1999
DOI: 10.1103/physrevd.59.043510
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GUT cosmic magnetic fields in a warm inflationary universe

Abstract: Sources of magnetic fields from grand unified theories are studied in the warm inflation regime. A ferromagnetic Savvidy vacuum scenario is presented that yields observationally interesting large scale magnetic fields. As an intermediate step, a general analysis is made of defect production at the onset of warm inflation and monopole constraints are obtained. Many features of this Savvidy vacuum scenario are applicable within a supercooled inflation regime and these points are discuused.

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Cited by 29 publications
(29 citation statements)
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“…They also solved the full set of equations for linear fluctuations, including metric and entropy perturbations, in addition to the inflaton perturbations. Solving the Langevin equation gives 26) at the freezout scale, in agreement with the heuristic description above. However, a new effect can be seen when the friction coefficient depends on the temperature of the radiation.…”
Section: Fluctuationssupporting
confidence: 81%
“…They also solved the full set of equations for linear fluctuations, including metric and entropy perturbations, in addition to the inflaton perturbations. Solving the Langevin equation gives 26) at the freezout scale, in agreement with the heuristic description above. However, a new effect can be seen when the friction coefficient depends on the temperature of the radiation.…”
Section: Fluctuationssupporting
confidence: 81%
“…2 also can serve to damp kinetic energy contributions before inflation, thus alleviating the initial condition problem of inflation [41]. Warm inflation is also a conducive regime for the creation of large scale cosmic magnetic fields based on the ferromagnetic Savvidy vacuum scenario [42]. Also, spontaneous baryogenesis has been shown to work efficiently in the last stages of warm inflation [43].…”
Section: Resultsmentioning
confidence: 99%
“…Since we are interested mainly in the analysis of the behavior of this system in the early universe, for which the actual ponderable matter should be identified with a primordial ionized plasma 17,18,19 , we are led to limit our considerations here to the case in which only the average of the squared magnetic field H 2 survives e . 12,17,18,20 This is formally equivalent to put E 2 = 0 in (8). Let us see what the consequences of this result are.…”
Section: Quantum Corrections Of Qed At the Radiation Eramentioning
confidence: 99%