2018
DOI: 10.1103/physrevb.98.024422
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Full angular dependence of the spin Hall and ordinary magnetoresistance in epitaxial antiferromagnetic NiO(001)/Pt thin films

Abstract: We report the observation of the three-dimensional angular dependence of the spin Hall magnetoresistance (SMR) in a bilayer of the epitaxial antiferromagnetic insulator NiO(001) and the heavy metal Pt, without any ferromagnetic element. The detected angular-dependent longitudinal and transverse magnetoresistances are measured by rotating the sample in magnetic fields up to 11 T, along three orthogonal planes (xy-, yz-and xz-rotation planes, where the z-axis is orthogonal to the sample plane). The total magneto… Show more

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Cited by 129 publications
(126 citation statements)
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References 45 publications
(96 reference statements)
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“…for Ip along E3, E2, and E1, respectively, as expected from the angular dependence of the damping-like SOT induced SH-AHE. 6,9,32 To corroborate the results in Fig. 2d, we use an independent approach to control the Néel order by an applied field (H) which aligns n  H via the in-plane spin-flop (SF) transition once H exceeds the SF field.…”
mentioning
confidence: 81%
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“…for Ip along E3, E2, and E1, respectively, as expected from the angular dependence of the damping-like SOT induced SH-AHE. 6,9,32 To corroborate the results in Fig. 2d, we use an independent approach to control the Néel order by an applied field (H) which aligns n  H via the in-plane spin-flop (SF) transition once H exceeds the SF field.…”
mentioning
confidence: 81%
“…2d, we use an independent approach to control the Néel order by an applied field (H) which aligns n  H via the in-plane spin-flop (SF) transition once H exceeds the SF field. Figure 2e shows an angular This indicates that the SF transition in our α-Fe2O3 films occurs at below 1 T with the total Néel order n  H. 32,33 The peak-to-valley magnitude of ΔRxy in Fig. 2e is 0.27 , which gives the upper limit of Hall resistance change in Pt/α-Fe2O3 switching measurement.…”
mentioning
confidence: 81%
“…The most extensively used FMI in insulating spintronics is yttrium iron garnet or YIG (Y 3 Fe 5 O 12 ), due to its low Gilbert damping, soft ferrimagnetism and negligible magnetic anisotropy 1,[4][5][6][7][10][11][12][13][14][15]17,18,[21][22][23][24][25][26][27][28][29][30] . Alternative magnetic insulators include antiferromagnets [31][32][33] , non-collinear magnets [34][35][36] , hexagonal ferrites 8 , ferrimagnetic spinels 19,[37][38][39] and other ferrimagnetic garnets 9,[40][41][42][43][44][45] .…”
Section: Introductionmentioning
confidence: 99%
“…Much of this research focuses on interactions involving magnons or spin waves at magnetic interfaces in hybrid structures. Examples of this are spin pumping [13][14][15][16][17][18][19], spin transfer [15,[20][21][22], and spin Hall magnetoresistance [23][24][25][26][27][28] at normal metal interfaces, and magnon-mediated superconductivity [9,10]. Recently, an experiment has also demonstrated spin transport in an antiferromagnetic insulator over distances up to 80 µm [29].…”
mentioning
confidence: 99%