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Femtosecond laser heating induced ultrafast magnetization reversal in TbCo films with different electron-phonon coupling inter-action

机译:飞秒激光加热在具有不同电子-声子耦合相互作用的TbCo薄膜中引起超快磁化反转

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TbCo alloy films possess ferrimagnetic structure and high perpendicular anisotropy and have been proven to rapidly reverse their magnetic moments irradiated with an ultra-short pulse laser, which have the potential to use as all optical switching media [1-2]. In this paper, we have adopted a two-temperature model [3] and a general theoretical framework [4] to calculate the temperatures of the electron gas (Te) and the phonon (Tp) and the magnetization dynamics of Tb26Co74 films, respectively, and found that electron-phonon coupling factor (G) plays a significant influence on the Te and magnetization reversal dynamics of TbCo films. In our simulation, the laser wavelength and pulse width, laser fluence are 560 nm, 100 fs and 15 J/m2, respectively. The G values vary from 1 to 10×1017 W/m3. K. Fig 1 shows the time evolution of Te and Tp. Te rapidly increases to the peak temperature within about 0.3ps and then decreases with different rates until reaching the same value as Tp. TbCo films with a smaller G have a higher peak temperature of Te and exhibit a slower cooling rate, and thus experience a longer heat exchange time between the electron gas and phonon. Fig 2 presents the computed time-resolved magnetization dynamics of Co- and Tb- sublattices. When G is just 1×1017W/m3. K, only the rapid demagnetization process occurs in Co- and Tb- sublattices and no magnetization reversal is observed due to the higher Te and slower cooling rate. As G continues to increase, the demagnetization time of Co- sublattice rises slowly, but the initial reversal time of Co- sublattice drops gradually from 1.27ps to 0.66ps, which is attributed to the decreasing Te and the increasing cooling rate of electron gas. Moreover, Tb- sublattice delays to reverse its magnetic moment with the increase of G perhaps owing to the lower Te and the slower demagnetization of Tb- sublattice. Furthermore, although Co- and Tb- sublattices both generate magnetization reversal, the total magnetization reversal of Tb26Co74 films does not occur within the timescale of 5ps and will happen after a relatively longer recovery of magnetic moments of Tb- sublattice.
机译:TbCo合金膜具有亚铁磁性结构和较高的垂直各向异性,并已被证明可以快速逆转其超短脉冲激光辐照的磁矩,它们有可能用作所有光学开关介质[1-2]。在本文中,我们采用了两温模型[3]和通用理论框架[4]来计算电子气的温度(T e )和声子(T p )和Tb的磁化动力学 26 有限公司 74 薄膜,并发现电子-声子耦合因子(G)对T具有重要影响 e TbCo薄膜的磁化反转动力学。在我们的仿真中,激光波长和脉冲宽度,激光通量分别为560 nm,100 fs和15 J / m 2 , 分别。 G值从1到10×10不等 17 瓦/米 3 。 K。图1显示了T的时间演变 e 和T p 。 Ť e 在约0.3ps内迅速上升至峰值温度,然后以不同的速率下降,直到达到与T相同的值 p 。 G较小的TbCo薄膜具有较高的T峰值温度 e 并且表现出较慢的冷却速率,因此在电子气与声子之间经历了更长的热交换时间。图2给出了Co-和Tb-亚晶格的时间分辨磁化动力学。当G仅为1×10 17 瓦/米 3 。 K,仅在Co-和Tb-亚晶格中发生快速退磁过程,并且由于较高的T而未观察到磁化反转 e 和较慢的冷却速度随着G的持续增加,共晶格的退磁时间缓慢增加,但共晶格的初始反转时间从1.27ps逐渐降至0.66ps,这归因于T的减小 e 以及电子气冷却速度的提高。此外,随着G的增加,Tb-亚晶格延迟了其磁矩的反转,这可能是由于较低的T e Tb-亚晶格的退磁速度较慢。此外,尽管Co-和Tb-亚晶格都会产生磁化反转,但是Tb的总磁化反转 26 有限公司 74 薄膜不会在5ps的时间范围内发生,而是会在相对较长的Tb-亚晶格磁矩恢复后发生。

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