2007
DOI: 10.1016/j.jallcom.2006.06.003
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Phase transformation and magnetic properties in Ni–Mn–Ga Heusler alloys

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Cited by 39 publications
(18 citation statements)
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“…1a). Compared with 2 2 0 diffraction peak, which is the strongest one of the 2:17R phase, the 0 0 6 diffraction peak along the easy magnetization direction of the 2:17R is relatively low, which indicates there is no evident [21] preferred orientation growth in the as-cast master alloy during cooling. The ribbons prepared by as-cast master alloy, which are melt-spun at 20 m/s, mainly consist of TbCu 7 -type Sm(Co, M) 7 (M = Fe, Cu, Zr) phase (for short 1:7H) (see Fig.…”
Section: Phase Analysismentioning
confidence: 95%
“…1a). Compared with 2 2 0 diffraction peak, which is the strongest one of the 2:17R phase, the 0 0 6 diffraction peak along the easy magnetization direction of the 2:17R is relatively low, which indicates there is no evident [21] preferred orientation growth in the as-cast master alloy during cooling. The ribbons prepared by as-cast master alloy, which are melt-spun at 20 m/s, mainly consist of TbCu 7 -type Sm(Co, M) 7 (M = Fe, Cu, Zr) phase (for short 1:7H) (see Fig.…”
Section: Phase Analysismentioning
confidence: 95%
“…5,7,13,23,24 However it is not so often in bulk polycrystalline FSMAs where the low-field magnetization generally keeps unchanged between T A and T C . [25][26][27][28] Up until now there is no report on the thermomagnetization behavior of the FSMA ribbons annealed at high temperature over 1000 K. Here after annealing at 1073 K the austenite magnetiza- tion M aust ͑100 Oe͒ between T A and T C varies in a way that FSMAs behave under high magnetic field ͑generally over 1 T͒ ͑Refs. 25, 26, 29, and 30͒ or that the saturation magnetization M S ͑T͒ / M S ͑0͒ typically acts as a function of the temperature T / T C for ferromagnetic materials.…”
Section: B Magnetic Characteristicsmentioning
confidence: 99%
“…They concluded that this alloy, on heating, undergoes a first-order magnetocrystalline transition from tetragonal martensite to a cubic austenite structure at a transformation temperature, T M , ranging from 175 K to 220 K; followed by a second-order ferromagnetic-paramagnetic transition identified with a Curie temperature of the austenite phase, T C , between 375 K and 380 K; the transitions are reversible with temperature [10,11]. Later it was found [12][13][14][15][16] that the supposed transition temperatures, T M and T C , could made nearly coincident either by doping the alloy with Co or Cu or by slightly varying the alloy composition in the off-stoichiometric form of Ni 50+X Mn 25−X−Y Ga 25+Y , with X ≈ 5 and Y ≈ l-2. The isothermal magnetization versus field loops displayed large hysteresis losses and the magnetization characteristics indicative of a field-induced magneto-structural phase transformation [17][18][19][20][21][22].…”
Section: Introductionmentioning
confidence: 99%