The observed ionization rate of the intergalactic medium and the ionizing emissivity at z ≥ 5: Evidence for a photon starved and extended epoch of reionization
نویسندگان
چکیده
Galaxies and quasars are thought to provide the bulk of the photons responsible for ionizing the hydrogen in the intergalactic medium (IGM). We use a large set of hydrodynamical simulations, combined with measurements of the Lyα opacity of the IGM taken from the literature, to obtain robust estimates of the photoionization rate per hydrogen atom at z = 5 and 6. We find the photoionization rate drops by a factor of two and four, respectively, compared to our recent measurements at z = 2− 4. The number of ionizing photons emitted by known sources at z = 5 and 6, based on a moderate extrapolation of source numbers below the detection limit and standard assumptions for the relationship between the ionizing emissivity and observed luminosity density at 1500Å, are in reasonable agreement with the photoionization rates inferred from the Lyα forest if the escape fraction of ionizing photons is large (>∼ 20 per cent). The expected number of ionizing photons from observed sources at these redshifts therefore appears sufficient to maintain the IGM in its highly ionized state. Claims to the contrary may be attributed to the adoption of an unduly high value for the clumping factor of ionized hydrogen. Using physically motivated assumptions for the mean free path of ionizing photons our measurements of the photoionization rate can be turned into an estimate of the ionizing emissivity. In comoving units the inferred ionizing emissivity is nearly constant over the redshift range 2 − 6 and corresponds to 1.5 − 3 photons emitted per hydrogen atom over a time interval corresponding to the age of the Universe at z = 6. This strongly suggests that the epoch of reionization was photon-starved and extended. Completion of reionization at or before z = 6 requires either an emissivity which rises towards higher redshifts or one which remains constant but is dominated by sources with a rather hard spectral index. For standard assumptions, the ionizing emissivity required for completion of reionization at or before z = 6 lies at the upper end of recently reported values from searches for high redshift galaxies at z = 8− 10.
منابع مشابه
History of Hydrogen Reionization in the Cold Dark Matter Model
We calculate the reionization history in Cold Dark Matter (CDM) models. The epoch of the end of reionization and the Thomson scattering optical depth to the cosmic microwave background depend on the power spectrum amplitude on small scales and on the ionizing photon emissivity per unit mass in collapsed halos. We calibrate the emissivity to reproduce the measured ionizing background intensity a...
متن کاملOn the evolution of the ionizing emissivity of galaxies and quasars required by the hydrogen reionization
The average rate of emission of ionizing radiation per unit volume (or emissivity) in the universe can be calculated as the ratio of the intensity of the ionizing background to the mean free path of ionizing photons. The intensity of the background is measured from the mean transmitted flux of the Lyα forest, and the mean free path is measured from the abundance of Lyman limit systems, which ha...
متن کاملOptical Depth of the Cosmic Microwave Background and Reionization of the Intergalactic Medium
We examine the constraints on the epoch of reionization (redshift zr) set by recent WMAP-3 observations of τe = 0.09 ± 0.03, the electron-scattering optical depth of the cosmic microwave background (CMB), combined with models of highredshift galaxy and black hole formation. Standard interpretation begins with the computed optical depth, τe = 0.042± 0.003, for a fully ionized medium out to zr = ...
متن کاملThe Impact of Small-scale Structure on Cosmological Ionization Fronts and Reionization
The propagation of cosmological ionization fronts during the reionization of the universe is strongly influenced by small-scale gas inhomogeneities due to structure formation. These inhomogeneities include both collapsed minihalos, which are generally self-shielding, and lower-density structures, which are not. The minihalos are dense and sufficiently optically-thick to trap intergalactic ioniz...
متن کاملConstraints on First-Light Ionizing Sources from Optical Depth of the Cosmic Microwave Background
We examine the constraints on high-redshift star formation, ultraviolet and X-ray preionization, and the epoch of reionization at redshift zr, inferred from the recent WMAP-5 measurement, e 1⁄4 0:084 0:016, of the electronscattering optical depth of the cosmic microwave background (CMB). Half of this scattering can be accounted for by the optical depth, e 1⁄4 0:04Y0.05, of a fully ionized inter...
متن کامل