
Galaxy number counts – V. Ultradeep counts: the Herschel and Hubble Deep Fields
Author(s) -
Metcalfe N.,
Shanks T.,
Campos A.,
McCracken H. J.,
Fong R.
Publication year - 2001
Publication title -
monthly notices of the royal astronomical society
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 2.058
H-Index - 383
eISSN - 1365-2966
pISSN - 0035-8711
DOI - 10.1046/j.1365-8711.2001.04168.x
Subject(s) - physics , astrophysics , galaxy , astronomy , luminosity function , dwarf galaxy , galaxy formation and evolution , luminous infrared galaxy , lenticular galaxy , elliptical galaxy , hubble deep field , hubble ultra deep field , galaxy group , spiral galaxy , luminosity , hubble space telescope
We present u , b , r and i galaxy number counts and colours from both the North and South Hubble Space Telescope Deep Fields and the William Herschel Deep Field. The latter comprises a 7×7 arcmin 2 area of sky, reaching b∼28.5 at its deepest. Following Metcalfe et al., we show that simple Bruzual & Charlot evolutionary models which assume exponentially increasing star formation rates with look‐back time and q 0 =0.05 continue to give excellent fits to galaxy counts and colours in the deep imaging data. With q 0 =0.5, an extra population of ‘disappearing dwarf’ galaxies is required to fit the optical counts. We further find that the (r−i):(b−r) colour–colour diagrams show distinctive features corresponding to two populations of early‐ and late‐type galaxies which are well fitted by features in the Bruzual & Charlot models. The (r−i):(b−r) data also suggest the existence of an intrinsically faint population of early‐types at z∼0.1 with similar properties to the ‘disappearing dwarf’ population required if q 0 =0.5. The outstanding issue remaining for the early‐type models is the dwarf‐dominated initial mass function (IMF), which we invoke to reduce the numbers of z>1 galaxies predicted at K<19. For the spiral models, the main issue is that even with the inclusion of internal dust absorption at the A B =0.3 mag level, the model predicts too blue (u−b) colours for late‐type galaxies at z∼1. Despite these possible problems, we conclude that these simple models with monotonically increasing star formation rates broadly fit the data out to z∼3. We compare these results for the star formation rate history with those from the different approach of Madau et al. We conclude that when the effects of internal dust absorption in spirals are taken into account the results from this latter approach are completely consistent with the τ=9 Gyr, exponentially rising star formation rate density out to z≈3 which fits the deepest, optical/IR galaxy count and colour data. When we compare the observed and predicted galaxy counts for UV dropouts in the range 2≲z≲3.5 from the data of Steidel et al. and Madau et al., and new data from the Herschel and HDF‐S fields, we find excellent agreement, indicating that the space density of galaxies may not have changed much between z=0 and z=3, and identifying the Lyman‐break galaxies with the bright end of the evolved spiral luminosity function. Making the same comparison for B dropout galaxies in the range 3.5≲z≲4.5 we find that the space density of intrinsically bright galaxies remains the same, but the space density of faint galaxies drops by a factor of ∼5, consistent with the idea that L* galaxies were already in place at z≈4 but that dwarf galaxies may have formed later at 3≲z≲4.