Magnetic properties of Co-Cu metastable solid solution alloys

2004 ◽  
Vol 69 (9) ◽  
Author(s):  
Xu Fan ◽  
Tsutomu Mashimo ◽  
Xinsheng Huang ◽  
Tomoko Kagayama ◽  
Akira Chiba ◽  
...  
Atomic Energy ◽  
2000 ◽  
Vol 88 (1) ◽  
pp. 42-47 ◽  
Author(s):  
V. K. Orlov ◽  
V. M. Teplinskaya ◽  
N. T. Chebotarev

2008 ◽  
Vol 59 (4) ◽  
pp. 444-447 ◽  
Author(s):  
K OKADA ◽  
S KOHIKI ◽  
F TSUTSUI ◽  
H SHIMOOKA ◽  
M MITOME ◽  
...  

RSC Advances ◽  
2017 ◽  
Vol 7 (4) ◽  
pp. 2019-2024 ◽  
Author(s):  
Jianming Deng ◽  
Aimei Yang ◽  
M. A. Farid ◽  
Hao Zhang ◽  
Jian Li ◽  
...  

The solid solution (Eu1−xMnx)MnO3−δ (0 ≤ x ≤ 0.126) has been synthesized using a conventional solid-state method.


1981 ◽  
Vol 7 ◽  
Author(s):  
G. Battaglin ◽  
A. Carnera ◽  
G. Della Mea ◽  
P. Mazzoldi ◽  
Animesh K. Jain ◽  
...  

ABSTRACTWe present a comparative study (by 1.8 MeV 4He+ ion channeling) of virgin, self and Eu implanted single crystals of nickel, under irradiation with single ruby laser pulses. The as implanted Eu is nearly non-substitutional and remains so, even after laser treatment. The comparative defect dechanneling behaviour provides explicit evidence of defect-impurity interaction which may be suppressing the formation of an expected metastable solid solution in the Eu-Ni system, which possesses miscibility in the liquid phase. A clear surface Eu peak appears at 2.1 J/cm2.


2018 ◽  
Vol 56 (1A) ◽  
pp. 197
Author(s):  
Nguyen Hoang Tuan

In this study, we present some results on the structure and properties of the solid solution of Bi0.5K0.5TiO3– BiFeCoO3 (BKT – BFCO) by Sol-gel method. Crystal structures of BKT – BFCO solid solutions were studies by XRD and Raman spectroscopy. The results were in good agreement with the previous reports of Bi0.5K0.5TiO3– BiFeO3 (BKT – BFO) and Bi0.5K0.5TiO3 – BiCoO3 (BKT – BCO) solid solutions. The magnetic properties were investigated via unsaturated M-H loop, which showed the competition of paramagnetic and antiferromagnetic ordering in BKT – BFCO. However, differing from the BKT – BFO and BKT – BCO solid solutions, the unclear values of saturated magnetism in BKT – BFCO raised the unexplained question, which needed further studies.


2006 ◽  
Vol 408-412 ◽  
pp. 1205-1209 ◽  
Author(s):  
Md. Tahidul Haque ◽  
Hirohisa Satoh ◽  
Naoki Kamegashira

1979 ◽  
Vol 46 (6) ◽  
pp. 1740-1747 ◽  
Author(s):  
Fumitaka Matsubara ◽  
Sakari Inawashiro

2004 ◽  
Vol 1 (7) ◽  
pp. 1706-1710 ◽  
Author(s):  
M. S. Ben Kraiem ◽  
M. Ellouze ◽  
A. Cheikh-Rouhou ◽  
Ph. L'Héritier

1993 ◽  
Vol 07 (01n03) ◽  
pp. 716-720
Author(s):  
B. WALL ◽  
M. KATTER ◽  
W. RODEWALD ◽  
M. VELICESCU

In cast Sm2Fe17 ingots minor fractions of SmFe2 and SmFe3 may occur. Nitrogenation of such alloy-powders inidicates that only Sm2Fe17 forms an interstitial solid solution whereas SmFe2 and SmFe3 decompose directly into SmN and α-Fe. From Sm2Fe17Nx alloy powders with an average particle size of about 3 μm anisotropic magnets were prepared by adding 15 wt% Zn-powder. Annealing at 390 ºC results in intrinsic coercivities > 15 kOe promoted by the formation of an unknown binary Fe8Zn92-compound. Whereas annealing at temperatures > 420 ºC leads to the formation of binary Fe3Zn7 and ternary Sm2FeZn2. By the formation of Sm2FeZn2 from Sm2Fe17Nx+Zn some α-Fe occurs inducing a step in the demagnetization curve J(H).


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