% IMPORTANT: The following is UTF-8 encoded. This means that in the presence
% of non-ASCII characters, it will not work with BibTeX 0.99 or older.
% Instead, you should use an up-to-date BibTeX implementation like “bibtex8” or
% “biber”.
@INPROCEEDINGS{Hutanu:840586,
author = {Hutanu, Vladimir and Sazonov, Andrew and Roth and Murakawa
and Tokura and Bordacs and Kezsmarki and Nafradi and Braden
and Stein and Baum and Oh,},
title = {{S}pherical neutron polarimetry in multiferroics under
external stimuli},
volume = {A70},
issn = {0108-7673},
address = {Oxford [u.a.]},
publisher = {Blackwell},
reportid = {FZJ-2017-08091},
pages = {C151},
year = {2014},
abstract = {Study of multiferroics, materials simultaneously having
more than one primary ferroic order parameter, is a hot
topic of mate rial sciences. The most extensively studied
class of these compounds is the family of magnetoelectric
multiferroics, where ferroelectricity can be induced by
various types of magnetic orderings via the relativistic
spin-orbit interaction. As a consequence of the cross
coupling between spins and electric polarization, the
spectacular control of the ferroelectric polarization by
external magnetic field and the manipulation of the magnetic
order via electric field can often be realized in these
systems. Depending on the symmet ry and microscopic
mechanism of the multiferroicity the coupling energy between
magnetic and electric ordering parameters can significantly
vary. Classical neutron diffraction often fails in the
precise determining of the complex magnetic structure in the
multiferroics due to the presence of the statistically
distributed domains in the macroscopic sample. Using
spherical neutron polarimetry (SNP), known also as 3D
polarization analysis, it is possible not only to precisely
determine the complex magnetic structure, but also to
investigate in-situ its evolution with external parameters
and to control the magnetic domains distribution under the
influence of the external electric or/and magnetic field.
Here we will present some SNP results on few different mu
ltiferroic materials. In some of them, e.g. square lattice
2D antiferromagnet Ba2CoGe2O7, even strong electric field
does not change the magnetic order. However rater week
magnetic field is sufficient to create a mono-domain
structure and to rotate spins in the plane. In other e.g.
incommensurate (spiral) magnetic structure of the TbMnO3,
solely electric field is sufficient to fully control the
chirality of the magnetic structure. In the case of Cr2O3
both electric and magnetic fields should be applied in
parallel in order to switch between the different
antiferromagnetic domains.},
month = {Aug},
date = {2014-08-05},
organization = {Twenty-Third Congress and General
Assembly of the International Union of
Crystallography, Montreal (Canada), 5
Aug 2014 - 12 Aug 2014},
cin = {JCNS (München) ; Jülich Centre for Neutron Science JCNS
(München) ; JCNS-FRM-II / JCNS-2 / JARA-FIT},
ddc = {530},
cid = {I:(DE-Juel1)JCNS-FRM-II-20110218 /
I:(DE-Juel1)JCNS-2-20110106 / $I:(DE-82)080009_20140620$},
pnm = {524 - Controlling Collective States (POF3-524) / 6212 -
Quantum Condensed Matter: Magnetism, Superconductivity
(POF3-621) / 6G15 - FRM II / MLZ (POF3-6G15) / 6G4 - Jülich
Centre for Neutron Research (JCNS) (POF3-623)},
pid = {G:(DE-HGF)POF3-524 / G:(DE-HGF)POF3-6212 /
G:(DE-HGF)POF3-6G15 / G:(DE-HGF)POF3-6G4},
experiment = {EXP:(DE-MLZ)POLI-HEIDI-20140101},
typ = {PUB:(DE-HGF)8},
url = {https://juser.fz-juelich.de/record/840586},
}