Aharanov-Bohm Effect: Difference between revisions
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'''Yakir Aharonov'''(b. 1932)<br> | '''Yakir Aharonov''' (b. 1932)<br> | ||
'''David Bohm'''(b.1917) | '''David Bohm''' (b.1917) | ||
'''''AharonovâBohm effect''''' 1959 | '''''AharonovâBohm effect''''' 1959 | ||
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== Discussion: == | == Discussion: == | ||
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Latest revision as of 20:08, 30 January 2021
Yakir Aharonov (b. 1932)
David Bohm (b.1917)
AharonovâBohm effect 1959
The AharonovâBohm effect, sometimes called the EhrenbergâSidayâAharonovâBohm effect, is a quantum mechanical phenomenon in which an electrically charged particle is affected by an electromagnetic potential (Ď, A), despite being confined to a region in which both the magnetic field B and electric field E are zero. The underlying mechanism is the coupling of the electromagnetic potential with the complex phase of a charged particle's wave function, and the AharonovâBohm effect is accordingly illustrated by interference experiments.