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@INPROCEEDINGS{Jin:824611,
author = {Jin, Wentao and Xiao, Yinguo and Su, Yixi and Nandi,
Shibabrata and Li, W. and Jiao, W. H. and Meven, Martin and
Sazonov, Andrew and Nisbet, G. and Demirdis, Sultan and
Feng, Erxi and Chen, Y. and Ting, C. S. and Cao, G. H. and
Brückel, Thomas},
title = {{M}agnetism in {E}u({F}e1-x{I}rx)2{A}s2 iron pnictides
studied by complementary scattering methods},
reportid = {FZJ-2016-07174},
year = {2016},
abstract = {Abstract: Doped EuFe2As2 is a unique representative of the
122 type family of iron based superconductors due to the two
magnetic sublattices and the strong coupling between spin-,
lattice- and charge degrees of freedom. In present work, the
magnetic ground states of the localized Eu2+ spins in
underdoped, nonsuperconducting Eu(Fe0.94Ir0.06)2As2 and
optimally doped, superconducting Eu(Fe0.88Ir0.12)2As2 (TSC =
22 K) were investigated by polarized and unpolarized
single-crystal neutron diffraction measurements,
respectively. The Eu2+ spins in the underdoped (x = 0.06)
crystal were found to order within the ab plane in the
A-type antiferromagnetic (AFM) structure. However, the Eu2+
spins in the optimally doped (x = 0.12) crystal were found
to be ferromagnetically aligned along the c direction with
an ordered moment of 7.0(1) μB at 2.5 K, coexisting with
the bulk superconductivity. In addition, compared with the
parent compound EuFe2As2, which shows the AFM order of the
Fe2+ moments below TN,Fe = 190 K, TN,Fe was significantly
suppressed to 85(2) K and completely suppressed, by $6\%$
and $12\%$ Ir doping, respectively. Most strikingly, the
x-ray resonant magnetic scattering measurements on the
underdoped (x = 0.06) crystal revealed the magnetic
polarization of the 5d Ir dopant atoms and suggested a
possible interplay between the localized Eu2+ moments and
the conduction d electrons on the FeAs layers.},
month = {Oct},
date = {2016-10-03},
organization = {Joint JCNS-Workshop and Flipper 2016
“Modern Trends in Neutron Scattering
from Magnetic Systems and
Single-crystal Diffraction with
Polarized Neutrons”, Tutzing
(Germany), 3 Oct 2016 - 7 Oct 2016},
subtyp = {Invited},
cin = {JCNS (München) ; Jülich Centre for Neutron Science JCNS
(München) ; JCNS-FRM-II / JCNS-2 / PGI-4 / JARA-FIT /
Neutronenstreuung ; JCNS-1},
cid = {I:(DE-Juel1)JCNS-FRM-II-20110218 /
I:(DE-Juel1)JCNS-2-20110106 / I:(DE-Juel1)PGI-4-20110106 /
$I:(DE-82)080009_20140620$ / I:(DE-Juel1)JCNS-1-20110106},
pnm = {524 - Controlling Collective States (POF3-524) / 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)POF3-524 / G:(DE-HGF)POF3-6212 /
G:(DE-HGF)POF3-6G15 / G:(DE-HGF)POF3-6G4},
experiment = {EXP:(DE-MLZ)HEIDI-20140101 / EXP:(DE-MLZ)DNS-20140101},
typ = {PUB:(DE-HGF)6},
url = {https://juser.fz-juelich.de/record/824611},
}