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@ARTICLE{Tymoshenko:840399,
author = {Tymoshenko, Y. V. and Onykiienko, Y. A. and Müller, T. and
Thomale, R. and Rachel, S. and Cameron, A. S. and
Portnichenko, P. Y. and Efremov, D. V. and Tsurkan, V. and
Abernathy, D. L. and Ollivier, J. and Schneidewind, Astrid
and Piovano, A. and Felea, V. and Loidl, A. and Inosov, D.
S.},
title = {{P}seudo-{G}oldstone {M}agnons in the {F}rustrated {S}=3=2
{H}eisenberg {H}elimagnet {Z}n{C}r2{S}e4with a {P}yrochlore
{M}agnetic {S}ublattice},
journal = {Physical review / X},
volume = {7},
issn = {2160-3308},
address = {College Park, Md.},
publisher = {APS},
reportid = {FZJ-2017-07932},
pages = {041049},
year = {2017},
abstract = {Low-energy spin excitations in any long-range ordered
magnetic system in the absence of
magnetocrystallineanisotropy are gapless Goldstone modes
emanating from the ordering wave vectors. Inhelimagnets,
these modes hybridize into the so-called helimagnon
excitations. Here we employ neutronspectroscopy supported by
theoretical calculations to investigate the magnetic
excitation spectrum of theisotropic Heisenberg helimagnet
ZnCr2Se4 with a cubic spinel structure, in which spin-3=2
magnetic Cr3þions are arranged in a geometrically
frustrated pyrochlore sublattice. Apart from the
conventionalGoldstone mode emanating from the ð0 0 qhÞ
ordering vector, low-energy magnetic excitations in
thesingle-domain proper-screw spiral phase show soft
helimagnon modes with a small energy gap of∼0.17 meV,
emerging from two orthogonal wave vectors ðqh 00Þ and ð0
qh 0Þ where no magnetic Braggpeaks are present. We term
them pseudo-Goldstone magnons, as they appear gapless within
linear spinwavetheory and only acquire a finite gap due to
higher-order quantum-fluctuation corrections. Our resultsare
likely universal for a broad class of symmetric helimagnets,
opening up a new way of studying weakmagnon-magnon
interactions with accessible spectroscopic methods.},
cin = {JCNS (München) ; Jülich Centre for Neutron Science JCNS
(München) ; JCNS-FRM-II / JCNS-2},
ddc = {530},
cid = {I:(DE-Juel1)JCNS-FRM-II-20110218 /
I:(DE-Juel1)JCNS-2-20110106},
pnm = {6G15 - FRM II / MLZ (POF3-6G15) / 6G4 - Jülich Centre for
Neutron Research (JCNS) (POF3-623)},
pid = {G:(DE-HGF)POF3-6G15 / G:(DE-HGF)POF3-6G4},
experiment = {EXP:(DE-MLZ)PANDA-20140101},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000416432000002},
doi = {10.1103/PhysRevX.7.041049},
url = {https://juser.fz-juelich.de/record/840399},
}