Aharonov–Casher effect

{{Short description|Quantum-mechanical phenomenon}}

{{No footnotes|date=November 2019}}

The Aharonov–Casher effect is a quantum mechanical phenomenon predicted in 1984 by Yakir Aharonov and Aharon Casher,{{cite journal | author=Y. Aharonov | author2=A. Casher | title=Topological quantum effects for neutral particles | journal=Phys. Rev. Lett. | date=1984 | volume=53 | pages=319–321 | doi=10.1103/PhysRevLett.53.319 | url=http://www.tau.ac.il/~yakir/yahp/yh98 | issue=4|bibcode = 1984PhRvL..53..319A }} 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 {{cite journal | author=A. Cimmino | author2=G. I. Opat | author3=A. G. Klein| author4=H. Kaiser | author5=S. A. Werner | author6= M. Arif | author7=R. Clothier | title=Observation of the topological Aharonov–Casher phase shift by neutron interferometry | journal=Phys. Rev. Lett. | date=1989 | volume=63 | pages=380–383 | doi=10.1103/PhysRevLett.63.380 | url=http://www.atomwave.org/rmparticle/ao%20refs/aifm%20refs%20sorted%20by%20topic/Topological%20phases/a-c%20effect%20expts/Cimmino_PRL_1989.pdf | issue=4 | pmid=10041058|bibcode = 1989PhRvL..63..380C }} and later by fluxon interference of magnetic vortices in Josephson junctions.{{cite journal | author=W. J. Elion | author2=J. J. Wachters | author3=L. L. Sohn| author4=J. D. Mooij | title=Observation of the Aharonov–Casher effect for vortices in Josephson-junction arrays | journal=Phys. Rev. Lett. | date=1993 | volume=71 | pages=2311–2314 | doi=10.1103/PhysRevLett.71.2311 | url=http://repository.tudelft.nl/view/ir/uuid%3A1fc70550-ac87-49fd-af97-bf0372b260f0/ | issue=14 | pmid=10054641|bibcode = 1993PhRvL..71.2311E }} 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 AB} = \frac{q}{\hbar} \int_P \mathbf{A} \cdot d\mathbf{x}

While for the Aharonov–Casher effect it is

:\varphi_{\rm AC} = \frac{1}{\hbar c^2} \int_P (\mathbf{E}\times \boldsymbol \mu) \cdot d\mathbf{x}

where q is its charge and \boldsymbol \mu is the magnetic moment. The effects have been observed together.* {{cite journal | author=E. N. Bogachek | author2=U. Landman | title=Aharonov–Bohm and Aharonov–Casher tunneling effects and edge states in double-barrier structures | journal=Phys. Rev. B | date=1994 | volume=50 | doi=10.1103/PhysRevB.50.2678 | url=http://www.physics.gatech.edu/files/u26/papers/0164.pdf | issue=4 | pages=2678–2680| pmid=9976496 |bibcode = 1994PhRvB..50.2678B }}

References

Bibliography

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| title=Direct Observation of the Aharonov–Casher Phase | journal=Phys. Rev. Lett. | date=2006 | volume=96 | doi=10.1103/PhysRevLett.96.076804 | arxiv=cond-mat/0508396 | issue=7 |bibcode = 2006PhRvL..96g6804K | pmid=16606124 | pages=076804| s2cid=7934918 }}

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  • {{citation |last1=Frydman |first1=Aviad |title=Aharonov-casher Effect With Vortices In An Amorphous Superconductor |date=6 Mar 2020 |work=Bulletin of the American Physical Society |volume=65 |issue=1 |last2=Arnab |first2=Roy |url=https://meetings.aps.org/Meeting/MAR20/Session/W58.1}}

See also

{{DEFAULTSORT:Aharonov-Casher effect}}

Category:Quantum mechanics

Category:Physical phenomena

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