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{Rearrangement of the antiferromagnetic ordering at high magnetic fields in SmFeAsO and SmFeAsO$_{0.9}$F$_{0.1}$ single crystals

机译:{重新排列高磁场下的反铁磁有序   在smFeasO和smFeasO $ _ {0.9} $ F $ _ {0.1} $单晶

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摘要

The low-temperature antiferromagnetic state of the Sm-ions in bothnonsuperconducting SmFeAsO and superconducting SmFeAsO$_{0.9}$F$_{0.1}$ singlecrystals was studied by magnetic torque, magnetization, and magnetoresistancemeasurements in magnetic fields up to 60~T and temperatures down to 0.6~K. Weuncover in both compounds a distinct rearrangement of the antiferromagneticallyordered Sm-moments near $35-40$~T. This is seen in both, static and pulsedmagnetic fields, as a sharp change in the sign of the magnetic torque, which issensitive to the magnetic anisotropy and hence to the magnetic moment in the$ab$-plane, ({\it i.e.} the FeAs-layers), and as a jump in the magnetizationfor magnetic fields perpendicular to the conducting planes. This rearrangementof magnetic ordering in $35-40$~T is essentially temperature independent andpoints towards a canted or a partially polarized magnetic state in highmagnetic fields. However, the observed value for the saturation moment abovethis rearrangement, suggests that the complete suppression of theantiferromagnetism related to the Sm-moments would require fields in excess of60~T. Such a large field value is particularly remarkable when compared to therelatively small N\'{e}el temperature $T_{\rm N}\simeq5$~K, suggesting veryanisotropic magnetic exchange couplings. At the transition, magnetoresistivitymeasurements show a crossover from positive to negative field-dependence,indicating that the charge carriers in the FeAs planes are sensitive to themagnetic configuration of the rare-earth elements. This is indicates a finitemagnetic/electronic coupling between the SmO and the FeAs layers which arelikely to mediate the exchange interactions leading to the long rangeantiferromagnetic order of the Sm ions.
机译:通过在高达60°T和60°T的磁场中通过磁转矩,磁化强度和磁阻测量方法研究了非超导SmFeAsO和超导SmFeAsO $ _ {0.9} $ F $ _ {0.1} $单晶中Sm离子的低温反铁磁态温度降至0.6〜K Weun在这两种化合物中均发现反铁磁有序Sm矩在$ 35-40 $〜T附近有明显的重排。在静磁场和脉冲磁场中都可以看到,这是磁转矩符号的急剧变化,它对磁各向异性以及对ab $平面中的磁矩敏感。 FeAs层),并作为垂直于导电平面的磁场的磁化跃迁。 $ 35-40 $〜T中的磁性有序排列基本上是温度无关的,并且指向高磁场中的倾斜或部分极化的磁态。然而,高于该重排的饱和力矩的观测值表明,完全抑制与Sm矩有关的反磁性将需要超过60 T的磁场。当与相对较小的Nel'el温度$ T_ {rm N} \ simeq5 $〜K相比时,如此大的场值特别引人注目,这表明非常各向异性的磁交换耦合。在过渡过程中,磁阻测量值显示出从正场依赖到负场依赖的过渡,表明FeAs平面中的电荷载流子对稀土元素的磁性构型敏感。这表明SmO和FeAs层之间存在有限的磁/电耦合,它们可能介导导致Sm离子的长距离反铁磁序的交换相互作用。

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