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Astron. Astrophys. 363, 517-525 (2000)
1. Introduction
Recent multi-waveband galaxy surveys, carried out from UV to radio
wavelengths, have identified a population of rapidly star forming
galaxies in the range (Sullivan et al
1999; Lilly et al. 1996; Cowie et al. 1997, Rowan-Robinson et al.
1997; Hughes et al. 1998; Mobasher et al. 1999). In particular, these
studies confirm a relatively higher rate of star formation in the
past, as supported by the discovery of a population of massive,
starforming galaxies at (Madau et al.
1996; Steidel et al. 1996). These objects are likely to be progenitors
of the present day galaxies (Giavalisco et al. 1996; Lowenthal et al.
1997) and hence, a statistical study of this population from the epoch
of galaxy formation to the present, gives clues towards scenarios of
the formation and evolution of galaxies (Fukugita et al. 1996). This
can also constrain the star formation history of galaxies out to
. Such studies require redshift
information for a population of starforming galaxies at faint levels.
Recently, the depth of the available surveys is greatly extended by
the Hubble Space Telescope (HST) observations of the Hubble Deep
Fields (HDF). The large spectral coverage of the HDFs provide a unique
opportunity to study evolutionary properties of faint galaxies.
Ground-based spectroscopic measurements of the brighter
( mag.) sub-sample of the HDF have
been performed (Cohen et al. 2000; Steidel et al. 1996; Lowenthal et
al. 1997; Zepf et al. 1996). However, for the fainter galaxies in the
HDF, redshift measurements are more difficult with spectroscopic
features almost impossible to identify. For these objects, the
photometric redshift technique (Loh & Spillar 1986; Connolly et
al. 1995) is faster than its spectroscopic counterpart and applicable
to much fainter magnitudes. This is due to a larger bin size in
photometry compared to spectroscopy (
Å Å), leading to a shorter
exposure time with a trade-off in accuracy of the measured
redshifts.
Considering the new generation of 8m class telescopes, the planned
instrumentation on the HST and future, high sensitive radio
telescopes, a substantial number of deep surveys at different
wavelengths will soon become available. Most of these galaxies will be
too faint for spectroscopic study and hence, the photometric redshift
technique is the only practical way for estimating their redshifts. In
a recent assessment of different photometric redshift techniques,
using a redshift-limited spectroscopic survey, it was shown that
photometric redshifts can be predicted with an accuracy of 0.1 (0.3)
for
( ) of the sources examined (Hogg et
al. 1998). Therefore, photometric redshifts could provide a powerful
tool for statistical studies of evolutionary properties of
galaxies and in particular of faint galaxies for which spectroscopic
data are difficult to obtain.
The most important step in any study concerning photometric
redshift measurement, is the choice of the template Spectral Energy
Distributions (SEDs) for different populations of galaxies, with which
the observed SEDs should be compared. There are two general ways for
adopting the template SEDs:
-
a) Empirical templates: in this case one uses the mean
observed SEDs corresponding to different types of galaxies. The
problem here is that there are not enough information about the
observed SEDs for different classes of objects at different redshifts
(particularly at high redshifts). Therefore, incorporating the
spectral evolution of galaxies of different types on their template
SEDs is difficult and uncertain.
-
b) Synthetic templates: uses model SEDs for different spectral
types of galaxies, shifted in redshift space, assuming evolutionary
population synthesis models. The main problem here is to constrain the
evolutionary model parameters to produce realistic model SEDs (for
different types) as a function of redshift. In particular, the effect
of dust at high redshifts (specially in star forming galaxies) is not
known.
To avoid these problems, we introduce a combined approach,
producing realistic model SEDs based on chemo-photometric Evolutionary
Population Synthesis (EPS) models, extending from UV to 1 mm in
wavelength. The template SEDs here, are consistently and
simultaneously optimised to; a) produce the observed colours of
galaxies at ; b) incorporate
chemo-photometric evolution for galaxies of different types, in
agreement with observations; c) allow treatment of dust contribution
and its evolution with redshift, consistent with the EPS models; d)
include absorption and re-emission of radiation by dust and hence,
realistic estimates of the far-infrared radiation; e) include
correction for inter-galactic absorption by Lyman continuum and Lyman
forest. The evolutionary models and hence, the template SEDs, are
constrained by minimising the scatter between the photometric and
spectroscopic redshifts for a calibrating sample of galaxies with
known spectroscopic data .
The main advantage of this technique over the previous works is
that it simultaneously and self-consistently allows for the treatment
of both the photometric and chemical evolution of individual galaxies
with time. Moreover, since the synthetic template SEDs cover the range
from UV to sub-mm wavelengths, one could consistently use the
optimised SEDs to estimate contributions from individual galaxies to
the far-infrared and sub-mm wavelengths. Also, the effect of dust and
its evolution with redshift is self-consistently accounted for in the
template SEDs and optimised to produce the observations. This is
crucial in any photometric redshift technique if it is to be applied
on high redshift, star-forming galaxies (Meurer et al. 1997; Cimatti
et al. 1998).
The new photometric redshift technique is outlined in the next
section. In Sect. 3, the EPS models are briefly discussed.
Sect. 4 presents the calibration sample. This is followed by the
optimised template SEDs in Sect. 5. The uncertainties in the
photometric redshifts and spectral types are explored in Sect. 6.
The conclusions are presented in Sect. 7.
© European Southern Observatory (ESO) 2000
Online publication: December 11, 2000
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