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Tunneling wave function of the universe (1808.02032v2)

Published 6 Aug 2018 in gr-qc and hep-th

Abstract: The tunneling wave function of the universe is investigated in a minisuperspace framework of a de Sitter universe with a quantum scalar field, treated as a perturbation. We consider three different approaches to defining the tunneling wave function: (1) tunneling boundary conditions in superspace, (2) Lorentzian path integral, and (3) quantum tunneling from initial universe of a vanishing size. We show that the superspace approach requires Robin boundary conditions for the scalar field modes, the path integral approach requires adding an appropriate boundary term to the scalar field action, and the initial universe approach requires the initial quantum state of the scalar field to be Euclidean vacuum. We find that all three approaches yield identical wave functions and that scalar field fluctuations are well behaved, contrary to earlier claims in the literature.

Citations (70)

Summary

Tunneling Wave Function of the Universe

In this paper, Alexander Vilenkin and Masaki Yamada address the concept of the tunneling wave function of the universe within the framework of quantum cosmology. Their analysis centers around three approaches to defining the tunneling wave function of the universe: tunneling boundary conditions in superspace, Lorentzian path integral, and quantum tunneling from an initial universe of vanishing size. These three methodologies are applied in a minisuperspace framework, specifically focusing on a de Sitter universe with a quantum scalar field treated as a perturbation.

Summary of Approaches

The authors present a thorough investigation of the tunneling wave function using these approaches:

  1. Tunneling boundary conditions in superspace: The tunneling boundary condition is characterized by outgoing waves at the boundary of superspace, supplemented by a regularity condition ensuring boundary finiteness. This approach requires Robin boundary conditions for the scalar field modes, unlike the traditional Dirichlet boundary conditions usually adopted.
  2. Lorentzian path integral formulation: By employing Picard-Lefschetz theory, Vilenkin and Yamada standardize the path integral formulation of quantum cosmology. The appropriate boundary term is added to the scalar field action, guaranteeing that field fluctuations remain well-behaved and the resulting wave function aligns with the one derived using tunneling boundary conditions.
  3. Quantum tunneling from initial universe model: In this model, the initial quantum state is taken as the Euclidean vacuum. The boundary term added to the scalar field action within this approach ensures congruence with the tunneling proposal, demonstrating a universe nucleating from 'nothing'.

Findings and Implications

Interestingly, Vilenkin and Yamada find that all three methodologies yield identical wave functions with well-behaved scalar field fluctuations. Their findings challenge earlier claims suggesting runaway instabilities in the tunneling wave function. This convergence across approaches not only supports the robustness of quantum tunnology as a viable framework but also contributes significantly to the discourse on quantum cosmology's handling of initial conditions in the universe.

The exploration of boundary conditions, specifically transitioning from Dirichlet to Robin boundary conditions for quantifying fluctuations, is noteworthy. This shift is imperative for the consistency and predictability of the tunneling proposal, offering a fresh perspective on field fluctuation dynamics in the universe's early moments.

Future Outlook

This paper paves the way for future research to expand beyond perturbative models into non-perturbative domains with larger deviations from de Sitter geometry. There is potential for growth within the path integral approach, necessitating the inclusion of more degrees of freedom and admissible configurations in superspace. Therefore, a more comprehensive understanding of the universe's quantum birth could offer new insights into the early universe's structure and the origins of cosmic inflation.

Hence, further exploration and application of the tunneling wave function across broader cosmological models would enhance our comprehension of the universe's inception, the characteristics of preceding quantum states, and the embedded symmetries apparent in the initial conditions of cosmological models as put forth by quantum cosmology.

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