论文标题

激光驱动的一阶旋转重新定位和磁铁矿Fe $ _3 $ o $ $ _4 $以外热力学平衡的verwey阶段过渡

Laser-driven first-order spin reorientation and Verwey phase transitions in the magnetite Fe$_3$O$_4$ beyond the range of thermodynamic equilibrium

论文作者

Kuzikova, A. V., Shelukhin, L. A., Maksimov, F. M., Chernov, A. I., Pisarev, R. V., Kalashnikova, A. M.

论文摘要

在飞秒激光脉冲的影响下发生的超快光诱导的相变提供了多功能的统一性,可在明显不同的晶体,电子和磁状态之间切换固体,从而以显着的方式改变其功能性能。在本文中,我们报告了激光诱导的自旋重新定位和Verwey阶段过渡,以单晶的铁磁磁铁矿Fe $ _3 $ o $ _4 $。使用飞秒的光学和磁光泵探针技术,当零部器完整的照片诱导的相变从单胶线的绝缘液到立方金属状态,并从单一的磁性态转换从单一的磁性转换到单一的单位型,我们从单一的金属态转换时,定义了初始样品温度和激光液的范围。因此,当通过飞秒激光脉冲驱动时,我们揭示了这些相变的连接。使用瞬态线性和二次磁光效应,我们检查了磁化动力学启动了磁各向异性轴的切换。我们在激光诱导的相变下的域的存在甚至低于过渡的阈值阈值和最初位于立方相的材料时。这是两种激光诱导的相变超出热力学平衡范围的一阶的表现。

Ultrafast photo-induced phase transitions occurring under the impact of femtosecond laser pulses provide versatile opport unities for switching solids between distinctly-different crystalline, electronic, and magnetic states and thus modify their functional properties in a significant way. In this paper, we report on the laser-induced spin reorientation and Verwey phase transitions in a single crystalline ferrimagnetic magnetite Fe$_3$O$_4$. Using femtosecond optical and magneto-optical pump-probe techniques, we define the range of the initial sample temperatures and laser fluences when partialor complete photo-induced phase transitions occur from a monoclinic insulating to a cubic metallic state with concomitant switching of magnetic anisotropy from the uniaxial to the cubic one. We thus reveal a connection between these phase transitions when driven by femtosecond laser pulses.Using transient linear and quadratic magneto-optical effects, we examine magnetization dynamics launched the switching of the magnetic anisotropy axis. We unveil the presence of the domains under going the laser-induced phase transitions even below the established threshold fluence for the transitions, as well as when the material is initially in the cubic phase. This is the manifestation of the first-order of these both laser-induced phase transitions beyond the range of thermodynamic equilibrium.

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