2014/02/04 by Anastasia Fialkov, Rennan Barkana, Eli Visbal · 10 citations
Physics and Astronomy · #Astronomy #Astrophysics #Astrophysics and Cosmic Phenomena #COSMIC cancer database #Cosmic background radiation #Cosmic microwave background #Cosmic ray #Dark Ages #Galaxies: Formation, Evolution, Phenomena #Galaxy #Ion #Ionization #Optics #Photon #Physics #Radio Astronomy Observations and Technology #Redshift #Reionization #Spectral line #Universe #astro-ph.CO
paper · pdf · doi:10.1038/nature12999
25 pages, 5 figures, published in Nature on Feb. 5, 2014 (online), Feb. 13 (print)
openalex publication_date 2014/02/04 · arxiv created 2014/02/05 · arxiv updated 2015/06/18 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
Models and simulations of the epoch of reionization predict that spectra of the 21-cm transition of atomic hydrogen will show a clear fluctuation peak, at a redshift and scale, respectively, that mark the central stage of reionization and the characteristic size of ionized bubbles. This is based on the assumption that the cosmic gas was heated by stellar remnants - particularly X-ray binaries - to temperatures well above the cosmic microwave background at that time (~ 30 K). Here we show instead that the hard spectra (that is, spectra with more high-energy photons than low-energy photons) of X-ray binaries make such heating ineffective, resulting in a delayed and spatially uniform heating that modifies the 21-cm signature of reionization. Rather than looking for a simple rise and fall of the large-scale fluctuations (peaking at several millikelvin), we must expect a more complex signal also featuring a distinct minimum (at less than a millikelvin) that marks the rise of the cosmic mean gas temperature above the microwave background. Observing this signal, possibly with radio telescopes in operation today, will demonstrate the presence of a cosmic background of hard X-rays at that early time.