TY - JOUR
T1 - Thermal strain and magnetization of the ferromagnetic shape memory alloy Ni 52Mn 25Ga 23 in a magnetic field
AU - Sakon, T.
AU - Nagashio, H.
AU - Sasaki, K.
AU - Susuga, S.
AU - Numakura, D.
AU - Abe, M.
AU - Endo, K.
AU - Yamashita, S.
AU - Nojiri, H.
AU - Kanomata, T.
N1 - Funding Information:
This study was technically supported by the Center for Integrated Nanotechnology Support, Tohoku University , and the High Field Laboratory for Superconducting Materials, Institute for Materials Research, Tohoku University . One of the authors (H.N.) acknowledges the support by GCOE-material integration .
Funding Information:
This study was supported by a Grant-in-Aid of the three universities cooperation project in North Tohoku area in Japan, and Japan Science and Technology Project no. AS232Z02122B . This study was also partly supported by a Grant-in-Aid for Scientific Research (C) (Grant no. 21560693 ) from the Japan Society for the Promotion of Science (JSPS) of the Ministry of Education, Culture, Sports, Science and Technology, Japan .
PY - 2013/1
Y1 - 2013/1
N2 - The objective of this paper is the investigation of the correlations between crystal structure and the magnetization of Ni-Mn-Ga Heusler alloy. Thermal strain, permeability, and magnetization measurements of the ferromagnetic shape memory alloy Ni 52Mn 25Ga 23 were performed across the martensite transition temperature T M and reverse martensite transition temperature T R at atmospheric pressure. When cooling from the austenite phase, thermal strain steeply decreases because of martensite transition. Permeability suddenly increases at the Curie temperature T C=358 K, indicating ferromagnetism, and suddenly decreases to around T M=328 K. This indicates that the lattice transformation and magnetic phase transition correspond to each other. The percentage of contraction by martensite transition at T M and in a magnetic field is twice that in zero fields. Considering with other Ni-Mn-Ga alloys, it is supposed that the magnetic field influences the orientation of the easy c-axis along the magnetic field, and then the variant rearrangement occurs, and consequently, the variation in the strain between zero fields and non-zero field is observed. The measurement results indicate that the regions above and below T M or T R are the ferromagnetic-austenite (Ferro-A) and ferromagnetic-martensite (Ferro-M) phases, respectively. Magnetic phase diagrams were constructed from the results of the temperature dependence of thermal strain. T M and T R increase gradually with magnetic field. T M shift in magnetic fields (B) around zero magnetic field was estimated as dT M/dB=0.46 K/T, indicating that magnetization influences martensite transition and the dT M/dB value is the same as that of Ni 52Mn 12.5Fe 12.5Ga 23, thereby suggesting the Ferro-M to Ferro-A transition.
AB - The objective of this paper is the investigation of the correlations between crystal structure and the magnetization of Ni-Mn-Ga Heusler alloy. Thermal strain, permeability, and magnetization measurements of the ferromagnetic shape memory alloy Ni 52Mn 25Ga 23 were performed across the martensite transition temperature T M and reverse martensite transition temperature T R at atmospheric pressure. When cooling from the austenite phase, thermal strain steeply decreases because of martensite transition. Permeability suddenly increases at the Curie temperature T C=358 K, indicating ferromagnetism, and suddenly decreases to around T M=328 K. This indicates that the lattice transformation and magnetic phase transition correspond to each other. The percentage of contraction by martensite transition at T M and in a magnetic field is twice that in zero fields. Considering with other Ni-Mn-Ga alloys, it is supposed that the magnetic field influences the orientation of the easy c-axis along the magnetic field, and then the variant rearrangement occurs, and consequently, the variation in the strain between zero fields and non-zero field is observed. The measurement results indicate that the regions above and below T M or T R are the ferromagnetic-austenite (Ferro-A) and ferromagnetic-martensite (Ferro-M) phases, respectively. Magnetic phase diagrams were constructed from the results of the temperature dependence of thermal strain. T M and T R increase gradually with magnetic field. T M shift in magnetic fields (B) around zero magnetic field was estimated as dT M/dB=0.46 K/T, indicating that magnetization influences martensite transition and the dT M/dB value is the same as that of Ni 52Mn 12.5Fe 12.5Ga 23, thereby suggesting the Ferro-M to Ferro-A transition.
KW - A. Alloys
KW - B. Crystal growth
KW - C. X-ray diffraction
KW - D. Magnetic properties
KW - D. Thermal expansion
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U2 - 10.1016/j.jpcs.2012.09.004
DO - 10.1016/j.jpcs.2012.09.004
M3 - Article
AN - SCOPUS:84867685641
SN - 0022-3697
VL - 74
SP - 158
EP - 165
JO - Journal of Physics and Chemistry of Solids
JF - Journal of Physics and Chemistry of Solids
IS - 1
ER -