scholarly journals Overactivated transport in the localized phase of the superconductor-insulator transition

2021 ◽  
Vol 12 (1) ◽  
Author(s):  
V. Humbert ◽  
M. Ortuño ◽  
A. M. Somoza ◽  
L. Bergé ◽  
L. Dumoulin ◽  
...  

AbstractBeyond a critical disorder, two-dimensional (2D) superconductors become insulating. In this Superconductor-Insulator Transition (SIT), the nature of the insulator is still controversial. Here, we present an extensive experimental study on insulating NbxSi1−x close to the SIT, as well as corresponding numerical simulations of the electrical conductivity. At low temperatures, we show that electronic transport is activated and dominated by charging energies. The sample thickness variation results in a large spread of activation temperatures, fine-tuned via disorder. We show numerically and experimentally that this originates from the localization length varying exponentially with thickness. At the lowest temperatures, there is an increase in activation energy related to the temperature at which this overactivated regime is observed. This relation, observed in many 2D systems shows that conduction is dominated by single charges that have to overcome the gap when entering superconducting grains.

1994 ◽  
Vol 08 (07) ◽  
pp. 905-912 ◽  
Author(s):  
I. Terry ◽  
T. Penney ◽  
S. von Molnár ◽  
P. Becla

A series of resistivity curves is obtained as a function carrier concentration in just one sample of the dilute magnetic persistent photoconductor Cd0.91Mn0.09Te:In. The measurements, made at carrier concentrations approaching the metal-insulator transition, reveal a cross-over from an exp(To/T)1/2 dependence to an exp(EH/T) form when lowering temperature. The exp(To/T)1/2 dependence is characteristic of variable range hopping in the presence of Coulomb interactions, while the energy EH in the activated form is associated with a hard gap in the density of states that is magnetic in origin. All the data are shown to scale onto a single curve. The localization length. ξ, is found to have the same critical dependence on carrier concentration as that of the measured dielectric constant, κ, when approaching the metal-insulator transition. The temperature dependence of the resistivity is interpreted in terms of the orientation of Mn spins by carriers due to the s-d exchange interaction (the formation of magnetic polarons). This model can also account for the large positive and negative magnetoresistance observed in Cd0.91Mn0.09Te:In at low temperatures.


1991 ◽  
Vol 185-189 ◽  
pp. 1337-1338 ◽  
Author(s):  
C. Quitmann ◽  
M. Fleuster ◽  
C. Jarchow ◽  
D. Andrich ◽  
P.L. Paulose ◽  
...  

2006 ◽  
Vol 75 (4) ◽  
pp. 611-617 ◽  
Author(s):  
G Sambandamurthy ◽  
A Johansson ◽  
E Peled ◽  
D Shahar ◽  
P. G Björnsson ◽  
...  

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

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

2013 ◽  
Vol 9 (7) ◽  
pp. 415-418 ◽  
Author(s):  
Maoz Ovadia ◽  
David Kalok ◽  
Benjamin Sacépé ◽  
Dan Shahar

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