Geometry of quantum evolution
Abstract
For an arbitrary quantum evolution, it is shown that the integral of the uncertainty of energy with respect to time is independent of the particular Hamiltonian used to transport the quantum system along a given curve in the projective Hilbert space. It is the distance along this curve measured by the Fubini-Study metric. This gives a new time-energy uncertainty principle. New geometric meanings to time as measured by a clock and the transition probability during a quantum measurement are also obtained.
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Another bound, based on the average energy E, was established by Margolus and Levitin.
“Another bound, based on the average energy E , was established by Margolus and Levitin.”
From Fundamental Limit on the Rate of Quantum Dynamics: The Unified Bound Is Tight (2009) · cites this paper as [3]
The bounds coincide, and can be exactly attained by certain initial states if ΔE = E.
“The bounds coincide, and can be exactly attained by certain initial states if ∆ E = E .”
From Fundamental Limit on the Rate of Quantum Dynamics: The Unified Bound Is Tight (2009) · cites this paper as [3]
The Anandan-Aharonov relation states that the speed of evolution of a quantum state is 2ħ^{-1} ΔH.
“This relation is indeed natural if we recall the Anandan-Aharonov relation [12] which states that the 'speed' of the evolution of a given quantum state is given by 2h -1 H .”
From Elementary derivation for passage times (2003) · cites this paper as [12]
The above expression generalizes in a unified manner previous results derived in Refs. [7-22].
“The above expression generalizes in an unified manner previous results derived in Refs. [7, 8, 9, 10, 11, 12, 13, 14, 15, 16, 17, 18, 19, 20, 21, 22].”
From Energy–time uncertainty relation for driven quantum systems (2013) · cites this paper as [7]
The correct interpretation of the time-energy Heisenberg uncertainty principle is that a quantum state with spread in energy ΔE takes time at least Δt = π hbar/2ΔE to evolve to an orthogonal state.
“In particular, the correct interpretation of the time-energy Heisenberg uncertainty principle ∆ E ∆ t ≥ ¯ h is not that it takes time ∆ t to measure energy to an accuracy ∆ E (a fallacy that was put to rest by Aharonov and Bohm 23 -24 ) but rather that that a quantum state with spread in energy ∆ E takes time at least ∆ t = π ¯ h/ 2∆ E to evolve to an orthogonal (and hence distinguishable) state 2”
From Ultimate physical limits to computation (2000) · cites this paper as [25]
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“In the case of a pure state, the fact that squared velocity of the state evolution is given by the energy uncertainty is known as the Anandan–Aharonov relation [21].”
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- Authors
- Anandan, J., & Aharonov, Y.
- Affiliations
- University of Cambridge (GB)
- University of South Carolina (US)
- Venue
- Physical Review Letters
- Publisher
- American Physical Society (APS)
- Published
- 1990-10-01
- Volume
- 65
- Issue
- 14
- Pages
- 1697-1700
- ISSN
- 0031-9007 (ISSN-L)
- OpenAlex
- W2017028422
- Cited by
- 794
- References
- 2
- Citations by year
- 2026: 46 · 2025: 59 · 2024: 50 · 2023: 51 · 2022: 53 · 2021: 49 · 2020: 48 · 2019: 32 · 2018: 34 · 2017: 24 · 2016: 28 · 2015: 36 · 2014: 25 · 2013: 29 · 2012: 22
- FWCI
- 5.30
- Type
- journal article
- Language
- en
- Open access
- closed
- Locations
- Physical Review Letters (publishedVersion)
- PubMed (publishedVersion)
- Topics
- Physical Sciences › Physics and Astronomy › Atomic and Molecular Physics, and Optics › Quantum Mechanics and Applications
- Physical Sciences › Physics and Astronomy › Statistical and Nonlinear Physics › Quantum chaos and dynamical systems
- Physical Sciences › Computer Science › Artificial Intelligence › Quantum Information and Cryptography
- Keywords
- time-energy uncertainty relation, quantum evolution, projective Hilbert space, Fubini-Study metric, quantum clocks, quantum measurement, transition probabilities, quantum geometry
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