Abstract
Quantized solutions of the Wheeler–DeWitt (WDW) equation describing a closed Friedmann–Robertson–Walker universe with a \(\Lambda \) term and a set of massless scalar fields are studied. It is shown that when \(\Lambda \ll 1\) units and the standard in-vacuum state is considered, the wave function of the universe \(\Psi \) behaves as a random quasiclassical field at rather large a, namely, \(1 \ll a \ll {{e}^{{\frac{2}{{3\Lambda }}}}}\) [1].
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ACKNOWLEDGMENTS
The work was supported by Grant NSh-6595.2016.2 of the President of the Russian Federation for Support of Leading Scientific Schools.
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Translated by M. Potapov
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Ivanov, P., Chernov, S.V. Third Quantization and Emergence of the Quasiclassical Wave Function of the Universe. Phys. Part. Nuclei 49, 514–519 (2018). https://doi.org/10.1134/S1063779618040299
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DOI: https://doi.org/10.1134/S1063779618040299