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@ARTICLE{Loewenhaupt:280626,
author = {Loewenhaupt, M. and Geselbracht, P. and Faulhaber, E. and
Rotter, M. and Doerr, M. and Schmalzl, K. and Schneidewind,
A.},
title = {{F}ield {D}ependence of the {M}agnetic {P}ropagation
{V}ector of the {H}eavy {F}ermion {C}ompound {C}e{C}u2{G}e2
{S}tudied by {N}eutron {D}iffraction},
journal = {Physics procedia},
volume = {75},
issn = {1875-3892},
address = {Amsterdam [u.a.]},
publisher = {Elsevier},
reportid = {FZJ-2016-00393},
pages = {230 - 237},
year = {2015},
abstract = {CeCu2Ge2, the counterpart of the heavy-fermion
superconductor CeCu2Si2, exhibits an in-commensurate
antiferromagnetically long-range ordered ground state with
τ = (0.28 0.28 0.54) below TN = 4.15K. The magnetism is
strongly affected by a Kondo screening of the Ce 4f-moments
by conduction electrons. The similar energy scale of both,
Kondo and exchange interactions, results in a complex
magnetic phase diagram and gives rise to potential quantum
critical phenomena at very low temperatures. We present
elastic neutron diffraction data obtained on a CeCu2Ge2
single crystal employing the cold triple axis spectrometer
PANDA at MLZ and the diffractometer D23 at ILL.The field
dependence of the magnetic propagation vector was measured
at T ≤ 400 mK in the [110]/[001] plane with vertical
magnetic fields applied along [1̄10]. We observe a
low-field incommensurate magnetic phase AF1, a first order
phase transition around 7.8 T with the coexistence of two
phases AF1 and AF2 with slightly different propagation
vectors, the disappearance of AF1 at 8 T and the existence
of AF2 up to 12 T with a possible modification at 10 T. At
12.6 T, yet still well below the value of 26 T of the
saturation for magnetic fields in [110] direction, the
AF2-type magnetic order is lost and magnetic intensities are
not to be found at incommensurate positions in the
[110]/[001] plane any more. These new results contradict a
previously suggested scenario with a QCP located at 8 T and
contribute new information to the B − T phase diagram of
CeCu2Ge2 in [110] direction.},
cin = {JCNS-2 / PGI-4 / JARA-FIT / JCNS-ILL / JCNS (München) ;
Jülich Centre for Neutron Science JCNS (München) ;
JCNS-FRM-II},
ddc = {530},
cid = {I:(DE-Juel1)JCNS-2-20110106 / I:(DE-Juel1)PGI-4-20110106 /
$I:(DE-82)080009_20140620$ / I:(DE-Juel1)JCNS-ILL-20110128 /
I:(DE-Juel1)JCNS-FRM-II-20110218},
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)PANDA-20140101},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000381129300032},
doi = {10.1016/j.phpro.2015.12.028},
url = {https://juser.fz-juelich.de/record/280626},
}