2018/06/04 by Ranita Jana, Biman B. Nath
Physics and Astronomy · #Astronomy #Astrophysics #Astrophysics and Cosmic Phenomena #Astrophysics and Star Formation Studies #Cosmic microwave background #Galaxies: Formation, Evolution, Phenomena #Galaxy #Galaxy formation and evolution #Intergalactic travel #Physics #Redshift #Reionization #Star formation #astro-ph.CO #astro-ph.GA
paper · pdf · doi:10.1093/mnras/sty1481
published as Mon.Not.R.Astron.Soc 479(2018) 153-161 · 10 pages, 9 figures, Accepted for publication in MNRAS
arxiv created 2018/06/04 · openalex publication_date 2018/06/06 · arxiv updated 2020/07/31 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
We study the heating of the intergalactic medium (IGM) surrounding high redshift star-forming galaxies due to cosmic rays (CR). We take into account the diffusion of low-energy CR and study the patchiness of the resulting heating. We discuss the case of IGM heating around a high redshift minihalo (|z| ∼ 10–20, M ∼ 105–107 M⊙) and put an upper limit on the diffusion coefficient D ≤ 1 × 1026 cm2 s−1 for the heating to be inhomogeneous at |z| ∼ 10 and D ≤ 5–6 × 1026 cm2 s−1 at |z| ∼ 20. For typical values of D, our results suggest uniform heating by CR at high redshift, although there are uncertainties in magnetic field and other CR parameters. We also discuss two cases with continuous star formation, one in which the star formation rate (SFR) of a galaxy is high enough to make the IGM in the vicinity photoionized, and another in which the SFR is low enough to keep it neutral but high enough to cause significant heating by CR protons. In the neutral case (low SFR), we find that the resulting heating can make the gas hotter than the cosmic microwave background radiation for D < 1030 cm2 s−1, within a few kpc of the galaxy, and unlikely to be probed by near future radio observations. In the case of photoionized IGM (high SFR), the resulting heating of the gas in the vicinity of high redshift (|z| ∼ 4) galaxies of mass ≥ 1012 M⊙ can suppress gas infall into the galaxy. At lower redshifts (|z| ∼ 0), an SFR of ∼1 M⊙ yr−1 can suppress the infall into galaxies of mass ≤1010 M⊙.