedferromagnetic insulating manganite Nd0.8Sr0.2MnO3 through temperature dependentlinear and non linear complex ac magnetic susceptibility measurements. Thisferromagnetic insulating manganite is found to have frequency independentferromagnetic to paramagnetic transition temperature at around 140 K. At around90 K (\approx T_f) the sample shows a second frequency dependent re - entrantmagnetic transition as explored through complex ac susceptibility measurements.Non linear ac susceptibility measurements (higher harmonics of acsusceptibility) have also been performed (with and without the superposition ofa dc magnetic field) to further investigate the origin of this frequencydependence (dynamic behavior at this re-entrant magnetic transition).Divergence of 3rd order susceptibility in the limit of zero exciting fieldindicates a spin glass like freezing phenomena. However, large value of spinrelaxation time (?0= 10-8 s) and small value of coercivity (~22 Oe) obtained atlow temperature (below T_f) from critical slowing down model and dc magneticmeasurements, respectively, are in contrast with what generally observed in acanonical spin glass (?0 = 10-12 - 10-14 s and very large value of coercivitybelow freezing temperature). We have attributed our observation to theformation of finite size ferromagnetic clusters which are formed as consequenceof intrinsic separation and undergo cluster glass like freezing below certaintemperature in this under doped manganite. The results are supported by theelectronic - and magneto - transport data.
机译:我们通过依赖温度的线性和非线性复交流磁化率测量,彻底研究了掺杂铁磁绝缘锰矿Nd0.8Sr0.2MnO3下的整个磁态。该铁磁绝缘锰矿在约140 K处具有与铁磁至顺磁的频率无关的频率。通过复杂的磁化率测量探索,样品在约90 K(约T_f)处显示出第二个随频率变化的反磁跃迁。 (有较高的谐波谐波)(在有和没有直流磁场叠加的情况下)也已经执行过,以进一步研究这种频率依赖性的起源(在该重入磁跃迁处的动力学行为)。零激励场表示旋转玻璃像冻结现象。然而,分别从临界减速模型和直流磁测量中获得的自旋弛豫时间的值较大(?0 = 10-8 s),而在低温(T_f以下)获得的矫顽力值较小(〜22 Oe)与一般情况相反。在典型的旋转玻璃中观察到(Δ0= 10-12-10-14 s,并且在凝固温度以下矫顽力值非常大)。我们将观察结果归因于有限尺寸铁磁团簇的形成,这些铁磁团簇是本征分离的结果,并在掺杂锰的情况下在一定温度以下经历了像冻结一样的团簇玻璃。结果由电子和磁传输数据支持。

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    Kundu, S.; Nath, T. K.;

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  • 年度 2010
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