APS March Meeting 2017
Volume 62, Number 4
Monday–Friday, March 13–17, 2017;
New Orleans, Louisiana
Session L47: Spin-Orbit Torque II
11:15 AM–2:15 PM,
Wednesday, March 15, 2017
Room: 394
Sponsoring
Units:
GMAG DMP FIAP
Chair: Joseph Sklenar, University of Illinois at Urbana-Champaign
Abstract ID: BAPS.2017.MAR.L47.4
Abstract: L47.00004 : Spin-Orbit Torque-Assisted Switching in Magnetic Insulator Thin Films with Perpendicular Magnetic Anisotropy
11:51 AM–12:27 PM
Preview Abstract
Abstract
Author:
Mingzhong Wu
(Department of Physics, Colorado State University)
As an in-plane charge current flows in a heavy metal film with spin-orbit
coupling, it produces a torque that can induce magnetization switching in a
neighboring ferromagnetic metal film. Such spin-orbit torque (SOT)-induced
switching has been studied extensively in recent years and has shown higher
efficiency than switching using conventional spin-transfer torque. This
presentation reports the SOT-assisted switching in heavy metal/magnetic
insulator systems.$^{\mathrm{1}}$ The experiments made use of
Pt/BaFe$_{\mathrm{12}}$O$_{\mathrm{19}}$ bi-layered structures. Thanks to
its strong spin-orbit coupling, Pt has been widely used to produce pure spin
currents in previous studies. BaFe$_{\mathrm{12}}$O$_{\mathrm{19}}$ is an
M-type barium hexagonal ferrite and is often referred as BaM. It is one of
the few magnetic insulators with strong magneto-crystalline anisotropy and
shows an effective uniaxial anisotropy field of about 17 kOe. It's found
that the switching response in the BaM film strongly depends on the charge
current applied to the Pt film. When a constant magnetic field is applied in
the film plane, the charge current in the Pt film can switch the normal
component of the magnetization ($M_{\mathrm{\bot }})$ in the BaM film between
the up and down states. The current also dictates the up and down states of
the remnant magnetization when the in-plane field is reduced to zero. When
$M_{\mathrm{\bot }}$ is measured by sweeping an in-plane field, the response
manifests itself as a hysteresis loop, which evolves in a completely
opposite manner if the sign of the charge current is flipped. When the
coercivity is measured by sweeping an out-of-plane field, its value can be
reduced or increased by as much as about 500 Oe if an appropriate charge
current is applied.
1. P. Li, T. Liu, H. Chang, A. Kalitsov, W. Zhang, G. Csaba, W. Li, D.
Richardson, A. Demann, G. Rimal, H. Dey, J. S. Jiang, W. Porod, S. Field, J.
Tang, M. C. Marconi, A. Hoffmann, O. Mryasov, and M. Wu, Nature Commun.
7:12688 doi: 10.1038/ncomms12688 (2016).
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2017.MAR.L47.4