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@PHDTHESIS{Gottschlich:22832,
author = {Gottschlich, Michael},
title = {{S}tructure, magnetism and excitations in some {M}n-based
magnetocaloric effect compounds},
volume = {62},
school = {RWTH Aachen},
type = {Dr. (FH)},
address = {Jülich},
publisher = {Forschungszentrum Jülich GmbH Zentralbibliothek, Verlag},
reportid = {PreJuSER-22832},
isbn = {978-3-89336-874-7},
series = {Schriften des Forschungszentrums Jülich.
Schlüsseltechnologien / Key Technologies},
pages = {175 S.},
year = {2012},
note = {Record converted from VDB: 12.11.2012; RWTH Aachen, Diss.,
2012},
abstract = {The magnetocaloric effect causes the cooling or heating of
a material due to the influence of an applied magnetic
field. This mechanism provides an alternative technique for
cooling, when using cheap and environment friendly
materials. Heating and cooling takes place without moving
any mechanical parts. Therefore, this effect attracts the
attention of many scientific studies. The magneto caloric
effect is characterized by the entropy change.
Polycrystalline samples of the compositions
Mn$_{5−x}$Fe$_{x}$Si$_{3}$ x=0,1,2,3,4 and a single
crystal of the composition Mn$_{5−x}$Fe$_{x}$Si$_{3}$ x=4
were prepared in order to analyze the magnetocaloric effect
in those materials. All samples were characterized with
magnetization measurements. Ferroand antiferromagnetic
behaviour could be detected. Diffraction patterns were taken
on the timeof- flight powder diffractometer POWGEN at the
Spallation Neutron Source (SNS), Oak Ridge National
Laboratory to analyze the magnetic structures of the
compounds. Inelastic neutron data were collected on the
single crystal Mn$_{5−x}$Fe$_{x}$Si$_{3}$ x=4 on the
thermal neutron triple axis spectrometer 2T1 at Laboratoire
Léon Brillouin to investigate the dynamic properties. The
refined data taken on samples Mn$_{5−x}$Fe$_{x}$Si$_{3}$
x=0,1,2,3,4 on POWGEN at room temperature confirm the
hexagonal structure. This has already been reported in
literature. Anomalies could be identified in several
crystallographic parameters as funtion of the Fe-content of
the samples Diffraction patterns taken on sample
Mn$_{5−x}$Fe$_{x}$Si$_{3}$ x=0 between the phase
transitions at 70K and 90K could be refined with an
orthorhombic unit cell including antiferromagnetism. Below
the phase transition at 62K the best refinements could be
performed using a monoclinic unit cell. Also, the structure
seems to exhibit weak ferromagnetism, which can be
annihilated with an applied magnetic field. This mechanism
is proposed to cause the negative magnetocaloric effect in
this compound. The analysis of diffraction patterns taken in
the ferromagnetic phase of Mn$_{5−x}$Fe$_{x}$Si$_{3}$ x=4
indicate different behaviours of the magnetic atoms
occupying the two crystallographic positions (the third is
occupied by Si). This property is proposed to influence
significantly the entropy in this material. Phonon branches
in the dispersion relation of Mn$_{5−x}$Fe$_{x}$Si$_{3}$
x=4 are anisotropic, which is due to the hexagonal
structure. In order to investigate the effect of Fe and Mn
on the change of the entropy the composition
Mn$_{5−x}$Fe$_{x}$Si$_{3}$ x=4 was doped with Co (for Mn
and Fe). The analysis of the diffraction patterns which were
taken on POWGEN identified at least one impurity phase in
every sample. Different behaviours of the magnetic moments
of the atoms in these compounds could also be verified,
which is similar to the composition
Mn$_{5−x}$Fe$_{x}$Si$_{3}$ x=4.},
cin = {PGI-4 / JCNS-2 / JARA-FIT},
cid = {I:(DE-Juel1)PGI-4-20110106 / I:(DE-Juel1)JCNS-2-20110106 /
$I:(DE-82)080009_20140620$},
pnm = {Grundlagen für zukünftige Informationstechnologien},
pid = {G:(DE-Juel1)FUEK412},
typ = {PUB:(DE-HGF)11 / PUB:(DE-HGF)3},
url = {https://juser.fz-juelich.de/record/22832},
}