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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:SmFeAsO和SmFeAsO_(0.9)F_(0.1)单晶中高磁场下反铁磁有序的重排

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摘要

The low-temperature antiferromagnetic state of the Sm ions in both nonsuperconducting SmFeAsO and superconducting SmFeAsO_(0.9)F_(0.1) single crystals was studied by magnetic torque, magnetization, and magnetoresistance measurements in magnetic fields up to 60 T and temperatures down to 0.6 K. We uncover in both compounds a distinct rearrangement of the antiferromagnetically ordered Sm moments near 35 — 40 T. This is seen in both static and pulsed magnetic fields as a sharp change in the sign of the magnetic torque, which is sensitive to the magnetic anisotropy and hence to the magnetic moment in the ab plane, (i.e., the FeAs layers), and as a jump in the magnetization for magnetic fields perpendicular to the conducting planes. This rearrangement of magnetic ordering in 35 — 40 T is essentially temperature independent and points toward a canted or a partially polarized magnetic state in high magnetic fields. However, the observed value for the saturation moment above this rearrangement, suggests that the complete suppression of the antiferromagnetism related to the Sm-moments would require fields in excess of 60 T. Such a large field value is particularly remarkable when compared to the relatively small Neel temperature T_n (~-) 5 K, suggesting very anisotropic magnetic exchange couplings. At the transition, magnetoresistivity measurements show a crossover from positive to negative field dependence, indicating that the charge carriers in the FeAs planes are sensitive to the magnetic configuration of the rare-earth elements. This points towards a finite magnetic/electronic coupling between the SmO and the FeAs layers which are likely to mediate the exchange interactions leading to the long-range antiferromagnetic order of the Sm ions.
机译:通过在高达60 T和温度低至0.6 K的磁场中测量磁矩,磁化强度和磁阻,研究了非超导SmFeAsO和超导SmFeAsO_(0.9)F_(0.1)单晶中Sm离子的低温反铁磁状态。我们在这两种化合物中发现35-40 T附近的反铁磁有序Sm矩有明显的重排,这在静磁场和脉冲磁场中都可以看作是磁转矩符号的急剧变化,这对磁各向异性很敏感。因此,对于ab平面(即FeAs层)中的磁矩,以及垂直于导电平面的磁场的磁化跃变。 35-40 T的磁有序重新排列基本上与温度无关,并且指向强磁场中的倾斜或部分极化的磁态。但是,高于此重排的饱和矩的观测值表明,要完全抑制与Sm矩有关的反铁磁,将需要超过60 T的磁场。与相对较小的磁场值相比,如此大的磁场值特别引人注目尼尔温度T_n(〜-)5 K,表明各向异性非常强的磁交换耦合。在过渡过程中,磁阻测量值显示出从正场到负场的依赖关系,这表明FeAs平面中的电荷载流子对稀土元素的磁构型敏感。这指向SmO和FeAs层之间的有限的磁/电耦合,这很可能介导交换相互作用,从而导致Sm离子的长距离反铁磁有序。

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  • 来源
    《Physical review》 |2011年第13期|p.134504.1-134504.7|共7页
  • 作者单位

    Physik-Institut der Universitdt Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland;

    Laboratory for Solid State Physics, ETH Zurich, CH-8093 Zurich, Switzerland;

    Institute of Physics, Polish Academy of Sciences, Aleja Lotnikow 32/46, PL-02-668 Warsaw, Poland;

    Department of Physics, University of Florida, Gainesville, Florida 32611, USA;

    National High Magnetic Field Laboratory, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA;

    National High Magnetic Field Laboratory, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA;

    Department of Physics, University of Florida, Gainesville, Florida 32611, USA;

    Laboratory for Solid State Physics, ETH Zurich, CH-8093 Zurich, Switzerland;

    Laboratory for Solid State Physics, ETH Zurich, CH-8093 Zurich, Switzerland;

    Laboratory for Solid State Physics, ETH Zurich, CH-8093 Zurich, Switzerland;

    Laboratory for Solid State Physics, ETH Zurich, CH-8093 Zurich, Switzerland;

    Physik-Institut der Universitdt Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland;

    Laboratory for Solid State Physics, ETH Zurich, CH-8093 Zurich, Switzerland;

    National High Magnetic Field Laboratory, Florida State University, Tallahassee, Florida 32310, USA;

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  • 关键词

    magnetic anisotropy; magnetic phase boundaries (including magnetic transitions, metamagnetism, etc.); antiferromagnetics;

    机译:磁各向异性磁相边界(包括磁跃迁;超磁性等);反铁磁;

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