APS March Meeting 2016
Volume 61, Number 2
Monday–Friday, March 14–18, 2016;
Baltimore, Maryland
Session X19: Magnetic Oxide Thin Films and Heterostructures: Electrostatic, Ionic, and Magnetoelectric Coupling
8:00 AM–11:00 AM,
Friday, March 18, 2016
Room: 318
Sponsoring
Units:
GMAG DMP
Chair: Philip Ryan, Argonne National Laboratory
Abstract ID: BAPS.2016.MAR.X19.1
Abstract: X19.00001 : Electric-Field Coupling to Spin Waves in a Centrosymmetric Ferrite
8:00 AM–8:36 AM
Preview Abstract
Abstract
Author:
Tianyu Liu
(Optical Science and Technology Center and Department of Physics and Astronomy, University of Iowa, Iowa City, Iowa 52242, USA)
A systematic control of spin waves via external electric fields has been a long standing issue for the design of magnonic devices, and is of fundamental interest. One way to attain such control is to use multiferroics [1], whose electric and magnetic polarizations are inherently coupled. The lack of electric polarization in a centrosymmetric ferrite, however, makes direct coupling of its magnetization to external electric fields a challenge. Indirect electric control of spin waves has been accomplished by hybridizing yttrium iron garnet (YIG), a centrosymmetric ferrite, with a piezoelectric material [2]. Here, we predict direct control of spin waves in YIG by {\it a flexoelectric interaction}, which couples an electric field to the spatial gradient of the magnetization, and thus the spin waves [3]. Based on a superexchange model, which describes the antiferromagnetic coupling between two nearest neighbor iron ions through an oxygen ion, including spin-orbit coupling, we estimate the coupling constant and predict a phase shift linear in the applied electric fields [4]. The theory is then confirmed by experimental measurement of the electric-field-induced phase shift in a YIG waveguide [5]. In addition to the flexoelectric effect, another electric effect is observed, which couples the electric field directly with the magnetization of YIG. We call this a magnetoelectric effect. By adjusting the direction of the electric field, the two effects can be well separated. Experimental results agree quantitatively with the theoretical prediction. A phenomenological coupling constant for the magnetoelectric effect is also obtained. Our findings point to an important avenue for manipulating spin waves and developing electrically tunable magnonic devices.
[1] P. Rovillain \textit{et al}., Nat. Mater. {\bf 9}, 975 (2010).
[2] M. Bao \textit{et al}., Appl. Phys. Lett. {\bf 101}, 022409 (2012).
[3] T. Liu and G. Vignale, J. Appl. Phys. {\bf 111}, 083907 (2012).
[4] T. Liu and G. Vignale, Phys. Rev. Lett. {\bf 106}, 247203 (2011).
[5] X. Zhang \textit{et al}., Phys. Rev. Lett. {\bf 113}, 037202 (2014).
[6]The author gratefully acknowledges collaborations with G. Vignale, M.E. Flatte', X. Zhang and H. X. Tang. This work is supported by DARPA MESO and an ARO MURI.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2016.MAR.X19.1