Superconducting Behavior of Tetragonal T ‘Eu2‐xCexO4±δ

1989 ◽  
Vol 169 ◽  
Author(s):  
V. J. Melim ◽  
Weimin Peng ◽  
C.W. Kimball ◽  
B. Dabrowski ◽  
Y. Zheng ◽  
...  

AbstractEu2.xCexCuO4±δ (0 ≤ x ≤ 0.17) has been synthesized with the tetragonal T’ structure. AC susceptibility and resistance measurements show that Eu2‐xCexCuO4±δ becomes superconducting with τc∼13 K for x= 0.15 and 0.17, when prepared under reducing conditions. The 151Eu Mossbauer shift shows that the Euvalence falls into a narrow range near Eu 3+ . The temperature dependence of the Mossbauer absorption yields a Debye temperature of 319 K for the Eu ion in Eu1.85Ce0.15CuO4±δ

2000 ◽  
Vol 215-216 ◽  
pp. 260-263 ◽  
Author(s):  
H Sassik ◽  
M Schönhart ◽  
R Grössinger ◽  
R Sato Turtelli ◽  
A Kottar

1997 ◽  
Vol 282-287 ◽  
pp. 1991-1992
Author(s):  
P.N. Mikheenko ◽  
J. Horvat ◽  
M. Ionescu ◽  
S.X. Dou

The amplitude of the de Haas-van Alphen oscillations in mercury has been studied at temperatures between 1 and 17 K and fields between 20 and 90 T. Because of the low Debye temperature of mercury, the Dingle temperature X might be expected to increase appreciably with temperature because of increased scattering of electrons by phonons. Such a temperature dependent X would also cause the appropriate logarithmic plot of amplitude against temperature to depart appreciably from linearity. Measurements of X as a function of temperature and of the temperature dependence of amplitude at a number of fields have however provided no evidence of any appreciable temperature dependence of X . This apparently paradoxical result turns out to be explicable by a recent many-body theory due to Engelsberg & Simpson of the effects of electron-phonon scattering on the de Haas-van Alphen amplitude.


InterConf ◽  
2021 ◽  
pp. 307-314
Author(s):  
Z. Nizomov ◽  
R. Saidzoda (Saidov) ◽  
B. Gulov ◽  
J. Sharipov

The results of comparison of heat capacity of aluminum, copper, silicon, magnesium and zinc with Debye's theory depending on temperature are given in the paper. It was revealed that the main components of the heat capacity of metals are the lattice component; is a component due to thermal expansion and is an electronic contribution. It is proposed that when creating the theory of heat capacity, it is necessary to take into account the anharmonicity of the oscillations of atoms in the nodes of the crystal lattice and the change in Debye temperature.


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