2016
DOI: 10.1103/physrevb.93.064401
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Dual-pump manipulation of ultrafast demagnetization in TbFeCo

Abstract: Laser-induced ultrafast demagnetization in TbFeCo has been studied with a dual-pumping system. Five different laser fluence combinations were applied at three different time intervals between two pump pulses. The experimental results are also compared with computational simulations using the atomistic model. Importantly, this demagnetization can be controllably manipulated in both its magnitude and temporal response.

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Cited by 14 publications
(7 citation statements)
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“…Since the electron–spin interaction channel is open here, within few femtoseconds, the temperature of the spin system increases to a higher value, following the sharp rise of electron temperature. Figure b shows that the reflectivity peak increases linearly with the increase in pump fluence, which is directly related to the electron temperature . The pump laser-excited hot electrons interact with the spin system via transfer of energy.…”
Section: Results and Discussionmentioning
confidence: 94%
“…Since the electron–spin interaction channel is open here, within few femtoseconds, the temperature of the spin system increases to a higher value, following the sharp rise of electron temperature. Figure b shows that the reflectivity peak increases linearly with the increase in pump fluence, which is directly related to the electron temperature . The pump laser-excited hot electrons interact with the spin system via transfer of energy.…”
Section: Results and Discussionmentioning
confidence: 94%
“…TbFeCo is an example of such a material, that, due to large coercive fields above 10 T, is well suitable for high density magnetic recording [28,29]. Although several attempts of modeling the laser-induced spin dynamics in TbFeCo have been performed [30][31][32], not only spin dynamics, but even the static spin structure of unperturbed TbFeCo are poorly understood. Moreover, experimental studies of high-coercive-field materials are seriously hampered by the need for even higher magnetic fields and thus require unique experimental installations.…”
Section: Introductionmentioning
confidence: 99%
“…HD-AOS induced by LP and CP pulse pairs with different power combinations at a fixed delay time, 1.6 ps, between them were investigated first. The energy transfer for the electron-spin system to the lattice system is mediated by the phonons, which takes about 1.6 ps to reach the spinelectron-lattice thermal equilibrium state [30][31][32] with the system in a largely demagnetized state when the second CP pulse arrives. Figure 4a shows each subtracted MOKE image centered along the scanning path of the dual-pump beam with a field of view of 60 lm  380 lm.…”
Section: Resultsmentioning
confidence: 99%