首页> 外文期刊>Journal of magnetism and magnetic materials >Mn_2V_(0.5)Co_(0.5)Z (Z = Ga, Al) Heusler alloys: High T_c compensated P-type ferrimagnetism in arc melted bulk and N-type ferrimagnetism in melt-spun ribbons
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Mn_2V_(0.5)Co_(0.5)Z (Z = Ga, Al) Heusler alloys: High T_c compensated P-type ferrimagnetism in arc melted bulk and N-type ferrimagnetism in melt-spun ribbons

机译:Mn_2V_(0.5)Co_(0.5)Z(Z = Ga,Al)Heusler合金:电弧熔体中高T_c补偿的P型亚铁磁性和熔纺薄带中的N型亚铁磁性

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摘要

Ferrimagnetic Heusler alloys with the low moment and high Curie temperature are desired material for spintronic devices utilizing spin transfer torque phenomena. Our earlier report showed compensated ferrimagnetism with high Curie temperature in arc melted bulk Mn(2)V(0.5)Co(0.5)Z (Z = Ga, Al) alloys. The low-temperature M-T behaviour of the bulk alloys was not explored and in this report we discuss the structural and magnetic properties of Mn(2)V(0.5)Co(0.5)Z (Z = Ga, Al) Heusler alloys in the ribbon and bulk forms, particularly concentrating on the distinct low-temperature M-T behaviour. The observed magnetic moment of the parent alloys is around 2 mu(B)/f.u. which was reduced to nearly zero as the Co is substituted at the V site of the Mn(2)VZ (Z = Ga, Al) alloys. The compensated moment value at room temperature for Mn2V0.5Co0.5Ga alloy in the bulk and ribbon forms are 0.13 and 0.09 mu(B)/f.u. respectively. For Mn2V0.5Co0.5Al, a further reduced moment was observed which are 0.08 and 0.04 ( )mu(B)/f.u for the bulk and ribbon samples respectively. The observed Curie temperatures are more than 640 K for both ribbons and bulk samples. A very different temperature dependent magnetic response was observed for the ribbon and bulk samples. The arc melted bulk samples exhibited Neel P-type ferrimagnetic behaviour where there is no full compensation temperature. In contrast to this, the ribbon samples exhibited Neel N-type ferrimagnetic behaviour with a full compensation temperature of 420 K for Mn2V0.5Co0.5Ga and 275 K for MnV0.5Co0.5Al.
机译:具有低力矩和高居里温度的亚铁磁Heusler合金是利用自旋传递转矩现象的自旋电子器件的理想材料。我们较早的报告表明,在电弧熔化的块状Mn(2)V(0.5)Co(0.5)Z(Z = Ga,Al)合金中,居里温度较高时,补偿了亚铁磁性。未探讨块状合金的低温MT行为,在本报告中,我们讨论了带状Mn(2)V(0.5)Co(0.5)Z(Z = Ga,Al)Heusler合金的结构和磁性能和散装形式,尤其是专注于独特的低温MT行为。观察到的母体合金的磁矩约为2μ(B)/f.u。当Co在Mn(2)VZ(Z = Ga,Al)合金的V位置被取代时,它几乎减少到零。块状和带状Mn2V0.5Co0.5Ga合金在室温下的补偿力矩值为0.13和0.09 mu(B)/f.u。分别。对于Mn2V0.5Co0.5Al,观察到进一步减小的力矩,对于大块和带状样品,力矩分别为0.08和0.04(μ)(B)/f.u。对于带状样品和块状样品,观察到的居里温度都超过640K。对于带状样品和块状样品,观察到非常不同的温度依赖性磁响应。电弧熔化的块状样品在没有完全补偿温度的情况下表现出Neel P型亚铁磁行为。与此相反,带状样品表现出Neel N型亚铁磁行为,对于Mn2V0.5Co0.5Ga的完全补偿温度为420 K,对于MnV0.5Co0.5Al的完全补偿温度为275K。

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  • 来源
    《Journal of magnetism and magnetic materials》 |2019年第11期|165298.1-165298.6|共6页
  • 作者单位

    Indian Inst Technol Madras, Dept Phys, Chennai 600036, Tamil Nadu, India;

    Def Met Res Lab, Kanchanbagh PO, Hyderabad 500058, India;

    Int Adv Res Ctr Powder Met & New Mat ARCI, Chennai 600113, Tamil Nadu, India;

    Int Adv Res Ctr Powder Met & New Mat ARCI, Chennai 600113, Tamil Nadu, India;

    Indian Inst Technol Madras, Dept Phys, Chennai 600036, Tamil Nadu, India;

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