A. Fontana et al., High-redshift evolution of optical- and infrared-selected galaxies: a comparison with cold dark matter scenarios, M NOT R AST, 310(2), 1999, pp. L27-L32
A combination of ground-based (NTT and VLT) and Hubble Space Telescope (HST
) (HDF-N and HDF-S) public imaging surveys has been used to collect a sampl
e of 1712 I-selected and 319 K less than or equal to 21 galaxies observed w
ith an extended spectral coverage from U to K bands. Photometric redshifts
have been obtained for all these galaxies, using a spectral library compute
d from Bruzual & Charlot models. The results have been compared with the pr
ediction of an analytic rendition of the current cold dark matter (CDM) hie
rarchical models for galaxy formation that explicitly accounts for magnitud
e limits and dust extinction. We focus in particular on two observed quanti
ties: the galaxy redshift distribution at K less than or equal to 21 and th
e evolution of the UV luminosity density. The former has been proposed by K
auffmann & Charlot to be a very robust prediction of any CDM hierarchical m
odel, and we show that it is remarkably constant among different cosmologic
al models. The derived photometric redshift distribution is in agreement wi
th the hierarchical CDM prediction, with a fraction of only 5 per cent of g
alaxies detected at z greater than or equal to 2. This result strongly supp
orts hierarchical scenarios where present-day massive galaxies are the resu
lt of merging processes. The observed UV luminosity density in our I-select
ed sample is confined within a factor of 4 over the whole range 0 < z < 4.5
, in agreement with previous spectroscopic and photometric surveys. CDM mod
els in a critical (Omega = 1, Lambda = 0) Universe are not able to produce
the density of UV photons that is observed at z greater than or equal to 3.
CDM models in a Lambda-dominated universe are in better agreement at 3 les
s than or equal to z less than or equal to 4.5, but predict a pronounced pe
ak at z similar or equal to 1.5 and a drop by a factor of 8 from z = 1.5 to
z = 4 that is not observed in the data. We conclude that improvements are
required in the treatment of the physical processes directly related to the
star formation rate (SFR), e.g. the starburst activity in merger processes
and/or different recipes for linking the supernova feedback to the star fo
rmation activity.