Challenges in Inflationary Magnetogenesis: Constraints from Strong Coupling, Backreaction and the Schwinger Effect
| Autor: | Sandhya Jagannathan, R. Sharma, Kandaswamy Subramanian, T. R. Seshadri |
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| Rok vydání: | 2017 |
| Předmět: |
Quantum chromodynamics
Inflation (cosmology) Physics Cosmology and Nongalactic Astrophysics (astro-ph.CO) 010308 nuclear & particles physics Spectrum (functional analysis) Inverse FOS: Physical sciences Function (mathematics) Astrophysics::Cosmology and Extragalactic Astrophysics Coupling (probability) 01 natural sciences Coherence length Magnetic field General Relativity and Quantum Cosmology Quantum mechanics 0103 physical sciences 010303 astronomy & astrophysics Mathematical physics Astrophysics - Cosmology and Nongalactic Astrophysics |
| DOI: | 10.48550/arxiv.1708.08119 |
| Popis: | Models of inflationary magnetogenesis with a coupling to the electromagnetic action of the form $f^2 F_{\mu\nu}F^{\mu\nu}$, are known to suffer from several problems. These include the strong coupling problem, the back reaction problem and also strong constraints due to Schwinger effect. We propose a model which resolves all these issues. In our model, the coupling function, $f$, grows during inflation and transits to a decaying phase post inflation. This evolutionary behaviour is chosen so as to avoid the problem of strong coupling. By assuming a suitable power law form of the coupling function, we can also neglect back reaction effects during inflation. To avoid back reaction post-inflation, we find that the reheating temperature is restricted to be below $ \approx 1.7 \times 10^4$ GeV. The magnetic energy spectrum is predicted to be non-helical and generically blue. The estimated present day magnetic field strength and the corresponding coherence length taking reheating at the QCD epoch(150 MeV) are $ 1.4 \times 10^{-12}$ G and $6.1 \times 10^{-4}$ Mpc, respectively. This is obtained after taking account of nonlinear processing over and above the flux freezing evolution after reheating. If we consider also the possibility of a non-helical inverse cascade, as indicated in direct numerical simulations, the coherence length and the magnetic field strength are even larger. In all cases mentioned above, the magnetic fields generated in our models satisfy the $\gamma$-ray bound below a certain reheating temperature. Comment: 13 pages, 4 figures, Published in PRD |
| Databáze: | OpenAIRE |
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