Final States in Quantum Cosmology: Cosmic Acceleration as a Quantum Post-Selection Effect

Fuente: arXiv
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Autore principale: Anastopoulos, Charis
Natura: Preprint
Pubblicazione: 2024
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author Anastopoulos, Charis
author_facet Anastopoulos, Charis
contents Standard quantum theory admits naturally statistical ensembles that are both pre-selected and post-selected, i.e., they involve both an initial and a final state. We argue that there is no compelling physical reason to preclude a probability assignment with a final quantum state at the cosmological level. We therefore analyze the implications of a final state in the probability assignment for quantum cosmology. To this end, we derive effective classical equations of motion for systems subject to both initial and final conditions. Remarkably, these effective equations do not depend on the details of the quantum theory, but only on the geometric features of the classical state space. When applied to Friedman-Robertson-Walker cosmological models, these effective equations generically describe cosmic acceleration in the absence of a cosmological constant, dark energy, or modified gravitational dynamics. Therefore, cosmic acceleration emerges as a quantum post-selection effect, that is, a macroscopic quantum phenomenon.
format Preprint
id arxiv_https___arxiv_org_abs_2401_07662
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Final States in Quantum Cosmology: Cosmic Acceleration as a Quantum Post-Selection Effect
Anastopoulos, Charis
General Relativity and Quantum Cosmology
Cosmology and Nongalactic Astrophysics
Quantum Physics
Standard quantum theory admits naturally statistical ensembles that are both pre-selected and post-selected, i.e., they involve both an initial and a final state. We argue that there is no compelling physical reason to preclude a probability assignment with a final quantum state at the cosmological level. We therefore analyze the implications of a final state in the probability assignment for quantum cosmology. To this end, we derive effective classical equations of motion for systems subject to both initial and final conditions. Remarkably, these effective equations do not depend on the details of the quantum theory, but only on the geometric features of the classical state space. When applied to Friedman-Robertson-Walker cosmological models, these effective equations generically describe cosmic acceleration in the absence of a cosmological constant, dark energy, or modified gravitational dynamics. Therefore, cosmic acceleration emerges as a quantum post-selection effect, that is, a macroscopic quantum phenomenon.
title Final States in Quantum Cosmology: Cosmic Acceleration as a Quantum Post-Selection Effect
topic General Relativity and Quantum Cosmology
Cosmology and Nongalactic Astrophysics
Quantum Physics
url https://arxiv.org/abs/2401.07662