scholarly journals Anisotropic temperature dependence of normal state resistivity in underdoped region of a layered electron-doped superconductor Nd2–xCexCuO4

2019 ◽  
Vol 45 (2) ◽  
pp. 217-223 ◽  
Author(s):  
A. S. Klepikova ◽  
T. B. Charikova ◽  
N. G. Shelushinina ◽  
M. R. Popov ◽  
A. A. Ivanov
1991 ◽  
Vol 185-189 ◽  
pp. 1239-1240 ◽  
Author(s):  
Shoichi Nagata ◽  
Mikio Nakajima ◽  
Kan-ichi Kido ◽  
Toshimi Ikeda ◽  
Susumu Chikazawa

1989 ◽  
Vol 39 (13) ◽  
pp. 9611-9613 ◽  
Author(s):  
S. Martin ◽  
M. Gurvitch ◽  
C. E. Rice ◽  
A. F. Hebard ◽  
P. L. Gammel ◽  
...  

1990 ◽  
Vol 04 (13) ◽  
pp. 863-870 ◽  
Author(s):  
H.C. LEE ◽  
S.G. LEE ◽  
Y.C. KIM ◽  
K.S. YI ◽  
M.S. JANG

The superconducting properties of CaBaLaCu 3 O y with Tc=76 K were reported. The X-ray diffraction pattern analysis shows that the CaBaLaCu3Oy compound has tetragonal structure at room temperature. The superconductivity of this compound was confirmed from the temperature dependence of electrical resistivity and self-inductance. We also examined the temperature dependence of the normal-state resistivity ρ(T) from 300 K to 900 K. From the linear behavior of ρ(T) in the range Tc<T<620 K, the strength of electron-phonon coupling constant λ and the electron mean free path l are obtained from the standard electron-phonon dissipation mechanism. Our estimated value of λ≃0.62 implies that the superconductivity of CaBaLaCu 3 O y is not to be interpreted only in terms of the phonon-mediated electron-electron interaction.


2000 ◽  
Vol 61 (17) ◽  
pp. 11752-11761 ◽  
Author(s):  
Anurag Gupta ◽  
Ratan Lal ◽  
A. Sedky ◽  
A. V. Narlikar ◽  
V. P. S. Awana

1987 ◽  
Vol 01 (03n04) ◽  
pp. 1067-1070 ◽  
Author(s):  
M. Petravić ◽  
A. Hamzić ◽  
B. Leontić ◽  
L. Forró

We present Hall effect measurements in the normal state of the high temperature superconducting ceramics La2−xSrxCuO4 (x=0, 0.1, 0.15, 0.2, 0.25, 0.3), YBa2Cu3o7 and GdBa2Cu3O7 . The first family has temperature independent Hall constant for x>0, while in the other two systems RH is proportional to 1/T. From the Hall effect it follows that the transport in these compounds is hole-like.


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