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@ARTICLE{Portnichenko:874993,
author = {Portnichenko, P. Y. and Akbari, A. and Nikitin, S. E. and
Cameron, A. S. and Dukhnenko, A. V. and Filipov, V. B. and
Shitsevalova, N. Yu. and Čermák, P. and Radelytskyi, I.
and Schneidewind, A. and Ollivier, J. and Podlesnyak, A. and
Huesges, Z. and Xu, J. and Ivanov, A. and Sidis, Y. and
Petit, S. and Mignot, J.-M. and Thalmeier, P. and Inosov, D.
S.},
title = {{F}ield-{A}ngle-{R}esolved {M}agnetic {E}xcitations as a
{P}robe of {H}idden-{O}rder {S}ymmetry in {C}e{B} 6},
journal = {Physical review / X Expanding access X},
volume = {10},
number = {2},
issn = {2160-3308},
address = {College Park, Md.},
publisher = {APS},
reportid = {FZJ-2020-01755},
pages = {021010},
year = {2020},
abstract = {In contrast to magnetic order formed by electrons’
dipolar moments, ordering phenomena associated with
higher-order multipoles (quadrupoles, octupoles, etc.) are
more difficult to characterize because of the limited choice
of experimental probes that can distinguish different
multipolar moments. The heavy-fermion compound CeB6 and its
La-diluted alloys are among the best-studied realizations of
the long-range-ordered multipolar phases, often referred to
as “hidden order.” Previously, the hidden order in phase
II was identified as primary antiferroquadrupolar and
field-induced octupolar order. Here, we present a combined
experimental and theoretical investigation of collective
excitations in phase II of CeB6. Inelastic neutron
scattering (INS) in fields up to 16.5 T reveals a new
high-energy mode above 14 T in addition to the low-energy
magnetic excitations. The experimental dependence of their
energy on the magnitude and angle of the applied magnetic
field is compared to the results of a multipolar interaction
model. The magnetic excitation spectrum in a rotating field
is calculated within a localized approach using the
pseudospin representation for the Γ8 states. We show that
the rotating-field technique at fixed momentum can
complement conventional INS measurements of the dispersion
at a constant field and holds great promise for identifying
the symmetry of multipolar order parameters and the details
of intermultipolar interactions that stabilize hidden-order
phases.},
cin = {JCNS-FRM-II / JCNS-2 / MLZ},
ddc = {530},
cid = {I:(DE-Juel1)JCNS-FRM-II-20110218 /
I:(DE-Juel1)JCNS-2-20110106 / I:(DE-588b)4597118-3},
pnm = {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)POF3-6212 / G:(DE-HGF)POF3-6G15 /
G:(DE-HGF)POF3-6G4},
experiment = {EXP:(DE-MLZ)PANDA-20140101},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000525447300001},
doi = {10.1103/PhysRevX.10.021010},
url = {https://juser.fz-juelich.de/record/874993},
}