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首页> 外文期刊>Physical review >Ultrafast demagnetization after laser irradiation in transition metals: Ab initio calculations of the spin-flip electron-phonon scattering with reduced exchange splitting
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Ultrafast demagnetization after laser irradiation in transition metals: Ab initio calculations of the spin-flip electron-phonon scattering with reduced exchange splitting

机译:过渡金属中激光辐照后的超快退磁:自旋翻转电子声子散射的从头算,具有减小的交换分裂

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Despite intensive research, the underlying mechanisms for ultrafast demagnetization after laser irradiation in transition metals are still not understood. We discuss the possible processes which have been suggested in order to explain the ultrafast demagnetization within several hundreds of femtoseconds and argue that the spin angular momentum has to go to the lattice in the end. Based on this argument, we consider spin-flip electron-phonon scatterings. The demagnetization time ι_M and the demagnetization rate dM/dt due to spin-flip electron-phonon scattering is calculated for fcc Ni and bcc Fe. Thereby, the electronic states and phononic states are calculated ab initio. We find that the demagnetization rates for fcc Ni and bcc Fe are too small to explain experimental demagnetization rates, which is in agreement with earlier publications. In addition, the demagnetization rates for band structures with reduced exchange splitting are calculated, however, also these demagnetization rates are too small. Finally, the phase space for scattering processes which is related to the maximum possible demagnetization is estimated for band structures with ground-state exchange splitting and with reduced exchange splitting. The maximum possible demagnetization is too small for bcc Fe and fcc Co but not necessarily for fcc Ni. We suggest to include magnons and to consider independent combinations of spin-flip electron-phonon and spin-flip electron-magnon scattering processes as a possible explanation for the ultrafast demagnetization.
机译:尽管进行了深入研究,但过渡金属中激光辐照后超快退磁的潜在机理仍不清楚。我们讨论了可能的过程,这些过程已被建议用来解释数百飞秒内的超快退磁,并认为自旋角动量最终必须进入晶格。基于这一论点,我们考虑了自旋翻转电子-声子散射。对于fcc Ni和bcc Fe,计算了由于自旋翻转电子-声子散射而引起的退磁时间ΔM和退磁率dM / dt。由此,从头计算电子状态和声子状态。我们发现fcc Ni和bcc Fe的退磁率太小,无法解释实验性退磁率,这与早期的出版物是一致的。另外,计算了具有减小的交换分裂的带结构的退磁率,但是,这些退磁率也太小。最后,对于具有基态交换分裂和减少的交换分裂的频带结构,估计了与最大可能退磁有关的散射过程的相空间。对于bcc Fe和fcc Co,最大可能的退磁量太小,但对于fcc Ni则不一定。我们建议包括磁振子,并考虑将自旋翻转电子声子和自旋翻转电子磁子散射过程的独立组合作为超快退磁的可能解释。

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