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首页> 外文期刊>Journal of Physics, D. Applied Physics: A Europhysics Journal >Magnetic, electronic transport and magneto-transport behaviours of (Co1-xMnx)(2)P compounds
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Magnetic, electronic transport and magneto-transport behaviours of (Co1-xMnx)(2)P compounds

机译:(Co1-xMnx)(2)P化合物的磁,电子迁移和磁迁移行为

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Magnetic, electronic transport and magneto-transport behaviours of (Co1-xMnx)(2)P (0.55 <= x <= 0.675) compounds have been systematically investigated. A typical metallic-conductivity behaviour is observed in the ferromagnetic compound (Co0.45Mn0.55)(2)P. The increase in the Mn concentration gives rise to dramatic changes in magnetic, electronic transport and magneto-transport behaviours. With increasing temperature, a first-order phase transition from antiferromagnetism to ferromagnetism takes place at about 145 K, 185K and 240K for x = 0.60, 0.625 and 0.65, respectively. (Co0.4Mn0.6)(2)P and (Co0.375Mn0.625)(2)P compounds experience a metal-insulator transition (Anderson transition) with decreasing temperature. An external magnetic field of 5 T strongly influences the Anderson transition, lowering the transition temperature from 80 to 55K for (Co0.4Mn0.6)(2)P and from 115 to 70K for (Co0.375Mn0.625)(2)P. In contrast with this metal-insulator transition, an insulating behaviour appears in the temperature range from 10 to 300K for (Co0.35Mn0.65)(2)P and (Co0.325Mn0.675)(2)P compounds. Below the antiferromagnetic-ferromagnetic transition temperature TAF-F, a metamagnetic transition can be induced by an external magnetic field. The metamagnetic transition is accompanied by a maximum magnetoresistance ratio of -7%, -6.3% or -3.7% at 5 T in the (Co0.4Mn0.6)(2)P, (Co0.375Mn0.625)(2)P or (Co0.35Mn0.65)(2)P compound at 10 K. The mechanisms of magnetoresistive behaviours are discussed in terms of the formation of a super-zone gap in the antiferromagnetic state.
机译:(Co1-xMnx)(2)P(0.55 <= x <= 0.675)化合物的磁,电子传输和磁传输行为已得到系统地研究。在铁磁化合物(Co0.45Mn0.55)(2)P中观察到典型的金属导电行为。锰浓度的增加引起磁,电子传输和磁传输行为的巨大变化。随着温度升高,对于x = 0.60、0.625和0.65,从反铁磁性到铁磁性的一阶相变分别发生在约145K,185K和240K。 (Co0.4Mn0.6)(2)P和(Co0.375Mn0.625)(2)P化合物会随着温度降低而经历金属-绝缘体转变(Anderson转变)。 5 T的外部磁场会强烈影响安德森跃迁,将(Co0.4Mn0.6)(2)P的跃迁温度从80降低到55K,将(Co0.375Mn0.625)(2)P的跃迁温度从115降低到70K 。与这种金属-绝缘体转变相反,对于(Co0.35Mn0.65)(2)P和(Co0.325Mn0.675)(2)P化合物,绝缘行为出现在10至300K的温度范围内。在反铁磁-铁磁转变温度TAF-F以下,可以通过外部磁场诱发亚磁转变。在(Co0.4Mn0.6)(2)P,(Co0.375Mn0.625)(2)P中,在5 T下,亚磁跃迁的最大磁阻比为-7%,-6.3%或-3.7%或(Co0.35Mn0.65)(2)P化合物在10 K时。根据在反铁磁状态下超区间隙的形成,讨论了磁阻行为的机理。

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