Studying the Neutral Intergalactic Medium Prior to the Epoch of
Reionization
Chris Carilli, Frazer Owen, (NRAO) & Nickolay Gnedin (U. of Colorado)
ABSTRACT
After recombining at z = 1000, the intergalactic medium (IGM) remains
largely neutral, and therefore opaque at wavelengths corresponding to
rest frame Ly alpha, until the formation of the first luminous
objects. The UV radiation from these first objects re-ionizes the
IGM, leading to the transparent IGM as seen today. Current
observations (principally the 'Gunn-Peterson' trough in a z = 6.3 QSO
and the strength of the first peak in the CMB spatial spectrum), place
the epoch of reionization in the range of z = 6.5 to 20. Simple
physical arguments, supported by detailed numerical calculations,
indicate that reionization is likely to occur in two phases: (i) a
slow phase during which each ionizing source is contained within its
own Stromgren sphere, and (ii) a fast phase when these spheres
overlap. The fast phase manifests itself as a 'cosmic phase
transition', when the mean neutral fraction, f, of the IGM goes from
f>=1% to f=1e-5 in a short redshift interval. At f>=1% the IGM is
opaque to the Ly alpha line, implying that there will be a substantial
redshift range, from the formation epoch of the first luminous objects
to the epoch of fast reionization, which will be largely opaque at
optical wavelengths. Hence the study of the first luminous objects in
the universe, and the neutral IGM, will be the responsibility of long
wavelength astronomy.
We will discuss methods for studying the neutral IGM during and prior
to the epoch of fast reionization using the HI 21cm line. Using the
latest numerical models for cosmic reionization, we will show that
future large area radio telescopes will reveal the detailed evolution
of the neutral IGM in a number of ways: (i) large scale structure
through observations of HI 21cm emission, and (ii) intermediate scale
structure (the 'HI 21cm Forest') and small scale structure
('minihalos') through absorption observations. These data will also
constrain the nature of the objects responsible for reionization: very
massive stars, star forming galaxies, or accreting massive black
holes.