Spin-reorientation transitions and crystalline-electric-field parameters inRFe10T2(R=rare earth;T=Si or V) intermetallic compounds

1991 ◽  
Vol 44 (5) ◽  
pp. 2182-2189 ◽  
Author(s):  
C. Christides ◽  
M. Anagnostou ◽  
Hong-Shuo Li ◽  
A. Kostikas ◽  
D. Niarchos
1999 ◽  
Vol 577 ◽  
Author(s):  
Nguyen Hoang Luong ◽  
Nguyen Phu Thuy ◽  
Pham Hong Quang ◽  
Pham Duc Thang

ABSTRACTIn this work the rare-earth anisotropy in the rare-earth - transition metal intermetallic compounds is investigated by studying the temperature-induced spin reorientation phenomena on aligned powder samples and by analyzing the temperature dependence of the magnetization measured along different principal axes of single crystals. From such investigations the crystalline-electric-field parameters of the rare-earth ions in these compounds have been derived. The results on different hard magnetic materials of the compositions R2Fe14B, RFe11 and their substituted compounds as well as R2Co17 are summarized.


1992 ◽  
Vol 115 (2-3) ◽  
pp. 281-286 ◽  
Author(s):  
Han Xiu-feng ◽  
Jin Han-min ◽  
Chen Hong ◽  
Guo Guang-hua ◽  
Zhao Tie-song

1965 ◽  
Vol 86 (6) ◽  
pp. 1235-1238 ◽  
Author(s):  
M N Ghatikar ◽  
A K Raychaudhuri ◽  
D K Ray

The theory that has been developed for rare-earth ions in crystals is here applied to the double nitrates. The paramagnetic resonance data and certain spectroscopic properties of the different rare-earth double nitrates, depending as they do on the crystalline electric field at a rare-earth ion, are related to the six parameters through which the field is defined. It is found that most of the experimental results can be fitted to values of the parameters that vary in a systematic fashion along the rare-earth series.


1996 ◽  
Vol 10 (29) ◽  
pp. 1471-1476
Author(s):  
MIRCEA ANDRECUT

The temperature dependence of the second-order crystalline electric field (CEF) parameters of rare earth intermetallic compound CeZn 2 was deduced from the least-squares nonlinear fit to the reciprocal paramagnetic susceptibility along principal crystalline axes. The results of the calculation are in good agreement with the experimental values.


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