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@INPROCEEDINGS{Hutanu:859536,
author = {Hutanu, V. and Kousaka, Y. and Ohishi, K. and Kakurai, K.
and Roth, G.},
title = {{C}rystal chirality versus magnetic chirality in
{C}s{C}u{C}l3 determined by neutron polarization analysis},
reportid = {FZJ-2019-00388},
year = {2018},
abstract = {The concept of chirality, meaning left- or
right-handedness, plays an essential role in symmetry
properties of nature at all length scales from elementary
particles to cosmic science. In material sciences, it is
very important to understand the chirality in molecules,
crystals and magnetic structures both from theoretical and
experimental points of view. Chiral helimagnetic ordering,
forming only right- or left-handed spiral magnetic
structure, has attract much attention in the last time due
to unique magnetic textures such as skyrmion and chiral
magnetic soliton lattice [1, 2]. Therefore, it is very
important to investigate the interplay between
crystallographic and helimagnetic chirality. However, only
very few experimental results on this interplay are reported
up to now, due to the difficulty to synthesize homo-chiral
single crystals, which consisting solely of right- or
left-handed crystalline domains.Using novel two-step
crystallization technique under stirring we succeeded in
obtaining the cm-large ordered homo-chiral single crystals
of CsCuCl3 with desired handedness [3]. Circular-polarized
synchrotron radiation at SPring 8, J-Park was employed to
determine the handedness of the crystal symmetry in
different samples [4]. Below 10.5 K a proper-screw magnetic
order with propagation vector k=(1/3,1/3, ±δ) with (δ ∼
0.09) is formed in CsCuCl3. The magnetic chirality of the
homo-chiral crystals was investigated using polarized single
crystal diffractometer POLI at MLZ. Our experimental results
revealed that the handedness of the magnetic helicity is
coupled and directly controlled by the crystallographic
lattice chirality [5]. The results could be understood in
terms of Dzyaloshinskii-Morya interaction strongly coupled
to the lattice, lifting the helix chiral
degeneracy.References:1. S. Muhlbauer et al., Science 323,
915 (2009).2. Y. Togawa et al., Phys. Rev. Lett. 108, 107202
(2012).3. Y. Kousaka et al., J.Phys.: Conf. Series 502
012019 (2014).4. H. Ohsumi et al., Angew. Chem., Int. Ed.
52, 8718 (2013).5. Y. Kousaka et al., Phys. Rev. Materials,
1, 071402(R) (2017).},
month = {Mar},
date = {2018-03-05},
organization = {26th Annual Meeting of the German
Crystallographic Society, Essen
(Germany), 5 Mar 2018 - 8 Mar 2018},
subtyp = {After Call},
cin = {JCNS-FRM-II / JCNS-2 / JARA-FIT},
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)6},
url = {https://juser.fz-juelich.de/record/859536},
}