15 micron Infrared Space Observatory observations of the 1415+52 Canada-France Redshift Survey field: The cosmic star formation rate as derived from deep ultraviolet, optical, mid-infrared, and radio photometry
H. Flores et al., 15 micron Infrared Space Observatory observations of the 1415+52 Canada-France Redshift Survey field: The cosmic star formation rate as derived from deep ultraviolet, optical, mid-infrared, and radio photometry, ASTROPHYS J, 517(1), 1999, pp. 148-167
The Canada-France Redshift Survey 1452+52 field has been deeply imaged with
the Infrared Space Observatory using ISOCAM through the LW3 filter (12-18
mu m). Careful data analysis and comparison with deep optical and radio dat
a have allowed us to generate a catalog of 78 15 mu m sources with both rad
io and optical identifications. They are redder and lie at higher redshift
than I-band selected galaxies, with most of them being star-forming galaxie
s. We have considered the galaxies detected at radio and 15 mu m wavelength
s, which potentially include all strong and heavily extincted starbursts, u
p to z = 1. Spectral energy distributions (SEDs) for each of the sources ha
ve been derived using deep radio, mid-IR, near-IR, optical, and UV photomet
ry. The sources were then spectrally classified by comparing with SEDs of w
ell-known nearby galaxies. By deriving their far-IR luminosities by interpo
lation, we can estimate their star formation rate (SFR) in a way that does
not depend sensitively on the extinction. Between 35% and 85% of the star f
ormation at z I 1 is related to IR emission, and the global extinction is i
n the range A(v) = 0.5-0.85. While heavily extincted starbursts with SFRs i
n excess of 100 M. yr(-1) constitute less than 1% of all galaxies, they con
tribute about 18% of the SFR density out to z = 1. Their morphologies range
from S0 to Sab, and more than a third are interacting systems. The SFR der
ived by far-IR fluxes is likely to be similar to 2.9 times higher than thos
e previously estimated from UV fluxes. The derived stellar mass formed sinc
e the redshift of 1 could be too high when compared with the present-day st
ellar mass density. This might be due to an initial mass function in distan
t star-forming galaxies different from the solar neighborhood one or an und
erestimate of the local stellar mass density.