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@INPROCEEDINGS{Maraytta:890691,
author = {Maraytta, Nour},
title = {{S}tructure and {D}ynamics of {M}agnetocaloric {M}aterials},
reportid = {FZJ-2021-01133},
year = {2021},
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)
describes the change of temperature or entropy of a material
when exposed to a change of the magnetic field and forms the
basis of magnetocaloric refrigeration technologies [1].In
the last years there has been an upsurge in the knowledge of
the MCE and many materials have been investigated for their
MCE characteristics [2]. In the context of this talk, I will
present the field direction dependence of the
thermo-magnetic behavior in single crystalline compounds
MnFe4Si3 and Mn5Ge3. The emphasis will be on the direct
measurement of the adiabatic temperature change ΔTad in
pulsed magnetic fields as it provides the opportunity to
examine the sample temperature response to the magnetic
field on a time scale close to the real process used in
applications [3]. A discussion of how the anisotropy affects
the magnetocaloric effect and a comparison between MnFe4Si3
compound, which exhibits easy plane anisotropy, and Mn5Ge3
which features uniaxial anisotropy, will be also presented
[4].The Mn5Si3 compound exhibits inverse MCE related to the
antiferromagnetic order phase transition AF1 to AF2, and
direct MCE related to the AF2 to the paramagnetic phase
transitions. Previous studies indicate a transition from the
AF1 to AF1' before reaching the AF2 phase [5]. The magnetic
structures of the AF1 and AF2 phases have been established
[6, 7], while the magnetic structure of the AF1' phase has
not been studied before. Therefore, the second part of the
talk will be devoted to discuss the results of the
investigation of the nuclear and magnetic structure of the
intermediate phase AF1' of the single crystalline compound
Mn5Si3.[1] K. A. Gschneidner Jr. and V.K. Pecharsky,
“Thirty years of near room temperature magnetic cooling:
Where we are today and future prospects”, International
Journal of Refrigeration, 31, 945(2008).[2] V. Franco, J. S.
Blazquez, B. Ingale, and A. Conde, “The magnetocaloric
effect and magnetic refrigeration near room temperature:
Materials and models”, Annual Review of Materials
Research, 42, 305(2012).[3] N. Maraytta, Y. Skourski, J.
Voigt, K. Friese, M. G. Herrmann, J. Perßon, J. Wosnitza,
S. M. Salman, and T. Brückel, “Direct measurements of the
magneto-caloric effect of MnFe4Si3 in pulsed magnetic
fields”, Journal of Alloys and Compounds, 805,
1161(2019).[4] N. Maraytta, J. Voigt, C. S. Mejia, K.
Friese, Y. Skourski, J. Perßon, S. M. Salman, and T.
Brückel, “Anisotropy of the magnetocaloric effect:
Example of Mn5Ge3”, Journal of Applied Physics, 128,
103903(2020).[5] M. R. Silva, P. J. Brown, and J. B.
Forsyth, “Magnetic moments and magnetic site
susceptibilities in Mn5Si3”, Journal of Physics: Condensed
Matter, 14, 8707(2002).[6] P. J. Brown, J. B. Forsyth, V.
Nunez, and F. Tasset, “The low-temperature
antiferromagnetic structure of Mn5Si3 revised in the light
of neutron polarimetry”, Journal of Physics: Condensed
Matter, 4, 10025 (1992).[7] P. J. Brown and J. B. Forsyth,
“Antiferromagnetism in Mn5Si3: The magnetic structure of
the AF2 phase at 70 K”, Journal of Physics: Condensed
Matter, 7, 7619(1995).},
month = {Feb},
date = {2021-02-25},
organization = {Digital Institute Seminar JCNS-2,
Forschungszentrum Jülich GmbH
(Germany), 25 Feb 2021 - 25 Feb 2021},
subtyp = {Invited},
cin = {JCNS-2 / PGI-4 / JARA-FIT},
cid = {I:(DE-Juel1)JCNS-2-20110106 / I:(DE-Juel1)PGI-4-20110106 /
$I:(DE-82)080009_20140620$},
pnm = {632 - Materials – Quantum, Complex and Functional
Materials (POF4-632) / 6G4 - Jülich Centre for Neutron
Research (JCNS) (FZJ) (POF4-6G4)},
pid = {G:(DE-HGF)POF4-632 / G:(DE-HGF)POF4-6G4},
experiment = {EXP:(DE-MLZ)NOSPEC-20140101},
typ = {PUB:(DE-HGF)31},
url = {https://juser.fz-juelich.de/record/890691},
}