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Final Published Version
Author
Melia, FulvioAffiliation
University of Arizona, Department of Physics, Applied Math ProgramUniversity of Arizona, Department of Astronomy
Issue Date
2019-06
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SPRINGER BERLIN HEIDELBERGCitation
Melia, F. Eur. Phys. J. C (2019) 79: 455. https://doi.org/10.1140/epjc/s10052-019-6963-5Journal
EUROPEAN PHYSICAL JOURNAL CRights
© The Author(s) 2019; Open Access: this article is distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution, and reproduction in any medium, provided you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made.Collection Information
This item from the UA Faculty Publications collection is made available by the University of Arizona with support from the University of Arizona Libraries. If you have questions, please contact us at repository@u.library.arizona.edu.Abstract
The recently measured cutoff, kmin=4.34±0.50/rcmb (with rcmb the comoving distance to the last scattering surface), in the fluctuation spectrum of the cosmic microwave background, appears to disfavor slow-roll inflation and the associated transition of modes across the horizon. We show in this Letter that kmin instead corresponds to the first mode emerging out of the Planck domain into the semi-classical universe. The required scalar-field potential is exponential, though not inflationary, and satisfies the zero active mass condition, ρϕ+3pϕ=0. Quite revealingly, the observed amplitude of the temperature anisotropies requires the quantum fluctuations in ϕ to have classicalized at ∼3.5×1015 GeV, consistent with the energy scale in grand unified theories. Such scalar-field potentials are often associated with Kaluza–Klein cosmologies, string theory and even supergravity.Note
Open access articleISSN
1434-60441434-6052
Version
Final published versionAdditional Links
http://link.springer.com/10.1140/epjc/s10052-019-6963-5ae974a485f413a2113503eed53cd6c53
10.1140/epjc/s10052-019-6963-5