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@PHDTHESIS{Biniskos:851282,
author = {Biniskos, Nikolaos},
title = {{I}nelastic neutron scattering on magnetocaloric compounds},
volume = {186},
school = {RWTH Aachen},
type = {Dr.},
address = {Jülich},
publisher = {Forschungszentrum Jülich GmbH Zentralbibliothek, Verlag},
reportid = {FZJ-2018-04977},
isbn = {978-3-95806-362-4},
series = {Schriften des Forschungszentrums Jülich. Reihe
Schlüsseltechnologien / Key Technologies},
pages = {III, 92 S.},
year = {2018},
note = {RWTH Aachen, Diss., 2018},
abstract = {The search for more efficient use of energy has been
leading to a growing interest in the research field of
magnetocaloric materials. The magnetocaloric effect (MCE)
refers to a change of temperature or entropy of a magnetic
material exposed to a change of magnetic field. The MCE
requires the exchange of magnetic, lattice and/or electronic
entropy during an adiabatic (de-)magnetization process. A
large MCE at room temperature and low magnetic field for a
material with abundant and environmentally friendly elements
opens the way for magnetic cooling devices. From the
Mn$_{5-x}$Fe$_{x}$Si$_{3}$ system, that exhibits a moderate
MCE at low magnetic fields, two materials in single crystal
form are under investigation: the ferromagnetic (FM)
compound MnFe$_{4}$Si$_{3}$ and the parent compound
Mn$_{5}$Si$_{3}$. The aim of this thesis is to investigate
the spin and lattice dynamics and their couplings in these
compounds that are up to nowadays unexplored with inelastic
neutron scattering (INS)and inelastic X-ray scattering (IXS)
measurements. Such studies might help to point out
ingredients that may favour large MCE, such as phonon-magnon
interaction, effect of spin fluctuations etc. The FM
compound MnFe$_{4}$Si$_{3}$ is a promising candidate for
applications since it exhibits a moderate MCE near room
temperature. Its magnetic excitation spectrum has been
investigated by means of polarized and unpolarized INS.
Spin-wave measurements at 1.5 K reveal a strong anisotropy
of the magnetic exchange interactions along the (h00) and
(00l) reciprocal directions of the hexagonal system, which
also manifests itself in the $\textit{q}$-dependent
linewidths in the paramagnetic (PM) state. The correlation
lengths indicate a short-range order, while the average
linewidth is of the order of k$_{B}$T$_{C}$ pointing to a
behavior typical of many ferromagnets. In addition, the in-
and out-of-plane spin-fluctuations are found to be isotropic
around T$_{C}$ and can be suppressed by a magnetic field of
2 T. In order to study the spin and lattice dynamics and
their interactions in MnFe$_{4}$Si$_{3}$, a combination of
IXS and INS (polarized and unpolarized) measurements was
performed. A remarkable feature evidenced by this
combination of measurements is that along the (h00)
direction the magnon branch close to the zone boundary falls
exactly on the two transverse acoustic (TA) phonons.
Furthermore, a large difference of intensities in the two
non-spin-flip (NSF) channels was observed for one TA phonon
mode. This difference of intensity between the two NSF
channels can be attributed to the nuclear-magnetic
interference term. The parent compound Mn$_{5}$Si$_{3}$ has
been extensively characterized as a model system by many
groups in the past decades by magnetometry, X-ray and
neutron diffraction on powder and single crystal samples.
Previous studies indicate the existence of two stable
antiferromagnetic (AF) phases at about 100K (AF2)and 66K
(AF1), respectively. AF2 and AF1 transitions are of
first-order and the inverse MCE (the sample heats up when an
external magnetic field is applied adiabatically) is
associated with the AF1-AF2 phase transition. INS
experiments revealed that AF1 is characterized by sharp
spin-waves, but AF2 is characterized by a mixed signal that
resembles the one of the AF1 and PM state, indicating strong
spin-fluctuations coexisting with spin-waves. Moreover, the
application of a magnetic field in the AF1 phase induces
spin-fluctuations, which points to their importance for the
inverse MCE in Mn$_{5}$Si$_{3}$.},
cin = {JCNS-2 / PGI-4 / JARA-FIT / JCNS-ILL},
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)PUMA-20140101 /
EXP:(DE-Juel1)ILL-IN12-20150421},
typ = {PUB:(DE-HGF)3 / PUB:(DE-HGF)11},
url = {https://juser.fz-juelich.de/record/851282},
}