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Magnetization study of the kinetic arrest of martensitic transformation in as-quenched Ni52.2Mn34.3In13.5 melt spun ribbons

Published online by Cambridge University Press:  05 March 2013

F.M. Lino-Zapata
Affiliation:
Instituto Potosino de Investigación Científica y Tecnológica, Camino a la Presa San José 2055 Col. Lomas 4ª, San Luis Potosí, S.L.P. 78216, México.
J.L. Sánchez Llamazares
Affiliation:
Instituto Potosino de Investigación Científica y Tecnológica, Camino a la Presa San José 2055 Col. Lomas 4ª, San Luis Potosí, S.L.P. 78216, México.
D. Ríos-Jara
Affiliation:
Instituto Potosino de Investigación Científica y Tecnológica, Camino a la Presa San José 2055 Col. Lomas 4ª, San Luis Potosí, S.L.P. 78216, México.
A.G. Lara-Rodríguez
Affiliation:
Instituto de Investigaciones en Materiales, UNAM, Circuito Exterior s/n, Ciudad Universitaria, México D.F. 04510, México.
T. García-Fernández
Affiliation:
Universidad Autónoma de la Ciudad de México, Prolongación San Isidro 151,Col. San Lorenzo Tezonco, México DF, C.P. 09790, México
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Abstract

The kinetic arrest of martensitic transformation (MT) has been observed in as-solidified Ni52.2Mn34.3In13.5 melt spun ribbons. The main characteristics of this unusual field-induced magneto-structural phenomenon have been determined through a dc magnetization study. The sample studied was fabricated by rapid solidification using the melt spinning technique at a high quenching rate of 48 ms-1. At room temperature, it is a single phase austenite (AST) with the bcc B2-type crystal structure and Curie temperature of TCA=285 K. With decreasing temperature, the austenite phase transforms into the martensite phase (MST) with TCM≈185 K at a starting martensitic transition temperature of MS=275 K. A moderate but progressive kinetic arrest of the AST to MST transformation has been observed for magnetic field values above H=10 kOe and was studied up to Hmax= 90 kOe. The metastable character of the non-equilibrium field-cooled state is revealed by the decreasing behavior of the saturation magnetization under a large magnetic field of 50 kOe after temperature cycling from 10 K to 150 K. The total magnetization difference Δσ between the zero field-cooling and field-cooling pathways of the temperature dependence of magnetization shows irreversible and reversible components and the former decreases with decreasing temperature.

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Articles
Copyright
Copyright © Materials Research Society 2013 

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References

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