Quantum coherence in sub-10 nm metal wires

2000 ◽  
Vol 636 ◽  
Author(s):  
Douglas Natelson ◽  
Robert L. Willett ◽  
Kenneth W. West ◽  
Loren N. Pfeiffer

AbstractWe report weak localization studies of quantum coherence in metal nanowires with widths as small as 5 nm, demonstrating that structures fabricated at sub-50 nm length scales can reveal coherence phenomena not accessible in larger devices. Through selective etching of cleaved molecular-beam epitaxy (MBE)-grown substrates, we produce precise nanoscale surface relief then used as a stencil for metal deposition. This nonlithographic method of lateral definition allows the fabrication of metal (AuPd) nanowires greater than one micron in length with widths below 5 nm, a previously unexplored size regime in studies of quantum corrections to the conductance of disordered metals. Analyzing magnetoresistance data, we find that the coherence time, Tφ, shows a low temperature T dependence close to quasi-1D theoretical expectations (Tφ ∼ T-2/3 in 5 nm wide wires, while exhibiting a relative saturation as T 0 for wide samples of the same material. Since an externally controlled parameter, the sample geometry, can cause a single material to exhibit both suppression and divergence ofTφ, this finding provides a new constraint on models of dephasing phenomena.

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.


1996 ◽  
Vol 76 (4) ◽  
pp. 668-671 ◽  
Author(s):  
A. V. Herzog ◽  
P. Xiong ◽  
F. Sharifi ◽  
R. C. Dynes

2001 ◽  
Vol 15 (04) ◽  
pp. 321-371 ◽  
Author(s):  
GEN TATARA

The resistivity due to a domain wall in a ferromagnetic metal is calculated based on a linear response theory. The scattering by impurities is taken into account. The electron-wall interaction is derived from the exchange interaction between the conduction electron and the magnetization by use of a local gauge transformation in the spin space. This interaction is treated perturbatively to the second order. The classical (Boltzmann) contribution from the wall scattering turns out to be negligiblly small if the wall is thick compared with the fermi wavelength. In small contacts a large classical domain wall resistance is expected due to a thin wall trapped in the constriction. In the dirty case, where quantum coherence among electrons becomes important at low temperature, spin flip scattering caused by the wall results in dephasing and hence suppresses weak localization. Thus the quantum correction due to the wall can lead to a decrease of resistivity. This effect grows rapidly at low temperature where the wall becomes the dominant source of dephasing. Conductance change in the quantum region caused by the motion of the wall is also calculated.


1989 ◽  
Vol 66 (11) ◽  
pp. 5409-5411 ◽  
Author(s):  
D. El‐Khatouri ◽  
A. Khater ◽  
M. Balkanski ◽  
J. Tuchendler

2015 ◽  
Vol 17 (19) ◽  
pp. 12826-12832 ◽  
Author(s):  
Yuan Jin ◽  
Xiao-Peng Cui ◽  
Wei-Hua Han ◽  
Shi-Xun Cao ◽  
Yu-Ze Gao ◽  
...  

We report the low temperature resistance upturn is mainly due to the quantum correction effects driven by the weak localization and the electron–electron interaction in such a strongly correlated system, and the contribution of each factor varies with grain boundaries.


2007 ◽  
Vol 21 (08n09) ◽  
pp. 1519-1523
Author(s):  
M. L. Peres ◽  
V. A. Chitta ◽  
G. M. Gusev ◽  
Nei F. Oliveira ◽  
P. H. O. Rappl ◽  
...  

We investigated the magnetotransport properties of n- and p-type films of Pb 1-x Eu x Te grown by molecular beam epitaxy, with Eu concentrations close to the Metal-Insulator transition. The n-type sample shows a negative magnetoresistance which magnitude increases continually as the temperature is lowered. On the other hand, for the p-type sample, a negative magnetoresistance can be observed only for temperatures below 7 K. Comparing the magnetoresistance of both samples we show that the scattering mechanism should have a different origin.


2003 ◽  
Vol 237 (2) ◽  
pp. 500-512 ◽  
Author(s):  
Mi-Ae Park ◽  
Kerim Savran ◽  
Yong-Jihn Kim

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