Analysis of the magnetoresistance of three-dimensional amorphous metals with weak localization and electron-electron interaction theories

1992 ◽  
Vol 4 (1) ◽  
pp. 177-188 ◽  
Author(s):  
P Lindqvist
1996 ◽  
Vol 10 (28) ◽  
pp. 1397-1406 ◽  
Author(s):  
AXEL VÖLKER ◽  
PETER KOPIETZ

We use the Lanczos method to calculate the variance σ2(E, ϕ) of the number of energy levels in an energy window of width E below the Fermi energy for noninteracting disordered electrons on a thin three-dimensional ring threaded by an Aharonov–Bohm flux ϕ. We confirm numerically that for small E the flux-dependent part of σ2(E, ϕ) is well described by the Altshuler–Shklovskii-diagram involving two Cooperons. However, in the absence of electron–electron interactions this result cannot be extrapolated to energies E where the energy-dependence of the average density of states becomes significant. We discuss consequences for persistent currents and argue that for the calculation of the difference between the canonical- and grand canonical current it is crucial to take the electron–electron interaction into account.


2014 ◽  
Vol 551 ◽  
pp. 195-199 ◽  
Author(s):  
Bunju Shinozaki ◽  
Kazuya Hidaka ◽  
Syouhei Ezaki ◽  
Kazumasa Makise ◽  
Takayuki Asano ◽  
...  

2007 ◽  
Vol 105 (1) ◽  
pp. 223-226 ◽  
Author(s):  
E. N. Tkachev ◽  
A. I. Romanenko ◽  
O. B. Anikeeva ◽  
T. I. Buryakov ◽  
V. E. Fedorov ◽  
...  

Open Physics ◽  
2010 ◽  
Vol 8 (3) ◽  
Author(s):  
Željana Lošić ◽  
Paško Županović

AbstractWe investigate the collective mode dispersions for the tight-binding dielectric matrix with two one-dimensional electron bands per donor and acceptor chains, and the three-dimensional long-range Coulomb electron-electron interaction within the random phase approximation. The hybridized collective modes are the result of the strong coupling between the intraband plasmon and the interband dipolar modes due to strong dipole Coulomb interactions. Our calculations show the existence of the low-energy renormalized plasmon mode above the electron-hole quasi-continuum in the long wavelength limit. The obtained modes are brought into correspondence with the optical data of quasi-one-dimensional organic conductor tetrathiafulvalene-tetracyanoquinodimethane (TTF-TCNQ). Namely, the renormalized plasmon and the dipolar mode are assigned to the observed excitations at respective energy scales of roughly 10 meV and 0.75 eV, explaining why lower excitation is eliminated while higher excitation persists below the temperature of the Peierls phase transition.


1986 ◽  
Vol 76 ◽  
Author(s):  
S. Ishida ◽  
K. Murase ◽  
Y. Shimamoto ◽  
K. Ishibashi ◽  
K. Gamo ◽  
...  

ABSTRACTThe low-temperature magnetoresistance of PtSi thin wires of varying width, prepared with different mask elements (Cu and Ni) in the reactive ion beam etching, has been studied, to determine the width dependence of the physical parameters in the weak localization. A drastic decrease of the magnetic impurity scattering time τs and that of the superconducting transition temperature Tc have been found for the wires prepared by Ni mask with narrowing width, which suggests that the phase coherence of diffusing electrons responsible for the weak localization and the superconductivity are strongly affected by the presence of a small amount of Ni impurities recoil implanted into the surface region of the sidewalls of wires.


2010 ◽  
Vol 24 (12n13) ◽  
pp. 2053-2071
Author(s):  
N. Giordano

A brief and selective review of experimental studies of electrical conduction in thin metal wires and films at low temperatures is given. This review will illustrate the importance of various length scales and of dimensionality in determining the properties disordered metals. A few intriguing and still unresolved experimental findings are also mentioned.


2014 ◽  
Vol 104 (15) ◽  
pp. 153114 ◽  
Author(s):  
Mingsheng Long ◽  
Youpin Gong ◽  
Xiangfei Wei ◽  
Chao Zhu ◽  
Jianbao Xu ◽  
...  

1997 ◽  
Vol 102 (1) ◽  
pp. 41-46 ◽  
Author(s):  
M Aprili ◽  
J Lesueur ◽  
L Dumoulin ◽  
P Nédellec

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