001     834127
005     20210129230545.0
037 _ _ |a FZJ-2017-04126
100 1 _ |a Freimuth, Frank
|0 P:(DE-Juel1)130643
|b 0
|e Corresponding author
|u fzj
111 2 _ |a Spincaloritronics VIII
|c Regensburg
|d 2017-06-12 - 2017-06-15
|w Germany
245 _ _ |a Thermal and electrical spin-orbit torques in collinear and noncollinear magnets
260 _ _ |c 2017
336 7 _ |a Conference Paper
|0 33
|2 EndNote
336 7 _ |a Other
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336 7 _ |a INPROCEEDINGS
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336 7 _ |a Conference Presentation
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520 _ _ |a While spin-orbit torques [1] in magnetic bilayers composed of a 5d transition metal layer and a ferromagnetic layer can serve as a competitive alternative to the Slonczewski spin-transfer torque in spin-valves and magnetic tunnel junctions in order to realize MRAM devices, spin-orbit torques have even more potential, and are a potential game-changer, in antiferromagnetic spintronics [2] and in noncollinear magnets. After discussing the theory of thermal and electrical spin-orbit torques in collinear magnets, we will shift the focus to current-induced torques and spin-orbit driven effects in noncollinear magnetic bilayers. The combination of structural inversion asymmetry present in the bilayer geometry with noncollinear magnetism leads to several additional spin-orbit driven effects, such as the Dzyaloshinskii-Moriya interaction [3,4,5,6] and chiral damping [7], which join the other effects and current-induced torques important in noncollinear magnets and magnetic bilayers, such as spin-transfer torque, spin-orbit torque and nonadiabatic torque. In particular the combined action of the Dzyaloshinskii-Moriya interaction and the spin-orbit torque from the spin Hall effect enables current-driven domain-wall motion at ultrahigh speeds [8,9]. The large number of current-induced torques and spin-orbit driven effects participating in the current-induced motion of domain-walls or skyrmions are difficult to disentangle and to quantify in experimental measurements. First-principles density functional theory is an ideal tool to understand and to quantify these effects. For this purpose we extend our computational formalism of spin-orbit torques [10,11,12] to noncollinear magnets. An important problem in the formalism development concerns the correct inclusion of vertex corrections, without which several components of the current-induced torques in noncollinear chiral magnets would violate conservation laws. We will discuss the current-induced torques and spin-orbit driven effects that arise from the combination of structural inversion asymmetry, spin-orbit coupling, and noncollinear magnetism in Co/Pt and Mn/W bilayer systems. References: [1] K. Garello et al., Nature Nanotechnology 8, 587 (2013), [2] P. Wadley et al., Science 351, 587 (2016), [3] F. Freimuth et al., JPCM 26, 104202 (2014), [4] F. Freimuth et al., PRB 88, 214409 (2013), [5] F. Freimuth et al., JPCM 28, 316001 (2016), [6] F. Freimuth et al., ArXiv e-prints (2016), 1610.06541, [7] E. Jue et al., Nature Materials 15, 272 (2016), [8] L. Thomas et al., Nature Nanotechnology 8, 527 (2013), [9] S. Emori et al., Nature Materials 12, 611 (2013), [10] F. Freimuth et al., PRB 92, 064415 (2015), [11] F. Freimuth et al., PRB 90, 174423 (2014), [12] G. Geranton et al., PRB 91, 014417 (2015)
536 _ _ |a 142 - Controlling Spin-Based Phenomena (POF3-142)
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909 C O |o oai:juser.fz-juelich.de:834127
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910 1 _ |a Forschungszentrum Jülich
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914 1 _ |y 2017
920 1 _ |0 I:(DE-Juel1)IAS-1-20090406
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|l Quanten-Theorie der Materialien
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920 1 _ |0 I:(DE-82)080009_20140620
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980 _ _ |a conf
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