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Time Symmetry and Asymmetry in Quantum Mechanics and Quantum Cosmology
General Relativity and Quantum Cosmology · Submitted 18 Apr 1993
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim A special initial condition and a final condition of indifference would be sufficient to explain the observed time asymmetries of the universe.
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
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The abstract, sentence by sentence
We investigate the origin of the arrow of time in quantum mechanics in the context of quantum cosmology. The ``Copenhagen'' quantum mechanics of measured subsystems incorporates a fundamental arrow of time. Extending discussions of Aharonov, Bergmann and Lebovitz, Griffiths, and others we investigate a generalized quantum mechanics for cosmology that utilizes both an initial and a final density matrix to give a time-neutral formulation without a fundamental arrow of time. Time asymmetries can arise for particular universes from differences between their initial and final conditions. Theories for both would be a goal of quantum cosmology. A special initial condition and a final condition of indifference would be sufficient to explain the observed time asymmetries of the universe. In this essay we ask under what circumstances a completely time symmetric universe, with T-symmetric initial and final condition, could be consistent with the time asymmetries of the limited domain of our experience. We discuss the approach to equilibrium, the electromagnetic system, and T-violation in the weak interactions in such universes. The decoherence of alternatives that is necessary for the prediction of probabilities in the quantum mechanics of closed systems is the origin of a fundamental limitation on quantum cosmologies with initial and final conditions. The initial and final density matrices cannot both be pure; if they are there is no decoherence and no prediction.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We investigate the origin of the arrow of time in quantum mechanics in the context of quantum cosmology. | contribution 0.80 | 0.81 | 0.05 | unclear 0.56 |
| s1 | The ``Copenhagen'' quantum mechanics of measured subsystems incorporates a fundamental arrow of time. | background 1.00 | 0.06 | 0.05 | asserted 1.00 |
| s2 | Extending discussions of Aharonov, Bergmann and Lebovitz, Griffiths, and others we investigate a generalized quantum mechanics for cosmology that utilizes both an initial and a final density matrix to give a time-neutral formulation without a fundamental arrow of time. | contribution 0.71 | 0.61 | 0.16 | asserted 0.84 |
| s3 | Time asymmetries can arise for particular universes from differences between their initial and final conditions. | result 0.61 | 0.27 | 0.23 | hedged possibility 0.77 |
| s4 | Theories for both would be a goal of quantum cosmology. | future work 0.84 | 0.05 | 0.06 | asserted 0.41 |
| s5 | A special initial condition and a final condition of indifference would be sufficient to explain the observed time asymmetries of the universe. | result 0.51 | 0.25 | 0.33 | hedged possibility 0.50 |
| s6 | In this essay we ask under what circumstances a completely time symmetric universe, with T-symmetric initial and final condition, could be consistent with the time asymmetries of the limited domain of our experience. | contribution 0.81 | 0.32 | 0.09 | hedged possibility 0.80 |
| s7 | We discuss the approach to equilibrium, the electromagnetic system, and T-violation in the weak interactions in such universes. | contribution 0.92 | 0.41 | 0.04 | unclear 0.63 |
| s8 | The decoherence of alternatives that is necessary for the prediction of probabilities in the quantum mechanics of closed systems is the origin of a fundamental limitation on quantum cosmologies with initial and final conditions. | result 0.55 | 0.57 | 0.32 | asserted 1.00 |
| s9 | The initial and final density matrices cannot both be pure; if they are there is no decoherence and no prediction. | result 0.60 | 0.61 | 0.26 | asserted 1.00 |
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The paper
Original abstract
We investigate the origin of the arrow of time in quantum mechanics in the context of quantum cosmology. The ``Copenhagen'' quantum mechanics of measured subsystems incorporates a fundamental arrow of time. Extending discussions of Aharonov, Bergmann and Lebovitz, Griffiths, and others we investigate a generalized quantum mechanics for cosmology that utilizes both an initial and a final density matrix to give a time-neutral formulation without a fundamental arrow of time. Time asymmetries can arise for particular universes from differences between their initial and final conditions. Theories for both would be a goal of quantum cosmology. A special initial condition and a final condition of indifference would be sufficient to explain the observed time asymmetries of the universe. In this essay we ask under what circumstances a completely time symmetric universe, with T-symmetric initial and final condition, could be consistent with the time asymmetries of the limited domain of our experience. We discuss the approach to equilibrium, the electromagnetic system, and T-violation in the weak interactions in such universes. The decoherence of alternatives that is necessary for the prediction of probabilities in the quantum mechanics of closed systems is the origin of a fundamental limitation on quantum cosmologies with initial and final conditions. The initial and final density matrices cannot both be pure; if they are there is no decoherence and no prediction.
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References
How the literature uses it
19 arXiv papers cite this in 25 sentences
Papers citing it · 17 sentences without a confident label
Cites it as support 1 paper
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DHQM of the universe can be formulated time neutrally with initial and final conditions playing symmetric roles in the formulation [ref] and no built in arrows of time.
Quantum Buzzwords · The Quantum Arrow of Time · 0.99
Cites it as background 7 papers
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Setting $ρ^(f)$ to the identity reproduces the usual formulation of quantum mechanics and has been termed by Gell-Mann and Hartle [ref] as the principle of indifference.
No Future in Black Holes · Introduction · 0.86
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Such time-symmetric cosmologies have been proposed by Gold, Wheeler, Hawking and Hartle and Gell-Mann, the latter two in the context of quantum cosmology [ref] .
Teleocosmology and quantum post-selection · Physical interpretation and discussion · 0.97
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Several distinct arrows of time can be identified in nature, based on intrinsic temporal asymmetries observed in different classes of physical phenomena [ref] :
Arrows of time in bouncing cosmologies · Arrows of time and their cosmological origin · 0.89
Discussion
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