Physics:Quantum Aharonov-Bohm effect: Difference between revisions
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{{Short description|Quantum phase effect caused by electromagnetic potentials}} | {{Short description|Quantum phase effect caused by electromagnetic potentials}} | ||
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|image=[[File:Quantum_aharonov_bohm_effect_yellow.png|430px|Aharonov-Bohm phase shift around a shielded magnetic flux.]] | |image=[[File:Quantum_aharonov_bohm_effect_yellow.png|430px|Aharonov-Bohm phase shift around a shielded magnetic flux.]] | ||
|text=The '''Quantum Aharonov-Bohm effect''' is a quantum phenomenon in which charged | |text=The '''Quantum Aharonov-Bohm effect''' is a quantum-mechanical phenomenon in which an electrically charged particle can be affected by electromagnetic potentials even while moving through a region where the classical electric and magnetic fields are zero.<ref>{{Cite web |title=Aharonov-Bohm effect |url=https://en.wikipedia.org/wiki/Aharonov%E2%80%93Bohm_effect |publisher=Wikipedia |access-date=2026-05-23}}</ref> | ||
The effect is most often illustrated with electron interference around a confined magnetic flux. The electrons do not pass through the magnetic field, but their wavefunction phases depend on the vector potential associated with the enclosed flux. When the two paths recombine, the interference pattern shifts. | |||
}} | }} | ||
== | == Magnetic Aharonov-Bohm effect == | ||
In the standard magnetic version, a coherent electron beam is split into two paths that pass on opposite sides of a long solenoid. The magnetic field is confined inside the solenoid, so the electrons travel in a region where the classical Lorentz force is zero. Nevertheless, the vector potential changes the relative phase of the electron wavefunctions. | |||
The phase shift around a closed path is proportional to the magnetic flux enclosed by the path: | |||
<math display="block">\Delta \phi = {q \over \hbar}\oint \mathbf{A}\cdot d\mathbf{l} = {q\Phi_B \over \hbar}.</math> | |||
Here <math>q</math> is the particle charge, <math>\mathbf{A}</math> is the vector potential, and <math>\Phi_B</math> is the enclosed magnetic flux. The observable consequence is a shift in the interference fringes. | |||
== Potentials and phase == | |||
Classical electromagnetism is often described in terms of the electric and magnetic fields, because those fields determine the local force on a charged particle. Quantum mechanics is more phase-sensitive. The wavefunction phase couples directly to the electromagnetic potentials, and interference can reveal this coupling even when the fields vanish along the particle paths. | |||
This does not make the vector potential an arbitrary mathematical decoration. In quantum theory, gauge potentials help determine phase relations. Gauge transformations can change the local expression for the potential, but they do not change the measured phase shift around a closed loop. | |||
== Electric version == | |||
There is also an electric Aharonov-Bohm effect, in which a scalar potential changes the phase of a charged particle even when the particle is not exposed to a classical electric field along its path. The electric and magnetic forms both show that quantum phases can encode information about potentials in field-free regions. | |||
== Significance == | == Significance == | ||
The Aharonov-Bohm effect is important in | The Aharonov-Bohm effect is important for several reasons: | ||
* it demonstrates the physical significance of electromagnetic potentials in quantum mechanics; | |||
* it connects interference, gauge invariance, and topology; | |||
* it provides a clear example of how global path information can affect a local measurement; | |||
* it underlies many ideas in mesoscopic physics, superconducting circuits, and topological quantum systems. | |||
The effect is closely related to [[Physics:Quantum Berry phase|Berry phase]] and other geometric phases. In both cases, the phase acquired by a quantum state depends on a path in a space of parameters or gauge fields, not merely on local forces along the path. | |||
== See also == | == See also == | ||
{{#invoke:PhysicsQC|tocHeadingAndList|Physics:Quantum basics/See also}} | |||
== References == | == References == | ||
Latest revision as of 22:19, 23 May 2026
The Quantum Aharonov-Bohm effect is a quantum-mechanical phenomenon in which an electrically charged particle can be affected by electromagnetic potentials even while moving through a region where the classical electric and magnetic fields are zero.[1]
The effect is most often illustrated with electron interference around a confined magnetic flux. The electrons do not pass through the magnetic field, but their wavefunction phases depend on the vector potential associated with the enclosed flux. When the two paths recombine, the interference pattern shifts.
Magnetic Aharonov-Bohm effect
In the standard magnetic version, a coherent electron beam is split into two paths that pass on opposite sides of a long solenoid. The magnetic field is confined inside the solenoid, so the electrons travel in a region where the classical Lorentz force is zero. Nevertheless, the vector potential changes the relative phase of the electron wavefunctions.
The phase shift around a closed path is proportional to the magnetic flux enclosed by the path:
Here is the particle charge, is the vector potential, and is the enclosed magnetic flux. The observable consequence is a shift in the interference fringes.
Potentials and phase
Classical electromagnetism is often described in terms of the electric and magnetic fields, because those fields determine the local force on a charged particle. Quantum mechanics is more phase-sensitive. The wavefunction phase couples directly to the electromagnetic potentials, and interference can reveal this coupling even when the fields vanish along the particle paths.
This does not make the vector potential an arbitrary mathematical decoration. In quantum theory, gauge potentials help determine phase relations. Gauge transformations can change the local expression for the potential, but they do not change the measured phase shift around a closed loop.
Electric version
There is also an electric Aharonov-Bohm effect, in which a scalar potential changes the phase of a charged particle even when the particle is not exposed to a classical electric field along its path. The electric and magnetic forms both show that quantum phases can encode information about potentials in field-free regions.
Significance
The Aharonov-Bohm effect is important for several reasons:
- it demonstrates the physical significance of electromagnetic potentials in quantum mechanics;
- it connects interference, gauge invariance, and topology;
- it provides a clear example of how global path information can affect a local measurement;
- it underlies many ideas in mesoscopic physics, superconducting circuits, and topological quantum systems.
The effect is closely related to Berry phase and other geometric phases. In both cases, the phase acquired by a quantum state depends on a path in a space of parameters or gauge fields, not merely on local forces along the path.
See also
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References
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