What is the effect on the Berry phase?

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    Berry phase Phase
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SUMMARY

The discussion centers on the effect of modifying a Hamiltonian H[s] by a function f[s] on the Berry phase γn[C] for a closed curve C. The Berry phase is defined through the integral γn[C] = ∫∫A[C] dA e[s] ⋅ Vn[s], where Vn[s] is derived from the eigenstates of H. The participants express confusion regarding the nature of the closed curve and the implications of the Hamiltonian's slow variation. The relationship between the Berry phase and the Aharonov-Bohm effect is also explored, highlighting the significance of the curve's topology in determining the phase.

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  • Understanding of quantum mechanics, specifically Hamiltonians and eigenstates.
  • Familiarity with the concept of the Berry phase in quantum systems.
  • Knowledge of vector calculus, particularly in the context of parameter spaces.
  • Basic principles of the Aharonov-Bohm effect and its implications in quantum mechanics.
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  • Study the derivation and implications of the Berry phase in quantum mechanics.
  • Explore the mathematical formulation of the Aharonov-Bohm effect and its relation to Berry phases.
  • Investigate the role of slowly varying parameters in quantum systems and their effects on eigenstates.
  • Learn about the topology of closed curves in parameter spaces and their impact on quantum phases.
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Quantum physicists, graduate students in physics, and researchers interested in the geometric phases in quantum mechanics.

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No Effort: Member warned that some effort must be shown on homework questions
Homework Statement
Consider a Hamiltonian H[s] that depends on a number of slowly varying parameters collectively called s(t). What is the effect on the Berry phase γn[C] for a given closed curve C, if H[s] is replaced with f[s] H[s], where f[s] is an arbitrary real numerical function of the s?
Relevant Equations
.
Homework Statement :
Consider a Hamiltonian H[s ] that depends on a number of slowly varying parameters collectively called s(t). What is the effect on the Berry phase γn[C] for a given closed curve C, if H[s ] is replaced with f[s ] H[s ], where f[s ] is an arbitrary real numerical function of the s?Homework Equations :
For any s, we can find a complete orthonormal set of eigenstates Φn of H with eigenvalues En(s):
n = EnΦn
n, Φm) = δnm
.Attempt at a Solution :
Could you help me to solve this problem?
Please...
 
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Do you know the equation for the Berry phase?
 
In the special case where i and j run over three values,
γn[C] = ∫∫A[C] dA e[s ] ⋅ Vn[s ], ----- (1)
where e[s ] is the unit vector normal to the surface A[C] at the point s, and Vn[s ] is a three-vector in parameter space:
Vn[s ] ≡ i m≠n{(Φn[s ], [∇H [s ]] Φm[s ])* × (Φn[s ], [∇H [s ]] Φm[s ])} × (Em[s ] - En[s ])-2.
 
I don't understand. Is the closed curve given or is it arbitrary? In the Aharonov-Bohm effect, do you not get different answers if your integration encloses or doesn't enclose the solenoid?

Why do you think that you are told the function is slowly varying?
 

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