2006 APS March Meeting
Monday–Friday, March 13–17, 2006;
Baltimore, MD
Session W20: Focus Session: Multiferroics IV
2:30 PM–5:30 PM,
Thursday, March 16, 2006
Baltimore Convention Center
Room: 317
Sponsoring
Units:
DMP GMAG
Chair: Sang-Wook Cheong, Rutgers University
Abstract ID: BAPS.2006.MAR.W20.4
Abstract: W20.00004 : Magnetoelectric effects in multiferroics
3:06 PM–3:42 PM
Preview Abstract
Abstract
Author:
Alois Loidl
(Center for Electronic Correlations and Magnetism, University of Augsburg)
Magneto-electric phenomena were investigated in two different multiferroic
systems: The strong coupling of dielectric and magnetic properties and the
simultaneous occurrence of long-range magnetic and ferroelectric order are
discussed for rare earth manganites and sulfo spinels. A phase diagram of
Eu$_{1-x}$Y$_{x}$MnO$_{3}$ is established, which recovers the main features
of the well-known magneto-electric phase diagram for the pure rare earth
manganites RMnO$_{3}$. Here a variety of magnetic and electric phases emerge
with varying rare earth ions R. As function of temperature and external
magnetic field, also Y doped EuMnO$_{3 }$compounds undergo a sequence of
different magnetic and polar phase transitions for varying effective ionic
radii of the rare earth ions. Special attention is paid to the occurrence of
fundamentally new hybrid spin-electromagnetic excitations, which we name
electromagnons and are characterized as spin waves that can be excited by an
ac electric field. These excitations are identified in
Eu$_{1-x}$Y$_{x}$MnO$_{3 }$with x = 0.2, in GdMnO$_{3}$, and in TbMnO$_{3}$.
Specifically in GdMnO$_{3}$ the electromagnons can easily be suppressed by
external magnetic fields and allow tuning the index of refraction by
moderate fields.
In the second part we discuss the simultaneous appearance of colossal
magneto-resistance (CMR) and colossal magneto-capacitance (CMC) effects in
chromium sulfo spinels. In CdCr$_{2}$S$_{4}$ ferromagnetism of localized Cr
spins evolves at 85 K, while polar order is established below 130 K. The
onset of ferroelectric order is neither accompanied by the occurrence of
soft modes nor by structural changes which break the inversion symmetry of
the high-temperature cubic phase. HgCr$_{2}$S$_{4}$ becomes ferroelectric
close to 70 K while a complex antiferromagnetic order is found below 25 K.
CMR and CMC effects are specifically strong in the mercury compound, as
moderate magnetic fields of only 0.1 T induce ferromagnetism at much higher
temperatures. We speculate that the occurrence of ferroelectricity in these
multiferroic compounds is rather of electronic than of ionic origin.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2006.MAR.W20.4