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@ARTICLE{Kbler:57845,
author = {Köbler, U. and Hoser, A. and Hoffmann, J.-U. and Thomas,
C.},
title = {{O}ne-dimensional bulk ferromagnets: {N}d{A}l2 and hcp
cobalt},
journal = {Solid state communications},
volume = {137},
issn = {0038-1098},
address = {New York, NY [u.a.]},
publisher = {Elsevier Science},
reportid = {PreJuSER-57845},
pages = {301 - 305},
year = {2006},
note = {Record converted from VDB: 12.11.2012},
abstract = {It is shown experimentally that NdAl2 and hcp cobalt are
one-dimensional (1D) bulk ferromagnets. For hcp cobalt this
is only under the condition that the sample is magnetically
saturated, i.e. that all moments are aligned parallel to the
hexagonal c-axis. In 1D magnets the transverse interactions
need not to be zero but must be sufficiently weak such that
the transverse correlation length does not diverge at the
critical temperature. The transverse interactions are then
not relevant and the phase transition is driven by the
longitudinal interactions. On the other hand, magnetic Bragg
scattering relies on finite transverse correlations. For
NdAl2 no conventional magnetic Bragg scattering is observed
if all moments are aligned vertical to the scattering plane
by a magnetic field. For hcp cobalt the scattering intensity
is considerably reduced in this geometry instead of having
its maximum. From this observation it can be concluded that
the transverse correlation length is practically zero in
NdAl2 but has a finite value in hcp cobalt. The macroscopic
magnetization shows normal ferromagnetic saturation. (c)
2005 Elsevier Ltd. All rights reserved.},
keywords = {J (WoSType)},
cin = {IFF-INS / IFF-ISM},
ddc = {540},
cid = {I:(DE-Juel1)VDB341 / I:(DE-Juel1)VDB342},
pnm = {Kondensierte Materie / Großgeräte für die Forschung mit
Photonen, Neutronen und Ionen (PNI)},
pid = {G:(DE-Juel1)FUEK414 / G:(DE-Juel1)FUEK415},
shelfmark = {Physics, Condensed Matter},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000235426400005},
doi = {10.1016/j.ssc.2005.11.041},
url = {https://juser.fz-juelich.de/record/57845},
}