Aharonov–Casher effect explained

The Aharonov–Casher effect is a quantum mechanical phenomenon predicted in 1984 by Yakir Aharonov and Aharon Casher,[1] in which a traveling magnetic dipole is affected by an electric field. It is dual to the Aharonov–Bohm effect, in which the quantum phase of a charged particle depends upon which side of a magnetic flux tube it comes through. In the Aharonov–Casher effect, the particle has a magnetic moment and the tubes are charged instead. It was observed in a gravitational neutron interferometer in 1989[2] and later by fluxon interference of magnetic vortices in Josephson junctions.[3] It has also been seen with electrons and atoms.

In both effects the particle acquires a phase shift (

\varphi

) while traveling along some path P. In the Aharonov–Bohm effect it is

\varphi\rm=

q
\hbar

\intPAdx

While for the Aharonov–Casher effect it is

\varphi\rm=

1
\hbarc2

\intP(E x \boldsymbol\mu)dx

where

q

is its charge and

\boldsymbol\mu

is the magnetic moment. The effects have been observed together.[4]

References

  1. Y. Aharonov . A. Casher . Topological quantum effects for neutral particles . Phys. Rev. Lett. . 1984 . 53 . 319–321 . 10.1103/PhysRevLett.53.319 . 4. 1984PhRvL..53..319A .
  2. A. Cimmino . G. I. Opat . A. G. Klein. H. Kaiser . S. A. Werner . M. Arif . R. Clothier . Observation of the topological Aharonov–Casher phase shift by neutron interferometry . Phys. Rev. Lett. . 1989 . 63 . 380–383 . 10.1103/PhysRevLett.63.380 . 4 . 10041058. 1989PhRvL..63..380C .
  3. W. J. Elion . J. J. Wachters . L. L. Sohn. J. D. Mooij . Observation of the Aharonov–Casher effect for vortices in Josephson-junction arrays . Phys. Rev. Lett. . 1993 . 71 . 2311–2314 . 10.1103/PhysRevLett.71.2311 . 14 . 10054641. 1993PhRvL..71.2311E .

Bibliography

See also