2022
DOI: 10.1209/0295-5075/ac8caf
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Time Fisher information associated with fluctuations in quantum geometry

Abstract: As time is not an observable, we use Fisher information (FI) to address the problem of time. We show that the Hamiltonian constraint operator cannot be used to analyze any quantum process for quantum geometries that are associated with time-reparametrization invariant classical geometries. This is because the Hamiltonian constraint does not contain FI about time. We demonstrate that although the Hamiltonian operator is the generator of time, the Hamiltonian constraint operator can not observe the change that a… Show more

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Cited by 9 publications
(17 citation statements)
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“…Now θ is defined as the unobservable variable probed by this operator [38,39]. Since θ acts as the time for the systems, and M 2 plays the same role as the Hamiltonian [38,39], we can write the θ evolution of a world-sheet mode |ϕ i m 0 ⟩ from θ = 0 to θ as…”
Section: Margolus-levitin Boundmentioning
confidence: 99%
See 4 more Smart Citations
“…Now θ is defined as the unobservable variable probed by this operator [38,39]. Since θ acts as the time for the systems, and M 2 plays the same role as the Hamiltonian [38,39], we can write the θ evolution of a world-sheet mode |ϕ i m 0 ⟩ from θ = 0 to θ as…”
Section: Margolus-levitin Boundmentioning
confidence: 99%
“…According to this equation, θ parameterizes the evolution of a string state to another orthogonal string state. This is expected as the unobservable parameter θ is viewed as time in string theory [38,39]. However, there is a bound on θ, and it is not possible for orthogonal string states to evolve into each other faster than this bound.…”
Section: Margolus-levitin Boundmentioning
confidence: 99%
See 3 more Smart Citations