带畴壁的铁磁圆柱形纳米线的磁热效应特性

A. Shevchenko, M. Barabash
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引用次数: 1

摘要

建立了在明显低于2М的弱磁场中,M为铁磁圆柱形纳米线的磁化强度,后者的熵由于其所组成的畴壁的热运动而增加。结果,在该系统中出现了负磁热效应。这种现象具有纳米级的性质,并且随着移动到块状材料而消失。结果表明,所建立的效应符合自调节热力学系统的基本勒夏特列尔-布朗原理。所获得的结果对于开发在低维磁性纳米结构上获得精确温度值的新方法具有重要意义。反过来,在原子中电子运动产生的磁场量级(~ (1-10)kOe)的强磁场中,会发生正磁热效应,即铁磁纳米线的温度随着磁场振幅的增加而增加。对于纳米线的直径,给出了从纵向畴壁向畴壁以布洛赫点形式过渡的估计。
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Peculiarities of Magnetocaloric Effect in Ferromagnetic Cylindrical Nanowires with a Domain Wall
It is established that in a weak magnetic field significantly lower than 2М, where M is the magnetization of a ferromagnetic cylindrical nanowire, the entropy of the latter increases due to the thermal motion of the domain wall comprised in it. As a result, a negative magnetocaloric effect emerges in this system. This phenomenon has a nanoscale nature and disappears with moving to bulk materials. It is shown that the established effect is in accordance with the fundamental Le Chatelier-Brown principle for the selfregulating thermodynamic systems. The obtained result is of significant interest in the context of the development of new methods to achieve precise temperature values on the low dimensional magnetic nanostructures. In turn, in strong magnetic fields of the order of the magnetic field generated by the movement of electrons in atoms (~ (1-10) kOe) a positive magnetocaloric effect takes place, i.e. the temperature of the ferromagnetic nanowire increases with increasing amplitude of the magnetic field. For the diameter of the nanowire, an estimate is given at which the transition from the longitudinal domain wall to the domain wall in the form of a Bloch point occurs.
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