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@ARTICLE{Kotla:637354,
author = {Kotla, Surya Rohith and Noohinejad, Leila and Pokhriyal,
Preeti and Tolkiehn, Martin and AGARWAL, HARSHIT and
Ramakrishnan, Sitaram and van Smaalen, Sander},
title = {{B}roken inversion symmetry in the charge density wave
phase in {E}u{A}l$_4$},
journal = {Physical review / B},
volume = {112},
number = {6},
issn = {2469-9950},
address = {Woodbury, NY},
publisher = {Inst.},
reportid = {PUBDB-2025-03846},
pages = {064113},
year = {2025},
abstract = {EuAl$_4$ exhibits a complex phase diagram, including the
development of a charge density wave (CDW) below
$T_{\mathrm{CDW}}$ = 145K. Below $T_N$ = 15.4K, a series of
antiferromagnetically (AFM) ordered phases appear, while
nontrivial topological phases, like skyrmion lattices, are
stabilized under an applied magnetic field. The symmetries
of the variously ordered phases are a major issue concerning
the understanding of the stabilization of the ordered phases
as well as concerning the interplay between the various
types of order. EuAl$_4$ at room temperature has tetragonal
symmetry with space group I4/mmm. The CDW phase has an
incommensurately modulated crystal structure described by
the modulation wave vector q ≈ 0.17 c$^{∗}$. On the
basis of various experiments, including elastic and
inelastic x-ray scattering, and second-harmonic generation,
it has been proposed that the symmetry of the CDW phase of
EuAl$_4$ could be centrosymmetric orthorhombic,
noncentrosymmetric orthorhombic or noncentrosymmetric
tetragonal. Here, we report temperature-dependent,
single-crystal x-ray diffraction experiments that show that
the CDW is a transverse CDW with phason disorder, and with
noncentrosymmetric symmetry according to the orthorhombic
superspace group F222(0 0 σ )00s. Essential for this
finding is the availability of a sufficient number of
second-order (2q) satellite reflections in the x-ray
diffraction data set. The broken inversion symmetry implies
that skyrmions might form due to Dzyaloshinskii-Moriya (DM)
interactions, instead of a more exotic mechanism as it is
required for centrosymmetric structures.},
cin = {FS DOOR-User / FS-PET-D},
ddc = {530},
cid = {$I:(DE-H253)FS_DOOR-User-20241023$ /
I:(DE-H253)FS-PET-D-20190712},
pnm = {632 - Materials – Quantum, Complex and Functional
Materials (POF4-632) / 6G3 - PETRA III (DESY) (POF4-6G3) /
FS-Proposal: I-20231047 (I-20231047) / DFG project
G:(GEPRIS)406658237 - Aperiodische Kristalle: Struktur,
Dynamik und elektronische Eigenschaften (406658237)},
pid = {G:(DE-HGF)POF4-632 / G:(DE-HGF)POF4-6G3 /
G:(DE-H253)I-20231047 / G:(GEPRIS)406658237},
experiment = {EXP:(DE-H253)P-P24-20150101},
typ = {PUB:(DE-HGF)16},
doi = {10.1103/kl2z-brms},
url = {https://bib-pubdb1.desy.de/record/637354},
}