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Strain glass versus antisite disorder induced ferromagnetic state in Fe doped Ni–Mn–In Heusler martensites
Fe doping in Ni 2 Mn 1.5 In 0.5 results in suppression of the martensitic phase via two contrasting routes. In Ni 2 Mn 1.5 − x Fe x In 0.5 , the martensitic phase is converted to a strain glassy phase, while in Ni 2 − y Fe y Mn 1.5 In 0.5 , a cubic ferromagnetic phase results at the expense of the...
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Published in: | Journal of physics. D, Applied physics Applied physics, 2021-05, Vol.54 (18), p.185002 |
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Main Authors: | , , |
Format: | Article |
Language: | English |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | Fe doping in Ni
2
Mn
1.5
In
0.5
results in suppression of the martensitic phase via two contrasting routes. In Ni
2
Mn
1.5 −
x
Fe
x
In
0.5
, the martensitic phase is converted to a strain glassy phase, while in Ni
2 −
y
Fe
y
Mn
1.5
In
0.5
, a cubic ferromagnetic phase results at the expense of the martensite. Careful studies of magnetic and structural properties reveal the presence of the impurity
γ
-(Fe,Ni) phase as the reason for the emergence of non-ergodic strain glassy phase when Fe is sought to be doped at Y/Z (Mn) sites of X
2
YZ Heusler alloy. Whereas attempts to dope Fe in the X (Ni) sublattice result in an A2 type antisite disorder that promotes a ferromagnetic ground state. |
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ISSN: | 0022-3727 1361-6463 |
DOI: | 10.1088/1361-6463/abe3b0 |