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Broad first-order magnetic entropy change curve in directionally solidified polycrystalline Ni-Co-Mn-In

We present the thermal dependence of the magnetic entropy change ΔSM(T) across the martensitic transformation for a polycrystalline sample, which was cut from a directionally solidified rod, with a nominal composition Ni42Co8Mn38In12 grown by the Bridgman-Stockbarger technique. This material combine...

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Bibliographic Details
Published in:Journal of alloys and compounds 2017-12, Vol.727, p.603-609
Main Authors: Chen, F., Tong, Y.X., Li, L., Sánchez Llamazares, J.L., Sánchez-Valdés, C.F., Müllner, P.
Format: Article
Language:English
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Summary:We present the thermal dependence of the magnetic entropy change ΔSM(T) across the martensitic transformation for a polycrystalline sample, which was cut from a directionally solidified rod, with a nominal composition Ni42Co8Mn38In12 grown by the Bridgman-Stockbarger technique. This material combines a first-order martensitic transformation expanded over a very large working temperature range with a large magnetization change of ∼86 A m2 kg−1. Accordingly, for a magnetic field change of 5 T (2 T), the coupled magneto-structural transition gives rise to a broad magnetic entropy change curve across the reverse martensitic transformation with a moderate maximum value of 6.8 (3.0) J kg−1 K−1 and a full-width at half-maximum δTFWHM for the ΔSM(T) curve of 49 (43) K. Such a broad structural transition may be due to the effect of chemical segregation introduced by the directional solidification which can be enhanced by the non-uniform distribution of second phase particles. Accompanying with such a wide working temperature range, a large refrigerant capacity of 334 J kg−1 was obtained for a field change of 5 T. •Chemical heterogeneity is enhanced by decomposition via precipitation.•The working temperature range is extended to 49 K.•A large value of refrigerant capacity (334 J kg−1) is achieved.
ISSN:0925-8388
1873-4669
DOI:10.1016/j.jallcom.2017.08.118