Observing Neutral Hydrogen Above Redshift 6: The "Global" Perspective
نویسندگان
چکیده
Above redshift 6, the dominant source of neutral hydrogen in the Universe shifts from localized clumps in and around galaxies and filaments to a pervasive, diffuse component of the intergalactic medium (IGM). This transition tracks the global neutral fraction of hydrogen in the IGM and can be studied, in principle, through the redshifted 21 cm hyperfine transition line. During the last half of the reionization epoch, the mean (global) brightness temperature of the redshifted 21 cm emission is proportional to the neutral fraction, but at earlier times (10 < z < 25), the mean brightness temperature should probe the spin temperature of neutral hydrogen in the IGM. Measuring the (of order 10 mK) mean brightness temperature of the redshifted 21 cm line as a function of frequency (and hence redshift) would chart the early evolution of galaxies through the heating and ionizing of the IGM by their stellar populations. Experiments are already underway to accomplish this task or, at least, provide basic constraints on the evolution of the mean brightness temperature. We provide a brief overview of one of these projects, the Experiment to the Detect the Global EOR Signature (EDGES), and discuss prospects for future results.
منابع مشابه
ar X iv : a st ro - p h / 05 01 08 6 v 2 1 0 Ja n 20 05 Redshifted 21 cm Emission From the Pre - Reionization Era II . H II Regions Around Individual
We use cosmological simulations of reionization to predict the effect of large H II regions around individual high-redshift quasars on the possible signal from the redshifted 21 cm line of neutral hydrogen in the pre-reionization era. We show that these H II regions appear as “spectral dips” in frequency space with equivalent widths in excess of 3mK MHz or depths in excess of about 1.5mK, and t...
متن کاملProbing the Dark Ages with Metal Absorption Lines
Recent observations of high redshift quasars at z ∼ 6 have finally revealed complete Gunn-Peterson absorption. However, this at best constrains the volume-weighted and mass-weighted neutral fractions to be x HI ≥ 10 and x HI ≥ 10 respectively; stronger constraints are not possible due to the high optical depth for hydrogen Lyman transitions. Here I suggest certain metal lines as tracers of the ...
متن کاملThe Extended Starformation History of the First Generation of Stars, and the Reionization of Cosmic Hydrogen
Population-III (Pop-III) starformation (SF) is thought to be quenched when the metallicity of the starforming gas has reached a critical level. At high redshift, when the general intergalactic medium (IGM) was enriched with metals, the fraction of primordial gas already collapsed in minihalos (above the Jeans mass but below the mass corresponding to the efficient atomic cooling threshold for SF...
متن کاملThe Mysterious Absence of Neutral Hydrogen within One Mpc of a Luminous Quasar at Redshift 2.168
The intense UV radiation from a highly luminous QSO should excite fluorescent Lyα emission from any nearby neutral hydrogen clouds. We present a very deep narrow-band search for such emission near the z=2.168 quasar PKS 0424-131, obtained with the Taurus Tunable Filter on the Anglo-Australian Telescope. By working in the UV, at high spectral resolution and by using charge shuffling, we have bee...
متن کاملDetecting the Earliest Galaxies through Two New Sources of 21cm Fluctuations
The first galaxies that formed at a redshift z ∼ 20–30 emitted continuum photons with energies between the Lyα and Lyman limit wavelengths of hydrogen, to which the neutral universe was transparent except at the Lyman-series resonances. As these photons redshifted or scattered into the Lyα resonance they coupled the spin temperature of the 21cm transition of hydrogen to the gas temperature, all...
متن کاملذخیره در منابع من
با ذخیره ی این منبع در منابع من، دسترسی به آن را برای استفاده های بعدی آسان تر کنید
عنوان ژورنال:
دوره شماره
صفحات -
تاریخ انتشار 2008