Principles of Quantum Mechanics · Problem 18.16

Time-Dependent Perturbation Theory — R. Shankar

Physics — Quantum Mechanics · adiabatic-approximation

Problem

Show that the Berry phase γn(t)=i∫0t⟨n(t′)∣n˙(t′)⟩ dt′\gamma_n(t) = i\int_0^t \langle n(t')|\dot{n}(t')\rangle\, dt' is real. [Hint: Differentiate the normalization condition ⟨n(t)∣n(t)⟩=1\langle n(t)|n(t)\rangle = 1 with respect to tt.]

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