Microwave Background Signatures of a Primordial Stochastic Magnetic Field
By A. Mack, T. Kahniashvili, A. Kosowsky. 2001
164 citations recorded by the source corpus.
A stochastic magnetic field in the early universe will produce anisotropies in the temperature and polarization of the cosmic microwave background. We derive analytic expressions for the microwave background temperature and polarization power spectra induced by vector and tensor perturbations from a power-law magnetic field. For a scale-invariant stochastic magnetic field smoothed over a comoving scale of 1 Mpc, the Microwave Anisotropy Probe satellite has the potential to constrain the comoving mean-field amplitude to be no greater than approximately $2\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}9} \mathrm{G}.$ Limits improve as the power-law slope increases: for causally generated power-law magnetic fields, the comoving mean-field amplitude has an upper bound of approximately $4\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}13} \mathrm{G}.$ Such constraints will surpass all current limits on galactic-scale primordial stochastic magnetic fields at decoupling.
Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics, Oceanography
View Paper: https://www.semanticscholar.org/paper/388bd6a60da7880725ea1e6ef2387e5d94f3f36b
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In Astronomy and Astrophysics
- D. Grasso
- Alberto Nicolis
- A. Dolgov
- C. Caprini
- G. Servant
- L. Senatore
- Claudia de Rham
- M. Zaldarriaga
In Nuclear and High Energy Physics
- D. Grasso
- Alberto Nicolis
- A. Dolgov
- C. Caprini
- G. Servant
- Claudia de Rham
- I. Sawicki
- Tsutomu Kobayashi
In Oceanography
Citations in the corpus
- Relic backgrounds of gravitational waves from cosmic turbulence (2002, background): “Furthermore magnetic fields may have produced observable effects on the CMB anisotropies [13, 14] and provided the seeds of galactic and intergalactic magnetic fields [10].”
- Planck 2015 results: XIX. Constraints on primordial magnetic fields (2015, unknown): “…over a comoving scale of λ = 1 Mpc, B2λ = ∫ ∞ 0 dk k2 2π2 e−k 2λ2 PB(k) = AB 4π2λnB+3 Γ ( nB + 3 2 ) · (2) For the damping scale we use (Subramanian & Barrow 1998a; Mack et al. 2002)4 kD = (5.5 × 104) 1 nB+5 ( Bλ nG )− 2nB+5 ( 2π λ/Mpc ) nB+3 nB+5 × h 1 nB+5 ( Ωbh2 0.022 ) 1 nB+5 ∣∣∣∣ λ= 1 Mpc…”