APS March Meeting 2011
Volume 56, Number 1
Monday–Friday, March 21–25, 2011;
Dallas, Texas
Session H33: Focus Session: Dielectric, Ferroelectric, and Piezoelectric Oxides: Multiferroics & Magnetoelectrics I
8:00 AM–11:00 AM,
Tuesday, March 22, 2011
Room: C143/149
Sponsoring
Units:
DMP DCOMP
Chair: Dipanjan Mazumdar, University of Alabama
Abstract ID: BAPS.2011.MAR.H33.1
Abstract: H33.00001 : Changing Dielectrics into Multiferroics---Alchemy Enabled by Strain
8:00 AM–8:36 AM
Preview Abstract
Abstract
Author:
Darrell Schlom
(Cornell University)
Ferroelectric ferromagnets are exceedingly rare, fundamentally
interesting
multiferroic materials. The properties of what few compounds
simultaneously
exhibit these phenomena pale in comparison to useful
ferroelectrics or
ferromagnets: their spontaneous polarizations ($P_{s})$ or
magnetizations
($M_{s})$ are smaller by a factor of 1000 or more. The same holds
for
(magnetic or electric) field-induced multiferroics. Recently,
however,
Fennie and Rabe proposed a new route to ferroelectric
ferromagnets\footnote{C.J. Fennie and K.M. Rabe, \textit{Phys.
Rev. Lett.}
\textbf{97} (2006) 267602.}---transforming magnetically ordered
insulators
that are
neither ferroelectric nor ferromagnetic, of which there are many,
into
ferroelectric ferromagnets using a single control parameter:
strain. The
system targeted, EuTiO$_{3}$, was predicted to simultaneously
exhibit strong
ferromagnetism ($M_{s}$~$\sim $~7~$\mu _{B}$/Eu) and strong
ferroelectricity ($P_{s}$~$\sim $~10~$\mu $C/cm$^{2})$ under
large biaxial
compressive strain. These values are orders of magnitude higher
than any
known ferroelectric ferromagnet and rival the best materials that
are solely
ferroelectric or ferromagnetic. Hindered by the absence of an
appropriate
substrate to provide the desired compression, we show$^{3}$ both
experimentally and theoretically the emergence of a multiferroic
state under
biaxial \textit{tension} with the unexpected benefit that even
lower misfits are
required, thereby enabling higher quality crystalline films. The
resulting genesis of a strong ferromagnetic ferroelectric points
the way to
high temperature manifestations of this spin-phonon coupling
mechanism.\footnote{J.H. Lee and K.M. Rabe, \textit{Phys. Rev.
Lett.} \textbf{104}
(2010) 207204.} Our work\footnote{J.H. Lee, L. Fang, E. Vlahos,
X. Ke, Y.W. Jung, L. Fitting
Kourkoutis, J-W. Kim, P.J. Ryan, T. Heeg, M. Roeckerath, V.
Goian, M. Bernhagen, R. Uecker, P.C. Hammel, K.M. Rabe, S. Kamba,
J. Schubert, J.W. Freeland, D.A. Muller, C.J. Fennie, P.
Schiffer, V. Gopalan, E. Johnston-Halperin, and D.G. Schlom,
\textit{Nature} \textbf{466} (2010) 954-958.} demonstrates that a
single
experimental
parameter, strain, simultaneously controls multiple order
parameters and is
a viable alternative tuning parameter to composition for creating
multiferroics.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2011.MAR.H33.1