Specific heat measurements in superconducting and normal state Ta-Nb-V ternary solid solutions

1978 ◽  
Vol 32 (3-4) ◽  
pp. 481-494 ◽  
Author(s):  
R. Y. P. Wang ◽  
R. L. Cappelletti
1999 ◽  
Vol 103 (1-3) ◽  
pp. 2080 ◽  
Author(s):  
Nathanael A. Fortune ◽  
Guruswamy Rajaram ◽  
Keizo Murata

1994 ◽  
Vol 230 (3-4) ◽  
pp. 397-406 ◽  
Author(s):  
P.C. Canfield ◽  
B.K. Cho ◽  
D.C. Johnston ◽  
D.K. Finnemore ◽  
M.F. Hundley
Keyword(s):  

1977 ◽  
Vol 20 (2) ◽  
pp. 224-227 ◽  
Author(s):  
G. I. Kalishevich ◽  
L. F. Lutskaya ◽  
P. V. Gel'd ◽  
Yu. V. Putintsev

1980 ◽  
Vol 58 (2) ◽  
pp. 164-167 ◽  
Author(s):  
Douglas L. Martin

The results of specific heat measurements on ordered In −51.67 at.% Mg are presented. A superconducting transition was seen at about 0.95 K. In the normal state, the lattice specific heat varies in the usual way with temperature, i.e., the Debye temperature initially decreases with increasing temperature. This behavior was also seen in ordered equiatomic CuPt but in ordered equiatomic CuAu I the Debye temperature first goes through a maximum before decreasing to the usual minimum. The structure of all three alloys consists of alternating layers of different mass and it was initially supposed that the CuAu I result was a two-dimensional effect. However, the more recent and normal results on InMg and CuPt make this improbable and it appears that the CuAu I result is related to the behavior of pure gold which is itself anomalous.


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