scholarly journals Direct observation of ensemble averaging of the Aharonov-Bohm effect in normal-metal loops

1986 ◽  
Vol 56 (4) ◽  
pp. 386-389 ◽  
Author(s):  
C. P. Umbach ◽  
C. Van Haesendonck ◽  
R. B. Laibowitz ◽  
S. Washburn ◽  
R. A. Webb
1987 ◽  
Vol 59 (16) ◽  
pp. 1791-1794 ◽  
Author(s):  
S. Washburn ◽  
H. Schmid ◽  
D. Kern ◽  
R. A. Webb

1986 ◽  
Vol 56 (2) ◽  
pp. 189-192 ◽  
Author(s):  
A. Douglas Stone ◽  
Y. Imry

1996 ◽  
Vol 10 (26) ◽  
pp. 3595-3608 ◽  
Author(s):  
B.C. GUPTA ◽  
P. SINGHA DEO ◽  
A.M. JAYANNAVAR

It is known that differential magnetoconductance of a normal metal loop connected to reservoirs by ideal wires is always negative when an electron travels as an evanescent modes in the loop. This is in contrast to the fact that the magnetoconductance for propagating modes is very sensitive to small changes in geometric details and the Fermi energy and moreover it can be positive as well as negative. Here we explore the role of impurities in the leads in determining the magnetoconductance of the loop. We find that the change in magnetoconductance is negative and can be made large provided the impurities do not create resonant states in the systems. This theoretical finding may play a useful role in quantum switch operations.


1986 ◽  
Vol 35 (4) ◽  
pp. 375-422 ◽  
Author(s):  
Sean Washburn ◽  
Richard A. Webb

Physics Today ◽  
1986 ◽  
Vol 39 (1) ◽  
pp. 17-20 ◽  
Author(s):  
Bertram Schwarzschild

1994 ◽  
Vol 08 (05) ◽  
pp. 301-310 ◽  
Author(s):  
A.M. JAYANNAVAR ◽  
P. SINGHA DEO

We have investigated the magnetoconductance of a normal metal loop connected to ideal wires in the presence of magnetic flux. The quantum mechanical potential, V, in the loop is much higher than that in the connecting wires (V=0). The electrons with energies less than the potential height on entering the loop propagate as evanescent modes. In such a situation, the contribution to the conductance arises from two non-classical effects, namely, Aharonov-Bohm effect and quantum tunneling. For this case we show that, on application of a small magnetic field, the conductance initially always decreases, or small field magnetoconductance is always negative. This is in contrast to the behavior in the absence of the barrier, wherein the small field magnetoconductance is either positive or negative depending on the Fermi energy and other geometric details. We also discuss the possibility of a better switch action based on quantum interference effects in such structures.


1985 ◽  
Vol 32 (7) ◽  
pp. 4789-4792 ◽  
Author(s):  
S. Washburn ◽  
C. P. Umbach ◽  
R. B. Laibowitz ◽  
R. A. Webb

1986 ◽  
Vol 33 (6) ◽  
pp. 4303-4306 ◽  
Author(s):  
C. P. Umbach ◽  
S. Maekawa ◽  
R. B. Laibowitz ◽  
S. P. McAlister

Sign in / Sign up

Export Citation Format

Share Document