The Classical Universes of the No-Boundary Quantum State
James B. Hartle, S. W. Hawking, Thomas Hertog

TL;DR
This paper investigates how the no-boundary quantum state leads to classical universe histories, highlighting the conditions for classicality, the role of inflation, and the influence of quantum probabilities on observable universe features.
Contribution
It provides a detailed analysis of classical histories arising from the no-boundary proposal in minisuperspace models, emphasizing the conditions for classicality and inflationary biases.
Findings
Classical histories require a minimum scalar field for late-time classical behavior.
The ensemble of histories is time symmetric, but individual histories are not.
The measure favors small inflation, but large e-foldings are probabilistically enhanced by volume factors.
Abstract
We analyze the origin of the quasiclassical realm from the no-boundary proposal for the universe's quantum state in a class of minisuperspace models. The models assume homogeneous, isotropic, closed spacetime geometries, a single scalar field moving in a quadratic potential, and a fundamental cosmological constant. The allowed classical histories and their probabilities are calculated to leading semiclassical order. We find that for the most realistic range of parameters analyzed a minimum amount of scalar field is required, if there is any at all, in order for the universe to behave classically at late times. If the classical late time histories are extended back, they may be singular or bounce at a finite radius. The ensemble of classical histories is time symmetric although individual histories are generally not. The no-boundary proposal selects inflationary histories, but the…
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