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Are there theorems for sufficient and necessary conditions for the vanishing of Berry and/or Wilzeck-Zee phases for a given quantum mechanical system?
There are no established theorems providing sufficient and necessary conditions for the vanishing of Berry and Wilczek-Zee phases in quantum mechanical systems. However, general conditions exist to assess the vanishing of these phases. Specifically, if the Hamiltonian of the system is time-independent, the Berry phase will always vanish. In contrast, the Wilczek-Zee phase may vanish if the Hamiltonian is periodic in time.
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