TY - JOUR
T1 - Crystal structures and magnetization distributions in the field dependent ferromagnetic shape memory alloy Ni54Fe19Ga27
AU - Brown, P. J.
AU - Gandy, A. P.
AU - Ishida, K.
AU - Kainuma, R.
AU - Kanomata, T.
AU - Morito, H.
AU - Neumann, K. U.
AU - Oikawa, K.
AU - Ziebeck, K. R.A.
PY - 2007/1/10
Y1 - 2007/1/10
N2 - The mesoscopic and microscopic mechanisms giving rise to shape memory behaviour in single crystals of the ferromagnetic alloy Ni54Fe 19Ga27 have been investigated using polarized and unpolarized neutron diffraction. The measurements confirm that the Curie temperature TC coincides with the martensitic phase transition at TM ≤ 296K. At room temperature the crystal, as grown, had the tetragonal L10 structure with c/a≈1.20. It transformed to the cubic Heusler L21 structure at ≈330K. In subsequent heating and cooling cycles the transition took place at TM≈295K and it was found that applying a magnetic field raised TM by ≈0.3KT -1, making the material attractive for applications. The tetragonal structure has space group I4/mmm and is related to the cubic parent phase by a Bain transformation. The change in cell volume at the transition is only ≈1%, suggesting that the atomic moments are unchanged, although the magnetization drops significantly. The polarized neutron results show that in the cubic phase the magnetic electrons at the iron-rich sites have predominantly eg symmetry (60(3)%), a distribution similar to that observed in Fe3Al and Fe3Si. A small transfer of magnetization from Fe to Ni is associated with the martensitic transition, but no significant redistribution of magnetic electrons between orbitals whose degeneracy is lifted, such as that predicated by the band Jahn-Teller mechanism, was observed.
AB - The mesoscopic and microscopic mechanisms giving rise to shape memory behaviour in single crystals of the ferromagnetic alloy Ni54Fe 19Ga27 have been investigated using polarized and unpolarized neutron diffraction. The measurements confirm that the Curie temperature TC coincides with the martensitic phase transition at TM ≤ 296K. At room temperature the crystal, as grown, had the tetragonal L10 structure with c/a≈1.20. It transformed to the cubic Heusler L21 structure at ≈330K. In subsequent heating and cooling cycles the transition took place at TM≈295K and it was found that applying a magnetic field raised TM by ≈0.3KT -1, making the material attractive for applications. The tetragonal structure has space group I4/mmm and is related to the cubic parent phase by a Bain transformation. The change in cell volume at the transition is only ≈1%, suggesting that the atomic moments are unchanged, although the magnetization drops significantly. The polarized neutron results show that in the cubic phase the magnetic electrons at the iron-rich sites have predominantly eg symmetry (60(3)%), a distribution similar to that observed in Fe3Al and Fe3Si. A small transfer of magnetization from Fe to Ni is associated with the martensitic transition, but no significant redistribution of magnetic electrons between orbitals whose degeneracy is lifted, such as that predicated by the band Jahn-Teller mechanism, was observed.
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U2 - 10.1088/0953-8984/19/1/016201
DO - 10.1088/0953-8984/19/1/016201
M3 - Article
AN - SCOPUS:33847195054
SN - 0953-8984
VL - 19
JO - Journal of Physics Condensed Matter
JF - Journal of Physics Condensed Matter
IS - 1
M1 - 016201
ER -