Abstract
The notion of adiabatic evolution or adiabatic process is an important theoretical concept, which occurs at several places in Physics. The main feature of this concept is that although the process is very slow, global changes can take place without local changes. Adiabaticity is at the border between dynamics and statics. This concept was introduced by Boltzmann in Classical Mechanics through the notion of adiabatic invariants. In Thermodynamics adiabatic processes play an important role. In Quan tum Mechanics, if the state of the system is an eigenfunction ψ(t o) for the eigenvalue e(t o) at t = t o, then in the adiabatic limit the state of the system at time t = t 1 is an eigenfunction ψ(t 1) for the eigenvalue e(t 1), provided the energy-level e(t) remains isolated during the time-interval [t 0,t 1]. Even if H(t o) = H(t 1), the eigenfunction ψ(t 1) is generally different from ψ(t o) by a phase which can be decomposed into a dynamical phase related to the energy-level e(t) and a geometric phase related to the spectral subspaces visited during the adiabatic process. This is the fundamental observation of Berry 1 which gave rise to extensive developments during the last ten years2,3,4.
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Joye, A., Pfister, CE. (1994). Quantum Adiabatic Evolution. In: Fannes, M., Maes, C., Verbeure, A. (eds) On Three Levels. NATO ASI Series, vol 324. Springer, Boston, MA. https://doi.org/10.1007/978-1-4615-2460-1_13
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DOI: https://doi.org/10.1007/978-1-4615-2460-1_13
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