Suppression of martensitic transformation in Ni-Mn-In metamagnetic shape memory alloy under very strong magnetic field

Patricia Lázpita; Anabel Pérez-Checa; Jose M. Barandiarán; Andrew Ammerlaan; Uli Zeitler; Volodymyr Chernenko

doi:10.1016/j.jallcom.2021.159814

Suppression of martensitic transformation in Ni-Mn-In metamagnetic shape memory alloy under very strong magnetic field

Patricia Lázpita^*, Anabel Pérez-Checa, Jose M. Barandiarán, Andrew Ammerlaan, Uli Zeitler, Volodymyr Chernenko

^*Autor correspondiente de este trabajo

Caracterización y Validación. Materiales

Producción científica: Contribución a una revista › Artículo › revisión exhaustiva

9 Citas (Scopus)

Resumen

The magnetic field induced martensitic transformation (MT) and its arrest exhibited by the prototype Ni-Mn-In metamagnetic shape memory alloy have been studied for its two distinct magnetic states achieved by different cooling routes, namely, a zero field cooling (ZFC) and a strong magnetic field cooling (SFC). For that, magnetization as a function of magnetic field up to 33 T was measured at different constant temperatures. As a result, two different phase diagrams “MT magnetic field versus temperature” were obtained for the ZFC and SFC samples. The magnetic entropy difference between the aforementioned two states was attributed to the different microstructures of the martensitic phase formed in the alloy along each route.

Idioma original	Inglés
Número de artículo	159814
Publicación	Journal of Alloys and Compounds
Volumen	874
DOI	https://doi.org/10.1016/j.jallcom.2021.159814
Estado	Publicada - 5 sept 2021

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title = "Suppression of martensitic transformation in Ni-Mn-In metamagnetic shape memory alloy under very strong magnetic field",

abstract = "The magnetic field induced martensitic transformation (MT) and its arrest exhibited by the prototype Ni-Mn-In metamagnetic shape memory alloy have been studied for its two distinct magnetic states achieved by different cooling routes, namely, a zero field cooling (ZFC) and a strong magnetic field cooling (SFC). For that, magnetization as a function of magnetic field up to 33 T was measured at different constant temperatures. As a result, two different phase diagrams “MT magnetic field versus temperature” were obtained for the ZFC and SFC samples. The magnetic entropy difference between the aforementioned two states was attributed to the different microstructures of the martensitic phase formed in the alloy along each route.",

keywords = "Martensitic transformation, NiMnIn metamagnetic shape memory alloy, Phase diagrams, Strong field cooling, Transformation arrest, Very strong magnetic field, Zero field cooling",

author = "Patricia L{\'a}zpita and Anabel P{\'e}rez-Checa and Barandiar{\'a}n, {Jose M.} and Andrew Ammerlaan and Uli Zeitler and Volodymyr Chernenko",

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doi = "10.1016/j.jallcom.2021.159814",

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AU - Lázpita, Patricia

AU - Pérez-Checa, Anabel

AU - Barandiarán, Jose M.

AU - Ammerlaan, Andrew

AU - Zeitler, Uli

AU - Chernenko, Volodymyr

PY - 2021/9/5

Y1 - 2021/9/5

N2 - The magnetic field induced martensitic transformation (MT) and its arrest exhibited by the prototype Ni-Mn-In metamagnetic shape memory alloy have been studied for its two distinct magnetic states achieved by different cooling routes, namely, a zero field cooling (ZFC) and a strong magnetic field cooling (SFC). For that, magnetization as a function of magnetic field up to 33 T was measured at different constant temperatures. As a result, two different phase diagrams “MT magnetic field versus temperature” were obtained for the ZFC and SFC samples. The magnetic entropy difference between the aforementioned two states was attributed to the different microstructures of the martensitic phase formed in the alloy along each route.

AB - The magnetic field induced martensitic transformation (MT) and its arrest exhibited by the prototype Ni-Mn-In metamagnetic shape memory alloy have been studied for its two distinct magnetic states achieved by different cooling routes, namely, a zero field cooling (ZFC) and a strong magnetic field cooling (SFC). For that, magnetization as a function of magnetic field up to 33 T was measured at different constant temperatures. As a result, two different phase diagrams “MT magnetic field versus temperature” were obtained for the ZFC and SFC samples. The magnetic entropy difference between the aforementioned two states was attributed to the different microstructures of the martensitic phase formed in the alloy along each route.

KW - Martensitic transformation

KW - NiMnIn metamagnetic shape memory alloy

KW - Phase diagrams

KW - Strong field cooling

KW - Transformation arrest

KW - Very strong magnetic field

KW - Zero field cooling

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Suppression of martensitic transformation in Ni-Mn-In metamagnetic shape memory alloy under very strong magnetic field

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