Home
For authors
Submission status

Current
Archive
Archive (English)
   Volumes 41-62
   Volumes 1-20
   Volumes 21-40
      Volume 40
      Volume 39
      Volume 38
      Volume 37
      Volume 36
      Volume 35
      Volume 34
      Volume 33
      Volume 32
      Volume 31
      Volume 30
      Volume 29
      Volume 28
      Volume 27
      Volume 26
      Volume 25
      Volume 24
      Volume 23
      Volume 22
      Volume 21
Search
VOLUME 33 (1981) | ISSUE 2 | PAGE 101
The Aaronov-Bohm effect in disordered conductors
It is shown that the Aaronov-Bohm effect, which is manifested in the oscillations of the kinetic coefficients as a function of the magnetic flux that penetrates the sample, must exist in disordered normal conductors. The period of these oscillations is Φ0 = bc/2e, i.e., it is half as large as in the ordinary Aaronov-Bohm effect.