TY - JOUR
T1 - Structure and Magnetic Properties of the ThMn12 Type NdFeM Alloys (M=Si/Al/B/Transition Metals)
AU - Chin, T. S.
AU - Chang, W. C.
AU - Ku, H. C.
AU - Weng, C. C.
AU - Lee, H. T.
AU - Hung, M. P.
N1 - Funding Information:
Acknowledgement The authors are grateful for the sponsorship of this project by the National Science Council of the Rep. of China, under the contract No. NSC 77-0405-E007-24. The help of Mr. S.K. Chen in magnetic measurements is gratefully acknowledged.
PY - 1989/9
Y1 - 1989/9
N2 - Among the 13 Nd(Fe, M)12 alloys studied, where M=Si, Al B, Ti, V, Cr, Mn, Zr, Ht, Nb, W, Mo, and Ta, those with Si, Ti, V, Cr, Mn, Mo, and W are tetragonal ThMn12(1-12 for short) type structure. For the other alloys, existence of either Fe3M, Fe2M, FeM, and/or FeM2 phases is evidenced from X-ray diffraction (XRD). The size of M atom is found crucial in determining its ability to stabilize the 1–12 phase. When M is Ti in NdFe 12-xMx alloys, the 1–12 phase exists in a wide range or x-values from 0.7-2.0, however Fe2Ti phase appears when x exceeds 1.0. Hence NdFe11Ti is not likely a line compound. For the other alloys with 1–12 phase only x=2 was examined. The c/a value keeps invariant at 0.558 to 0.559 when M is transition metal, and 0.564 for M = si. Curie temperatures(Tc) of these alloys, in decreasing order of M, are V (310 C), Si (301 C), Ti (278 C), Cr (270 C), W (252 C), Mo (195 C), and Mn (119 C); for the alloy with Ti, x=1 and for the others x=2. The determined anisotropy field (Ha) for these alloys from aligned polycrystalline powder at room temperature is low, the maximum one is 26.8 kOe for NdFe11Ti, which increases to 54.5 kOe at 4.2 K.
AB - Among the 13 Nd(Fe, M)12 alloys studied, where M=Si, Al B, Ti, V, Cr, Mn, Zr, Ht, Nb, W, Mo, and Ta, those with Si, Ti, V, Cr, Mn, Mo, and W are tetragonal ThMn12(1-12 for short) type structure. For the other alloys, existence of either Fe3M, Fe2M, FeM, and/or FeM2 phases is evidenced from X-ray diffraction (XRD). The size of M atom is found crucial in determining its ability to stabilize the 1–12 phase. When M is Ti in NdFe 12-xMx alloys, the 1–12 phase exists in a wide range or x-values from 0.7-2.0, however Fe2Ti phase appears when x exceeds 1.0. Hence NdFe11Ti is not likely a line compound. For the other alloys with 1–12 phase only x=2 was examined. The c/a value keeps invariant at 0.558 to 0.559 when M is transition metal, and 0.564 for M = si. Curie temperatures(Tc) of these alloys, in decreasing order of M, are V (310 C), Si (301 C), Ti (278 C), Cr (270 C), W (252 C), Mo (195 C), and Mn (119 C); for the alloy with Ti, x=1 and for the others x=2. The determined anisotropy field (Ha) for these alloys from aligned polycrystalline powder at room temperature is low, the maximum one is 26.8 kOe for NdFe11Ti, which increases to 54.5 kOe at 4.2 K.
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U2 - 10.1109/20.42283
DO - 10.1109/20.42283
M3 - Article
AN - SCOPUS:0024738999
SN - 0018-9464
VL - 25
SP - 3300
EP - 3302
JO - IEEE Transactions on Magnetics
JF - IEEE Transactions on Magnetics
IS - 5
ER -