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The magnetic properties of van der Waals magnetic topological insulators MnBi2Te4 and MnBi4Te7 are investigated by magneto-transport measurements. We evidence that the relative strength of the inter-layer exchange coupling J to the uniaxial anisotropy K controls a transition from an A-type antiferromagnetic order to a ferromagnetic-like metamagnetic state. A bi-layer Stoner-Wohlfarth model allows us to describe this evolution, as well as the typical angular dependence of specific signatures, such as the spin-flop transition of the uniaxial antiferromagnet and the switching field of the metamagnet. In micron-size magnets, the single-domain switching-field astroid are however partly truncated by the nucleation of domain walls along the easy-axis direction.References: A. Tan, V. Labracherie, N. Kunchur, A. U. B. Wolter, J. Cornejo, J. Dufouleur, B. Büchner, A. Isaeva and R. Giraud Metamagnetism of Weakly Coupled Antiferromagnetic Topological Insulators. Phys. Rev. Lett. 124, 197201. (2020)

MMM 2020

Meta-Magnetism of Weakly-Coupled Antiferromagnetic Topological Insulators

The 65th Annual Conference on Magnetism and Magnetic Materials (MMM 2020) was held in a virtual form. The COVID-19 pandemic, with its associated uncertainty about international travel and the ability to gather in large groups, meant that the Steering Committee decided to cancel the face-to-face meeting that had been planned in Palm Beach, Florida November 2-6, 2020.

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technical paper

Energy-efficient control of magnetization in nanoscale is fundamental for designing future generation spintronic devices. Current-induced magnetization switching via spin-orbit torques (SOTs), realized in ferromagnet/heavy metal bilayers, has emerged as one of the most promising approaches [1]. The magnitude and the sign of the SOT can be adjusted by optimizing the parameters of the system such as the thickness and the composition of the layers [2]. In this case, however, the SOTs are fixed once the multilayer is fabricated. However, for complex switching concepts, i.e. to selectively switch parts of the ferromagnet using single pulse lines, which may lead to drastically simplified device architectures, it is necessary to locally and dynamically tune the SOTs in a system. Here we demonstrate the possible dynamic control of SOTs in perpendicularly magnetized W/Co20Fe60B20/MgO multilayers by piezoelectric strain [3]. We find that modulated by an electric field, tensile strain increases the damping-like torque by a factor of two, while the compressive strain leads to a decrease. On the contrary, the field-like torque remains largely unaffected by strain. We explain our experimental results with the help of theoretical ab initio calculations revealing the difference in the response of the SOTs to the strain.References: 1. I.M. Miron et al., Nat. Mater. 9, 230 (2010). 2. A. Manchon et al., Rev. Mod. Phys. 91, 035004 (2019). 3. M. Filianina et al., Phys. Rev. Lett. 124, 217701 (2020).

Piezoelectric Strain Control of Spin-Orbit Torques in Perpendicularly Magnetized CoFeB Thin Films

Spin Hall oscillator (SHO) is a promising spin torque oscillator (STO) having high durability due to a small driving current. However, conventional SHOs with in-plane precession (IPP) mode require bias-fields for stable oscillations [1-4], which are not favored in certain applications such as a neuromorphic computing [5]. Here, we propose and theoretically analyze a bias-field-free SHO with an in-plane hard axis and out-of-plane precession (OPP) mode by solving the macrospin Landau-Lifshitz-Gilbert-Slonczewski equation analytically and numerically. Fig. 1 shows the schematic structure of our two-terminal bias-field-free SHO. The SHO consists of a magnetic tunnel junction, a spin source layer, and a shunting resistance. Materials with a small spin Hall angle are also available for the spin source because the shunting resistance provides an in-plane charge current path for a spin current generation by the spin Hall effect. A bias-field-free OPP mode can be obtained by controlling a magnetic hard axis of free layer in the same direction of a spin polarization. In our simulations, the magnetic anisotropy was controlled by demagnetization coefficients without the loss of generality. Fig. 2 shows the typical simulation result of the magnetization dynamics in our SHOs. Bias-field-free oscillations were successfully observed. We also derived formulas for a critical current, a driving current and an oscillation frequency by using the saddle and constant energy approximations [6], and they were in good agreement with numerical simulation results. Furthermore, the drive current of our SHOs were almost ten times smaller than that of conventional bias-field-free STOs.References: [1]L. Liu, C. -F. Pai and D. C. Ralph, Phys. Rev. Lett., Vol. 109, p.186602 (2012) [2]Z. Duan, A. Smith and L. Yang, Nat. Commun., Vol. 5, p.5616 (2014) [3]V. E. Demidov, S. Urazhdin and H. Ulrichs, Nat. Mater., Vol. 11, p.1028 (2012) [4]V. E. Demidov, S. Urazhdin and A. Zholud, Appl. Phys. Lett., Vol. 105, p.172410 (2014) [5]J. Torrejon, M. Riou and F. A. Araujo, Nature, Vol. 547, p.428 (2017) [6]T. Taniguchi and H. Kubota, Phys. Rev. B, Vol. 93, p.174401 (2016)

Bias-field-free spin Hall oscillator with an out-of-plane precession mode

In the spin Hall effect (SHE), a longitudinal charge-current induced transverse pure spin current has been extensively studied for the application of magnetization switching by spin-orbit torque. However, due to the strict right-hand rule among charge current, spin current, and spin polarization, this highly attractive switching scheme is not efficient and often accompanied by an unfavorable external magnetic field in a heterostructure with perpendicular magnetization (PM). In this work, we lift the restriction by demonstrating the magnetization-dependent spin Hall effect (MDSHE) in YIG/PM heterostructure, as shown in Fig. 1. Unlike the conventional SHE with the locked orientation of spin polarization, the spin current induced by the MDSHE can be arbitrarily and independently controlled by the magnetization direction of the magnetic layer. We reported about 3.6% of injected spins experience the effective spin rotation in PM layer of Pt(2)/Co(0.5)/Pt(2). Our approach provides an explicit route in exploring the spin-to-charge conversion with controllable orientations of spin polarization, which offers significant advantages in developing energy-efficient spintronic devices.

Controllable Orientations of Spin Polarization Beyond the Spin Hall Effect

Spin-torque ferromagnetic resonance (ST-FMR) is a common method used to measure spin-orbit torques (SOTs) in heavy metal/ferromagnet bilayer structures. In the course of a measurement, other resonant processes such as spin pumping (SP) and heating can cause spin current or heat flows between the layers, inducing additional resonant voltage signals via the inverse spin Hall effect (ISHE) and Nernst effects (NE). In the standard ST-FMR geometry, these extra artifacts exhibit a dependence on the angle of an in-plane magnetic field that is identical to the rectification signal from the SOTs. We show experimentally that the rectification and artifact voltages can be quantified separately by measuring the ST-FMR signal transverse to the applied current (i.e., in a Hall geometry) in addition to the usual longitudinal geometry. We find that in Pt (6 nm)/CoFeB samples the contribution from the artifacts is small compared to the SOT rectification signal for CoFeB layers thinner than 6 nm, but can be significant for thicker magnetic layers. We observe a sign change in the artifact voltage as a function of CoFeB thickness that we suggest may be due to a competition between a resonant heating effect and the SP/ISHE contribution.

Transverse and Longitudinal Spin-Torque Ferromagnetic Resonance for Improved Measurements of Spin-Orbit Torques

Using the first-principles non-equilibrium Green’s function technique [1] with supercell disorder averaging, we study the influence of interfacial intermixing on the spin-orbit torque in Co/Pt (111) bilayers. The interlayer distances are optimized, several models of intermixing are considered, and atomic potentials in the intermixed layers are obtained using the coherent potential approximation. The magnitude and thickness dependence of the damping-like torque are similar to earlier results for the Co/Pt (001) interface [1,2] and rather insensitive to intermixing. In contrast, the field-like torque, which is small in the case of an ideal interface, is strongly enhanced by intermixing.References: [1] K. D. Belashchenko, A. A. Kovalev, and M. van Schilfgaarde, Phys. Rev. Mater. 3, 011401 (2019). [2] K. D. Belashchenko, A. A. Kovalev, and M. van Schilfgaarde, arXiv:1908.02680.

Effect of interfacial intermixing on spin-orbit torque in Co/Pt bilayers

Weyl semimetals combine both topological and semimetallic effects in their transport of fermions through both bulk and surface states, making them excellent candidates for transverse thermomagnetic transport via the Nernst effect. The Nernst effect is a thermoelectric phenomenon requiring a magnetic field. A temperature gradient is applied to a sample, and the sample is placed in an external magnetic field orthogonal to the temperature gradient. The charge carriers, moving parallel to the temperature gradient, now experience a Lorentz force due to the cross product of the magnetic field and the temperature gradient. An electric field is produced in the mutually perpendicular direction. Single-crystal NbP has shown an unprecedentedly large Nernst thermopower at high magnetic fields, exceeding 800 μV K-1 at 109 K and 9 T [1]. Bulk polycrystalline NbP maintains a large Nernst thermopower, although its magnitude is decreased by approximately a factor of 8 under similar circumstances. Due to the high electrical conductivity of the material, polycrystalline NbP’s Nernst power factor is determined to be 35 x 10-4 W m-1 K-2 at 9 T and 136 K, which is comparable to that of state-of-the-art thermoelectric materials [2]. This high conversion of thermal-to-electrical energy in NbP has been determined as due to the chemical potential’s location near linear, Dirac band crossing points (called Weyl points), giving access to many mobile holes and electrons. These initial results of transverse thermomagnetic transport in both single-crystal and polycrystalline NbP motivate further study to elucidate Weyl fermion transport and the length scales over which it is effective and dominant. Here, we present a grain size study on bulk polycrystalline samples of NbP, where different annealing times result in different grain sizes. Via microstructural characterization and thermomagnetic transport measurements, we can begin to determine the effects of grain size on transport in Weyl semimetals.References: [1] S. J. Watzman et al. Phys. Rev. B 97(16), 161404(R) (2018). [2] C. Fu et al. Energy Environ. Sci. 11(10), 2813-2830 (2018).

Grain Size Dependence of Transverse Thermomagnetic Transport in the Weyl Semimetal NbP

Weyl semimetals (WSMs) are a newly discovered class of quantum materials which can host a number of massless quasiparticles called Weyl fermions. One of the most unique properties of WSMs is the chiral anomaly – a pair of Weyl nodes of opposite chirality acts as source and drain of electrons in the presence of non-perpendicular electric and magnetic fields. To date, the most remarkable phenomenon induced by the chiral anomaly is the longitudinal negative magnetoresistance, which is a linear response effect. In this work, we theoretically investigate the transport properties of WSMs in the nonlinear regime and predict a novel nonlinear Hall effect in tilted non-centrosymmetric Weyl semimetals. Intuitively, a steady-state density difference between a pair of Weyl nodes is established when the chiral pumping and internode relaxation reach a balance, which conspires with the anomalous velocity to give rise to this nonlinear Hall effect. Taking the semiclassical Boltzmann approach, we find that the nonlinear Hall conductivity scales linearly with both the electric and magnetic fields, and depends critically on the tilting of the Weyl cones in both type-I and type-II WSMs. For a pair of Weyl cones that are un-tilted or oppositely tilted, the chiral-anomaly-induced nonlinear Hall current vanishes because it is forbidden by a mirror symmetry. We also show that this effect does not rely on a finite Berry curvature dipole, in contrast to the intrinsic quantum nonlinear Hall effect that was proposed to occur in time-reversal invariant materials [1].References: [1] I. Sodemann and L. Fu, Phys. Rev. Lett. 115, 216806 (2015).

Chiral-Anomaly-Induced Nonlinear Hall Effect in Tilted Weyl Semimetals

We have investigated various electronic transport properties such as the anisotropic magnetoresistance, planar Hall effect, and anomalous Hall effect in kagome Fe3Sn2, which has been predicted to be a type II Weyl metal. Based on magnetortransport, we determine the spin reorientation transition to peak at 120 K and coexistence of both out of plane and in plane phases at temperatures around the spin reorientation, indicative of a first order phase transition. In planar Hall effect, we discover a field antisymmetric contribution in addition to the standard field symmetric contribution. This field antisymmetric planar Hall effect has an in-plane 3-fold rotational symmetry, which is distinctively different from the symmetric counterpart. Furthermore, the temperature and field dependence of the field antisymmetric contribution is different from both the symmetric planar Hall effect and anomalous Hall effect, pointing to a different origin. A linear and antisymmetric planar Hall effect is predicted to be present in the case of non-magnetic Weyl semimetals. The experimental signatures in our case fit well with the prediction in addition to reflecting contributions from its ferromagnetism. As the magnetization of Fe3Sn2 has a 3-fold rotational degeneracy, the associated band structure and Weyl nodes determined by the magnetization direction owing to the spin-orbit coupling will have accordingly a 3-fold rotational degeneracy giving rise to the 3-fold antisymmetric PHE. We thus propose that the antisymmetric PHE that we discovered is the realization of an antisymmetric and linear planar Hall effect due to the presence of Weyl nodes near the Fermi level in a time reversal symmetry broken system. Our finding offers a promising route for macroscopically probing Weyl systems.References: [1] Neeraj Kumar, Y. Soh, Yihao Wang, et al., Anomalous planar Hall effect in a kagome ferromagnet, arXiv:2005.14237 (2020). [2] Nandy, S., G. Sharma, A. Taraphder, et al., Chiral Anomaly as the Origin of the Planar Hall Effect in Weyl Semimetals. Phys Rev Lett, 119(17): p. 176804 (2017). [3] M. Yao, H. Lee, N. Xu, et al., Switchable Weyl nodes in topological Kagome ferromagnet Fe3Sn2, arXiv:1810.01514 (2018).

Anomalous planar Hall effect in predicted type II Weyl Fe3Sn2

YbPtBi is a half Heusler alloy with claimed properties of topological Weyl nodes and chiral anomaly; antiferromagnetism from the RKKY coupling of localized Yb f-electrons at low temperatures; and heavy fermion behaviour as those localized f-electrons interact with the conduction bands [1,2]. So far only bulk crystals have been grown of YbPtBi with no published work on thin films. By using c-plane sapphire the half Heusler alloy has an epitaxially relationship of YbPtBi(111)||Al2O3(0001) and YbPtBi(110)||Al2O3(1100). With thin films we could have to option of induced strain, device fabrication and many other thin films manipulation techniques. In this work, we present a study of epitaxially grown YbPtBi thin films that grew as triangular islands with matched faceted edge orientations. The structure is confirmed to be epitaxial from x-ray diffraction and cross-sectional transmission electron microscopy. We also measure the electrical transport properties and find a non-metallic ρ(T) similar to other semimetals RePtBi (Re=Gd, Ce, Sm) half Heusler Alloy, although different from bulk YbPtBi. We measured a negative longitudinal magnetoresistance and the temperature dependence of an apparent chiral anomaly (Fig: a,b). Both of which are indicators of a possible Weyl semimetal state. We also obversed a large hysteretic MR at very low temperatures, 250 mK, not previously seen in YbPtBi.References: [1] C. Y. Guo, F. Wu, Z. Z. Wu, M. Smidman, C. Cao, A. Bostwick, C. Jozwiak, E. Rotenberg,Y. Liu, F. Steglich, and H. Q. Yuan, Nature Communications. 9, 4622 (2018) [2] B. G. Ueland, A. Kreyssig, E. D. Mun, J. W. Lynn, L. W. Harriger, D. K. Pratt, K. Prokeš, Z. Hüsges, R. Toft-Petersen, S. Sauerbrei, S. M. Saunders, Y. Furukawa, S. L. Bud’ko, R. J.McQueeney, P. C. Canfield, and A. I. Goldman, Phys. Rev. B. 99, 184431 (2019)

Epitaxial Growth Of The Weyl Semimetal YbPtBi (111) On C-plane Sapphire By Co-Sputtering

How strong correlations drive quantum states of matter with nontrivial topology is an outstanding issue in contemporary condensed matter physics. This talk will provide an overview and discuss the latest development on Weyl-Kondo semimetal, which has been concurrently advanced by theoretical [1,2] and experimental [3,4,5] studies. The theoretical work addressed a nonsymmorphic Anderson lattice model that breaks the inversion symmetry while preserving the time-reversal symmetry, whereas the experimental effort focused on the non-magnetic non-centrosymmetric and non-symmorphic heavy fermion semimetal Ce3Bi4Pd3. The salient signatures of the Weyl-Kondo semimetal include a correlation enhanced specific heat C=ΓT3 [3], and a giant zero-magnetic-field Hall response and even-in-field Hall effects [4]. The latest high magnetic field experiments observed a two-stage topological phase transition, from Weyl-Kondo semimetal to Kondo insulator to heavy-fermion metal [5]. To bridge the latest experiments and our theoretical work, we investigated the aforementioned Anderson lattice model in the presence of a Zeeman coupling. Tuning both the Zeeman coupling and the inversion-symmetry-breaking potential controls the position and number of Weyl nodes in the Brillouin zone, and several topologically distinct phases emerge in this model.References: [1] H.-H. Lai, S. E. Grefe, S. Paschen, and Q. Si, Proc. Natl. Acad. Sci. U.S.A. 115, 93 (2018). [2] S. E. Grefe, H.-H. Lai, S. Paschen, and Q. Si, Phys. Rev. B, 101, 075138 (2020). [3] S. Dzsaber, L. Prochaska, A. Sidorenko, G. Eguchi, R. Svagera, M. Waas, A. Prokofiev, Q. Si, and S. Paschen, Phys. Rev. Lett. 118, 246601 (2017). [4] S. Dzsaber, X. Yan, G. Eguchi, A. Prokofiev, T. Shiroka, P. Blaha, O. Rubel, S. E. Grefe, H.-H. Lai, Q. Si, and S. Paschen., arXiv preprint arXiv:1811.02819, (2018). [5] S. Dzsaber, D. A. Zocco, A. McCollam, F. Weickert, R. McDonald, M. Taupin, X. Yan, A. Prokofiev, L. M. K. Tang, B. Vlaar, et al., arXiv preprint arXiv:1906.01182 (2019).

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