Low-temperature electrical conductivity and the superconductor-insulator transition induced by indium impurity states in (Pb0.5Sn0.5)1 − x In x Te solid solutions

2010 ◽  
Vol 52 (9) ◽  
pp. 1815-1819 ◽  
Author(s):  
D. V. Shamshur ◽  
R. V. Parfen’ev ◽  
A. V. Chernyaev ◽  
S. A. Nemov
2019 ◽  
Vol 34 (01) ◽  
pp. 2050008
Author(s):  
V. A. Abdurahmanova ◽  
N. M. Abdullaev ◽  
Sh. S. Ismayilov

The temperature range of [Formula: see text] = 77–770 K in the system alloys: Holl coefficient [Formula: see text], thermo-emf [Formula: see text], electric conductivity [Formula: see text], measured [Formula: see text]-density of components and analyzed. It has been established that samarium additive atoms contain donor-type properties and the effectiveness increases with the temperature increase: up to 40% proportional to [Formula: see text] K in [Formula: see text]-type specimens, whereas in [Formula: see text]-type samples this increase is higher and covers the contents of pH varying from [Formula: see text] to [Formula: see text]. An electrical conductivity of compounds increased due to the carrier activation with further increase of temperature. The activation energy of carriers at low temperatures ([Formula: see text] K) is [Formula: see text] eV for [Formula: see text] mol.% and [Formula: see text] mol.% compounds at [Formula: see text] = 77–320 K and for [Formula: see text] mol.% and [Formula: see text] mol.% compounds are [Formula: see text] eV. [Formula: see text] const at [Formula: see text]–400 K for [Formula: see text] mol.% and [Formula: see text] mol.% compounds, and passing with minimum increases at [Formula: see text] = 400–500 K.


2021 ◽  
Vol 229 ◽  
pp. 01056
Author(s):  
Mohamed Errai ◽  
Said Amrane

The electrical transport properties in sample 1 of impurity concentration n=xx of the 70Ge: Ga system are studied in the absence of a magnetic field and at low temperature in the range 0.53 to 0.017 K. It is noted that the electrical conductivity of sample 1 exhibits a metallic behavior. We found that the exponent S is equal to 0.5 (σ=σ(T=0)+mTs). This result is in agreement with the theory of weak localization (WL) at 3D and the theory of electronelectron interactions (EEI). We also found that sample 1 is located near the metal-insulator transition (MIT) of the metallic side.


JETP Letters ◽  
1998 ◽  
Vol 68 (4) ◽  
pp. 363-369 ◽  
Author(s):  
V. F. Gantmakher ◽  
M. V. Golubkov ◽  
V. T. Dolgopolov ◽  
G. E. Tsydynzhapov ◽  
A. A. Shashkin

2021 ◽  
pp. 2100532
Author(s):  
Panjuan Tang ◽  
Stefano Livraghi ◽  
Elio Giamello ◽  
Sebastiano Garroni ◽  
Luca Malfatti ◽  
...  

2008 ◽  
Vol 179 (27-32) ◽  
pp. 1432-1435 ◽  
Author(s):  
Elena Konysheva ◽  
John T.S. Irvine ◽  
Astrid Besmehn

1997 ◽  
Vol 78 (13) ◽  
pp. 2632-2635 ◽  
Author(s):  
A. J. Rimberg ◽  
T. R. Ho ◽  
Ç. Kurdak ◽  
John Clarke ◽  
K. L. Campman ◽  
...  

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