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@INPROCEEDINGS{Kiefer:1034066,
author = {Kiefer, Lara and Wirth, Felix and Bertin, Alexandre and
Becker, Petra and Bohatý, Ladislav and Schmalzl, Karin and
Stunault, Anne and Alberto Rodríguez-Velamazán, J. and
Fabelo, Oscar and Braden, Markus},
title = {{C}rystal structure and absence of magnetic order in single
crystalline {R}u{O}2},
reportid = {FZJ-2024-06887},
year = {2024},
abstract = {RuO2 initially attracted interest in the field of catalysts
and microelectronics, but the recent reportof
antiferromagnetic order occurring above room temperature and
its identificationas an altermagnetic state boosted
activities on this material [1,2,3].The combination of spin
splitting otherwise characteristic for ferromagnetic order
with the linearmagnon dispersion of an antiferromagnetic
system may open the path to applications in spintronicsand
magnonics [4].However, even the occurrence of magnetic order
in RuO2 was recently questioned by muon andneutron
experiments as well as by DFT calculations [5-7] and it was
proposed that magnetic orderonly occurs in the presence of
vacancies [5].We, therefore, performed polarized and
unpolarized neutron diffraction experiments on RuO2
crystalsthat were characterized by magnetization and
electrical conductance measurements as well asby X-ray
diffraction [8].Single crystals were grown by chemical vapor
transport using two different transport molecules.In
addition a powder sample was obtained by annealing a
commercial compound.The neutron experiments were performed
on D9, D3 and IN12 and the crystal structure was
investigatedon a Bruker D8 venture diffractometer. We were
not able to confirm the proposed structuraldistortion in our
crystals down to 2K. There are no superstructure reflections
[3]breaking the symmetry of the rutile-type structure in the
X-ray and long-wave length neutron experiments.Such peaks
are observed for short neutron wave lengths but can be
attributed to multiplediffraction. The amount of ruthenium
vacancies is below a few per cent in our crystals.
Polarizedneutron experiments do not indicate magnetic Bragg
reflections for the proposed propagation vectorof
⃗k=(0,0,0) [3]. Even magnetic order with a five times
smallerordered moment than what is claimed [3] would have
yielded significant intensities in our experiment.This
antiferromagnetic order can be ruled out in our
stoichiometric samples [8].[1] L. Smejkal et al., 2022,
Phys. Rev. X 12(3), 031042.[2] L. Smejkal et al., 2022,
Phys. Rev. X 12(4), 040501.[3] T. Berjilin et al., 2017,
Phys. Rev. Lett. 118, 077201.[4] L. Smejkal et al., 2023,
Phys. Rev. Lett. 131, 256703.[5] A. Smolyanyuk et al., 2024,
Phys. Rev. B. 109, 134424.[6] M. Hiraishi et al., 2024,
Phys. Rev. Lett. 132, 166702.[7] P. Keßler et al., 2024,
npj Spintronics 2, 50.[8] L. Kiefer et al., 2024, arXiv,
2410.05850.23},
month = {Dec},
date = {2024-12-11},
organization = {Flipper 2024 as a satellite workshop
of the ILL/ESS user meeting, Institut
Laue-Langevin (ILL) located on the
European Photon and Neutron (EPN)
campus (France), 11 Dec 2024 - 13 Dec
2024},
subtyp = {Invited},
cin = {JCNS-2 / JARA-FIT / JCNS-ILL},
cid = {I:(DE-Juel1)JCNS-2-20110106 / $I:(DE-82)080009_20140620$ /
I:(DE-Juel1)JCNS-ILL-20110128},
pnm = {632 - Materials – Quantum, Complex and Functional
Materials (POF4-632) / 6G4 - Jülich Centre for Neutron
Research (JCNS) (FZJ) (POF4-6G4)},
pid = {G:(DE-HGF)POF4-632 / G:(DE-HGF)POF4-6G4},
experiment = {EXP:(DE-Juel1)ILL-IN12-20150421},
typ = {PUB:(DE-HGF)6},
url = {https://juser.fz-juelich.de/record/1034066},
}