Determination of Curie temperature by Arrott plot technique in Gd5(SixGe1−x)4 for x>0.575

2008 ◽  
Vol 320 (20) ◽  
pp. e696-e698 ◽  
Author(s):  
R.L. Hadimani ◽  
Y. Melikhov ◽  
J.E. Snyder ◽  
D.C. Jiles
1976 ◽  
Vol 34 (2) ◽  
pp. K135-K137 ◽  
Author(s):  
S. Feierabend ◽  
U. Kishko ◽  
R. Niedermayer

2017 ◽  
Vol 53 (11) ◽  
pp. 1-4
Author(s):  
L. M. Moreno-Ramirez ◽  
V. Franco ◽  
M. Pekala ◽  
A. Conde

JETP Letters ◽  
2013 ◽  
Vol 97 (3) ◽  
pp. 141-144 ◽  
Author(s):  
N. I. Nurgazizov ◽  
D. A. Bizyaev ◽  
A. A. Bukharaev ◽  
V. N. Lisin ◽  
A. P. Chuklanov

Author(s):  
L.P. Barbosa ◽  
H. Takiishi ◽  
R.N. Faria ◽  
Daniel Rodrigues ◽  
S.R. Janasi

2010 ◽  
Vol 24 (1-2) ◽  
pp. 805-808
Author(s):  
P. Vašek ◽  
P. Svoboda ◽  
V. Novák ◽  
Z. Výborný ◽  
V. Jurka ◽  
...  

1977 ◽  
Vol 55 (17) ◽  
pp. 1481-1484 ◽  
Author(s):  
R. A. MacDonald ◽  
C. V. Stager

Magnetization and crystallographic measurements are reported for the Heusler alloy series (NixCu1−x)2MnSn. With the exception of Cu2MnSn and perhaps (Ni0.1Cu0.9)2MnSn all of the samples prepared had the cubic Heusler L21 structure at room temperature. The lattice parameter varies linearly as a function of composition. The saturation moment is constant at approximately 4μβ per manganese atom throughout the series. Curie temperatures vary smoothly but non-linearly with composition, providing some evidence for at least two competing mechanisms in the determination of the Curie temperature.


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