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@ARTICLE{Li:255497,
author = {Li, Hai-Feng and Senyshyn, Anatoliy and Fabelo, Oscar and
Persson, Jörg and Hou, Binyang and Boehm, Martin and
Schmalzl, Karin and Schmidt, Wolfgang and Vassalli,
Jean-Pierre and Thakuria, Pankaj and Sun, Xiao and
Khazaradze, Giorgi and Schmitz, Berthold and Zhang, Cong and
Roth, Georg and García Roca, Javier and Wildes, Andrew and
Wang, Liming},
title = {{A}bsence of magnetic ordering in the ground state of a
{S}r{T}m $_{2}$ {O} $_{4}$ single crystal},
journal = {Journal of materials chemistry / C},
volume = {3},
number = {29},
issn = {2050-7534},
address = {London {[u.a.]},
publisher = {RSC},
reportid = {FZJ-2015-05659},
pages = {7658 - 7668},
year = {2015},
abstract = {We report on the first single crystal study of SrTm2O4.
Magnetization measurements along the crystallographic axes
of a nearly stoichiometric Sr1.07(3)Tm2.07(6)O4.00(2) sample
show either a positive or a negative Curie–Weiss
temperature indicative of a competition between
antiferromagnetic and ferromagnetic couplings. The
field-dependent magnetization suggests an effective Zeeman
splitting of the high-level J-multiplets above ∼8.3 T and
that the paramagnetism may originate from only one of the
two inequivalent Tm3+ crystallographic sites. Our
single-crystal polarized neutron scattering and powder
unpolarized neutron diffraction data show no evidence for
either long- or short-range magnetic order even down to
∼65 mK. We reveal two TmO6 octahedral distortion modes,
i.e., one distortion is stronger than the other especially
at low temperatures, which is attributed to different
crystal fields of the two inequivalent octahedra. Therefore,
the compound SrTm2O4 is unique and different from its
brethren in the family of frustrated SrRE2O4 (RE = rare
earth) magnets. We propose that crystal field anisotropy may
dominate over weak dipolar spin interactions in SrTm2O4,
thereby leading to a virtually non-ordered magnetic state.},
cin = {JCNS-2 / PGI-4 / JARA-FIT / JCNS-ILL},
ddc = {540},
cid = {I:(DE-Juel1)JCNS-2-20110106 / I:(DE-Juel1)PGI-4-20110106 /
$I:(DE-82)080009_20140620$ / I:(DE-Juel1)JCNS-ILL-20110128},
pnm = {144 - Controlling Collective States (POF3-144) / 524 -
Controlling Collective States (POF3-524) / 6212 - Quantum
Condensed Matter: Magnetism, Superconductivity (POF3-621) /
6213 - Materials and Processes for Energy and Transport
Technologies (POF3-621) / 6G4 - Jülich Centre for Neutron
Research (JCNS) (POF3-623)},
pid = {G:(DE-HGF)POF3-144 / G:(DE-HGF)POF3-524 /
G:(DE-HGF)POF3-6212 / G:(DE-HGF)POF3-6213 /
G:(DE-HGF)POF3-6G4},
experiment = {EXP:(DE-MLZ)SPODI-20140101},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000358228400017},
doi = {10.1039/C5TC01607J},
url = {https://juser.fz-juelich.de/record/255497},
}