Entropy change reversibility in MnNi1−x Co x Ge0.97Al0.03 near the triple point

The nature of the phase transition has been studied in MnNi _1− _x Co _x Ge _0.97 Al _0.03 ( x = 0.20–0.50) through magnetization, differential scanning calorimetry and x-ray diffraction measurements; and the associated reversibility in the magnetocaloric effect has been examined. A small amount of...

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Main Authors: Tapas Samanta, Chris Taake, Laila Bondzio, Luana Caron
Format: Article
Language:English
Published: IOP Publishing 2023-01-01
Series:JPhys Energy
Subjects:
Online Access:https://doi.org/10.1088/2515-7655/acf957
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author Tapas Samanta
Chris Taake
Laila Bondzio
Luana Caron
author_facet Tapas Samanta
Chris Taake
Laila Bondzio
Luana Caron
author_sort Tapas Samanta
collection DOAJ
description The nature of the phase transition has been studied in MnNi _1− _x Co _x Ge _0.97 Al _0.03 ( x = 0.20–0.50) through magnetization, differential scanning calorimetry and x-ray diffraction measurements; and the associated reversibility in the magnetocaloric effect has been examined. A small amount of Al substitution for Ge can lower the structural phase transition temperature, resulting in a coupled first-order magnetostructural transition (MST) from a ferromagnetic orthorhombic to a paramagnetic hexagonal phase in MnNi _1− _x Co _x Ge _0.97 Al _0.03 . Interestingly, a composition-dependent triple point (TP) has been detected in the studied system, where the first-order MST is split into an additional phase boundary at higher temperature with a second-order transition character. The critical-field-value of the field-induced MST decreases with increasing Co concentration and disappears at the TP ( x = 0.37) resembling most field-sensitive MST among the studied compositions. An increase of the hexagonal lattice parameter a _hex near the TP indicates a lattice softening associated with an enhancement of the vibrational amplitude in the Ni/Co site. The lattice softening leads to a larger field-induced structural entropy change (structural entropy change≫ magnetic entropy change, for this class of materials) with the application of a lower field, which results in a larger reversibility of the low-field entropy change (|Δ S _rev | = 6.9 J kg ^−1 K for Δ μ _0 H = 2 T) at the TP.
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spelling doaj.art-9299699c0bb44f419b5025d15182fd9a2023-09-25T09:40:01ZengIOP PublishingJPhys Energy2515-76552023-01-015404400210.1088/2515-7655/acf957Entropy change reversibility in MnNi1−x Co x Ge0.97Al0.03 near the triple pointTapas Samanta0https://orcid.org/0000-0002-0964-502XChris Taake1Laila Bondzio2Luana Caron3Faculty of Physics, Bielefeld University , PO Box 100131, Bielefeld D-33501, GermanyFaculty of Physics, Bielefeld University , PO Box 100131, Bielefeld D-33501, GermanyFaculty of Physics, Bielefeld University , PO Box 100131, Bielefeld D-33501, GermanyFaculty of Physics, Bielefeld University , PO Box 100131, Bielefeld D-33501, Germany; Helmholtz-Zentrum Berlin für Materialien und Energie , Berlin 12489, GermanyThe nature of the phase transition has been studied in MnNi _1− _x Co _x Ge _0.97 Al _0.03 ( x = 0.20–0.50) through magnetization, differential scanning calorimetry and x-ray diffraction measurements; and the associated reversibility in the magnetocaloric effect has been examined. A small amount of Al substitution for Ge can lower the structural phase transition temperature, resulting in a coupled first-order magnetostructural transition (MST) from a ferromagnetic orthorhombic to a paramagnetic hexagonal phase in MnNi _1− _x Co _x Ge _0.97 Al _0.03 . Interestingly, a composition-dependent triple point (TP) has been detected in the studied system, where the first-order MST is split into an additional phase boundary at higher temperature with a second-order transition character. The critical-field-value of the field-induced MST decreases with increasing Co concentration and disappears at the TP ( x = 0.37) resembling most field-sensitive MST among the studied compositions. An increase of the hexagonal lattice parameter a _hex near the TP indicates a lattice softening associated with an enhancement of the vibrational amplitude in the Ni/Co site. The lattice softening leads to a larger field-induced structural entropy change (structural entropy change≫ magnetic entropy change, for this class of materials) with the application of a lower field, which results in a larger reversibility of the low-field entropy change (|Δ S _rev | = 6.9 J kg ^−1 K for Δ μ _0 H = 2 T) at the TP.https://doi.org/10.1088/2515-7655/acf957magnetocaloric effecttriple pointreversible entropy changelattice softening
spellingShingle Tapas Samanta
Chris Taake
Laila Bondzio
Luana Caron
Entropy change reversibility in MnNi1−x Co x Ge0.97Al0.03 near the triple point
JPhys Energy
magnetocaloric effect
triple point
reversible entropy change
lattice softening
title Entropy change reversibility in MnNi1−x Co x Ge0.97Al0.03 near the triple point
title_full Entropy change reversibility in MnNi1−x Co x Ge0.97Al0.03 near the triple point
title_fullStr Entropy change reversibility in MnNi1−x Co x Ge0.97Al0.03 near the triple point
title_full_unstemmed Entropy change reversibility in MnNi1−x Co x Ge0.97Al0.03 near the triple point
title_short Entropy change reversibility in MnNi1−x Co x Ge0.97Al0.03 near the triple point
title_sort entropy change reversibility in mnni1 x co x ge0 97al0 03 near the triple point
topic magnetocaloric effect
triple point
reversible entropy change
lattice softening
url https://doi.org/10.1088/2515-7655/acf957
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