
TL;DR
This paper introduces the concept of weak energy in quantum mechanics, linking it to phases, geometric structures, and uncertainty relations, and explores its implications for quantum state evolution and measurement.
Contribution
It defines the weak energy of evolution and the pointed weak energy, establishing their properties, geometric interpretations, and connections to known quantum phases and principles.
Findings
Weak energy manifests as dynamical and geometric phases.
Weak energy satisfies a stationary action principle.
Imaginary part of pointed weak energy relates to survival probability.
Abstract
The equation of motion for a time-independent weak value of a quantum mechanical observable contains a complex valued energy factor - the weak energy of evolution. This quantity is defined by the dynamics of the pre-selected and post-selected states which specify the observable's weak value. It is shown that this energy: (i) is manifested as dynamical and geometric phases that govern the evolution of the weak value during the measurement process; (ii) satisfies the Euler-Lagrange equations when expressed in terms of Pancharatnam (P) phase and Fubini-Study (FS) metric distance; (iii) provides for a PFS stationary action principle for quantum state evolution; (iv) time translates correlation amplitudes; (v) generalizes the temporal persistence of state normalization; and (vi) obeys a time-energy uncertainty relation. A similar complex valued quantity - the pointed weak energy of an…
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