Device Research Laboratory, Department of Electrical Engineering, University of California, Los Angeles, California 90095, United States.
Nano Lett. 2012 Dec 12;12(12):6372-9. doi: 10.1021/nl303645k. Epub 2012 Dec 3.
In this Letter, the magnetic phase transition and domain wall motion in a single-crystalline Mn(5)Ge(3) nanowire were investigated by temperature-dependent magneto-transport measurements. The ferromagnetic Mn(5)Ge(3) nanowire was fabricated by fully germaniding a single-crystalline Ge nanowire through the solid-state reaction with Mn contacts upon thermal annealing at 450 °C. Temperature-dependent four-probe resistance measurements on the Mn(5)Ge(3) nanowire showed a clear slope change near 300 K accompanied by a magnetic phase transition from ferromagnetism to paramagnetism. The transition temperature was able to be controlled by both axial and radial magnetic fields as the external magnetic field helped maintain the magnetization aligned in the Mn(5)Ge(3) nanowire. Near the magnetic phase transition, the critical behavior in the 1D system was characterized by a power-law relation with a critical exponent of α = 0.07 ± 0.01. Besides, another interesting feature was revealed as a cusp at about 67 K in the first-order derivative of the nanowire resistance, which was attributed to a possible magnetic transition between two noncollinear and collinear ferromagnetic states in the Mn(5)Ge(3) lattice. Furthermore, temperature-dependent magneto-transport measurements demonstrated a hysteretic, symmetric, and stepwise axial magnetoresistance of the Mn(5)Ge(3) nanowire. The interesting features of abrupt jumps indicated the presence of multiple domain walls in the Mn(5)Ge(3) nanowire and the annihilation of domain walls driven by the magnetic field. The Kurkijärvi model was used to describe the domain wall depinning as thermally assisted escape from a single energy barrier, and the fitting on the temperature-dependent depinning magnetic fields yielded an energy barrier of 0.166 eV.
在这封信件中,通过温度依赖的磁输运测量研究了单晶 Mn(5)Ge(3)纳米线中的磁相变和畴壁运动。通过在 450°C 下通过 Mn 接触与单晶 Ge 纳米线进行固态反应,完全锗化单晶 Ge 纳米线来制备铁磁 Mn(5)Ge(3)纳米线。在 Mn(5)Ge(3)纳米线上进行的温度依赖的四探针电阻测量在 300 K 附近显示出明显的斜率变化,伴随着从铁磁性到顺磁性的磁相变。通过轴向和径向磁场都可以控制相变温度,因为外磁场有助于保持 Mn(5)Ge(3)纳米线中的磁化方向一致。在磁相变附近,1D 系统的临界行为由具有临界指数α=0.07±0.01 的幂律关系来描述。此外,在纳米线电阻的一阶导数中发现了另一个有趣的特征,即约 67 K 处的尖峰,这归因于 Mn(5)Ge(3)晶格中两个非共线和共线铁磁态之间可能发生的磁转变。此外,温度依赖的磁输运测量表明 Mn(5)Ge(3)纳米线具有滞后、对称和阶跃的轴向磁电阻。急剧跳跃的有趣特征表明 Mn(5)Ge(3)纳米线中存在多个畴壁,并且畴壁在磁场的驱动下被消除。Kurkijärvi 模型用于描述畴壁去钉扎,即热辅助从单个能量势垒中逃逸,并且在温度依赖的去钉扎磁场上的拟合得出了 0.166 eV 的能量势垒。