NOTICE: Due to a lapse in annual appropriations, most of this website is not being updated. Learn more.
Form submissions will still be accepted but will not receive responses at this time. Sections of this site for programs using non-appropriated funds (such as NVLAP) or those that are excepted from the shutdown (such as CHIPS and NVD) will continue to be updated.
An official website of the United States government
Here’s how you know
Official websites use .gov
A .gov website belongs to an official government organization in the United States.
Secure .gov websites use HTTPS
A lock (
) or https:// means you’ve safely connected to the .gov website. Share sensitive information only on official, secure websites.
Differentiation between Strain and Charge Mediated Magnetoelectric Coupling in La0.7Sr0.3MnO3/Pb(Mg1/3Nb2/3)d0.7^Ti0.3O3(001)
Published
Author(s)
T. Bhatnagar-Schoffmann, Emmanuel Kentzinger, A. Sarkar, P. Schoffmann, Q. Lan, L. Jin, A. Kovacs, Alexander Grutter, Brian Kirby, R. Beerwerth, M. Waschk, Annika Stellhorn, U. Rucker, R. E. Dunin-Borkowski, Th. Bruckel
Abstract
Magnetoelectric (ME) coupling in La0.7Sr0.3MnO3/Pb(Mg1/3Nb2/3)d0.7^Ti0.3O3 (LSMO/PMN-PT (001)) has been probed in the past years to identify the underlying mechanism behind it. PMN-PT, which is well known for its excellent piezoelectric properties, also exhibits ferroelectricity. This motivates our interest to differentiate which effect is dominant for this 'Voltage control of magnetism'. Here, we present results for the magnetoelectric coupling at different temperatures: 300 K and 80 K. In this article we discuss and explain, how the nature of ME coupling is influenced by different parameters such as magnetic field, electric field, directional dependence (hard axis, easy axis) and temperature. Owing to large lattice mismatch between LSMO and PMN-PT, the strain-mediated coupling is strongly prevalent, however the change in strain behaviour from butterfly loop to linear loop is observed as a function of temperature. ME measurements are performed along hard axis [100] and easy axis [110] of LSMO in the presence of remanent magnetic field which showcases the pure influence of electric field on the system, resulting in a combination of strain- and charge-mediated coupling. The magnetic depth profile is probed by Polarized Neutron Reflectometry (PNR) as a function of electric field which demonstrates the existence of an interlayer with reduced Nuclear Scattering Length Density (NSLD) and reduced Magnetic Scattering Length Density (MSLD) at the interface. From Transmission Electron Microscopy (TEM), stoichiometric variations are observed due to the presence of Mn3O4 particles at the interface.
Bhatnagar-Schoffmann, T.
, Kentzinger, E.
, Sarkar, A.
, Schoffmann, P.
, Lan, Q.
, Jin, L.
, Kovacs, A.
, Grutter, A.
, Kirby, B.
, Beerwerth, R.
, Waschk, M.
, Stellhorn, A.
, Rucker, U.
, Dunin-Borkowski, R.
and Bruckel, T.
(2020),
Differentiation between Strain and Charge Mediated Magnetoelectric Coupling in La<sub>0.7</sub>Sr<sub>0.3</sub>MnO<sub>3</sub>/Pb(Mg<sub>1/3</sub>Nb<sub>2/3)</sub>d0.7^Ti<sub>0.3</sub>O<sub>3</sub>(001), New Journal of Physics
(Accessed October 7, 2025)