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Reynolds numbers in the early Universe
After electron-positron annihilation and prior to photon decoupling the magnetic Reynolds number is approximately twenty orders of magnitude larger than its kinetic counterpart which is, in turn, smaller than one. In this globally neutral system the large-scale inhomogeneities are provided by the sp...
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Lenguaje: | eng |
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2011
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Acceso en línea: | https://dx.doi.org/10.1016/j.physletb.2012.04.007 http://cds.cern.ch/record/1400110 |
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author | Giovannini, Massimo |
author_facet | Giovannini, Massimo |
author_sort | Giovannini, Massimo |
collection | CERN |
description | After electron-positron annihilation and prior to photon decoupling the magnetic Reynolds number is approximately twenty orders of magnitude larger than its kinetic counterpart which is, in turn, smaller than one. In this globally neutral system the large-scale inhomogeneities are provided by the spatial fluctuations of the scalar curvature. Owing to the analogy with the description of Markovian conducting fluids in the presence of acoustic fluctuations, the evolution equations of a putative magnetic field are averaged over the large-scale flow determined by curvature perturbations. General lessons are drawn on the typical diffusion scale of magnetic inhomogeneities. It is speculated that Reynolds numbers prior to electron-positron annihilation can be related to the entropy contained in the Hubble volume during the various stages of the evolution of the conducting plasma. |
id | cern-1400110 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2011 |
record_format | invenio |
spelling | cern-14001102023-03-14T16:56:51Zdoi:10.1016/j.physletb.2012.04.007http://cds.cern.ch/record/1400110engGiovannini, MassimoReynolds numbers in the early UniverseAstrophysics and AstronomyAfter electron-positron annihilation and prior to photon decoupling the magnetic Reynolds number is approximately twenty orders of magnitude larger than its kinetic counterpart which is, in turn, smaller than one. In this globally neutral system the large-scale inhomogeneities are provided by the spatial fluctuations of the scalar curvature. Owing to the analogy with the description of Markovian conducting fluids in the presence of acoustic fluctuations, the evolution equations of a putative magnetic field are averaged over the large-scale flow determined by curvature perturbations. General lessons are drawn on the typical diffusion scale of magnetic inhomogeneities. It is speculated that Reynolds numbers prior to electron-positron annihilation can be related to the entropy contained in the Hubble volume during the various stages of the evolution of the conducting plasma.After electron–positron annihilation and prior to photon decoupling the magnetic Reynolds number is approximately twenty orders of magnitude larger than its kinetic counterpart which is, in turn, smaller than one. In this globally neutral system the large-scale inhomogeneities are provided by the spatial fluctuations of the scalar curvature. Owing to the analogy with the description of Markovian conducting fluids in the presence of acoustic fluctuations, the evolution equations of a putative magnetic field are averaged over the large-scale flow determined by curvature perturbations. General lessons are drawn on the typical diffusion scale of magnetic inhomogeneities. It is speculated that Reynolds numbers prior to electron–positron annihilation can be related to the entropy contained in the Hubble volume during the various stages of the evolution of the conducting plasma.After electron-positron annihilation and prior to photon decoupling the magnetic Reynolds number is approximately twenty orders of magnitude larger than its kinetic counterpart which is, in turn, smaller than one. In this globally neutral system the large-scale inhomogeneities are provided by the spatial fluctuations of the scalar curvature. Owing to the analogy with the description of Markovian conducting fluids in the presence of acoustic fluctuations, the evolution equations of a putative magnetic field are averaged over the large-scale flow determined by curvature perturbations. General lessons are drawn on the typical diffusion scale of magnetic inhomogeneities. It is speculated that Reynolds numbers prior to electron-positron annihilation can be related to the entropy contained in the Hubble volume during the various stages of the evolution of the conducting plasma.arXiv:1111.3867CERN-PH-TH-2011-281CERN-PH-TH-2011-281oai:cds.cern.ch:14001102011-11-17 |
spellingShingle | Astrophysics and Astronomy Giovannini, Massimo Reynolds numbers in the early Universe |
title | Reynolds numbers in the early Universe |
title_full | Reynolds numbers in the early Universe |
title_fullStr | Reynolds numbers in the early Universe |
title_full_unstemmed | Reynolds numbers in the early Universe |
title_short | Reynolds numbers in the early Universe |
title_sort | reynolds numbers in the early universe |
topic | Astrophysics and Astronomy |
url | https://dx.doi.org/10.1016/j.physletb.2012.04.007 http://cds.cern.ch/record/1400110 |
work_keys_str_mv | AT giovanninimassimo reynoldsnumbersintheearlyuniverse |