Undergrad Aharonov-Bohm Effect & Adiabatic Approximation

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SUMMARY

The discussion centers on the Aharonov-Bohm (A-B) effect and its relation to the adiabatic approximation as presented in Griffiths' textbook on Quantum Mechanics. The A-B effect illustrates a net phase change around a closed loop, which is a key concept in quantum mechanics. Although Griffiths introduces the A-B effect in the context of the adiabatic approximation, it is clarified that the A-B effect does not require adiabatic conditions, highlighting its broader significance in quantum theory. The conversation emphasizes the pedagogical choice of Griffiths to simplify the introduction of net phase changes using the adiabatic approximation.

PREREQUISITES
  • Understanding of Quantum Mechanics principles, particularly the adiabatic theorem.
  • Familiarity with the Aharonov-Bohm effect and its implications in quantum systems.
  • Knowledge of geometric phases, specifically the Berry phase.
  • Basic grasp of Hamiltonian mechanics and nonholonomic systems.
NEXT STEPS
  • Study the derivation of the geometric Berry phase from Griffiths' Quantum Mechanics textbook.
  • Explore the implications of the Aharonov-Bohm effect in various quantum systems.
  • Investigate nonholonomic systems and their measurable phenomena in quantum mechanics.
  • Learn about the mathematical foundations of the adiabatic approximation in quantum mechanics.
USEFUL FOR

Students and educators in quantum mechanics, physicists interested in the implications of the Aharonov-Bohm effect, and researchers exploring geometric phases and adiabatic processes in quantum systems.

Silviu
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Hello! I am reading Griffiths book on QM and in the chapter about the adiabatic approximation he introduces the Aharonov-Bohm effect. I am not sure why is this effect an example of adiabatic approximation. The hamiltonian doesn't depend on time as the vector potential is not a function of time so I don't really see how does this fit in the chapter. Griffiths mentions, indeed, that the same effect holds even when the vector potential depends on time, but again, there is nothing mentioned about slow change (which is required for the adiabatic approximation to hold). Can someone explain to me what is Griffiths actually doing there? Thank you!
 
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Silviu said:
Can someone explain to me what is Griffiths actually doing there?
Since no one else has answered, here's my $0.02...

Chapter 10 of Griffiths progresses through the following sequence:

-- The adiabatic theorem,

-- Nonholonomic systems (in which interesting measurable phenomena can happen even adiabatically, by transport around a closed loop),

-- Geometric Berry phase (which is an example of such "interesting, measurable" phenomena). He derives the geometric net phase change formula [10.49] using the adiabatic approximation back in [10.40]. See his remarks under point 3 on p338.

-- Then he gives an example of an electron in a magnetic field of constant magnitude, but changing direction, (still using the adiabatic approximation), and derives the net phase change of the electron wave function.

-- Then he moves on the A-B effect (presumably because it involves a net phase change around a closed loop, similar to geometric phase). BUT, as he notes on p348 after eq[10.95], in this case the process of going around the solenoid doesn't have to be adiabatic.

I'm not sure why Griffiths does it this way. Maybe it's because the general idea of net phase change around a closed loop is easier to present at introductory level if one uses the adiabatic approximation (which simplifies some of the math). But the A-B effect, which doesn't need the adiabatic approximation, shows that net phase change around a closed loop is of far more general importance in QM, not merely in the restricted circumstances of the adiabatic approximation.

HTH.
 
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