Table 2: Main characteristics of the datasets in HDFN. Column (1): observing band. Column (2): effective wavelength of the filter calculated by convolving the Vega spectrum (Colina & Bohlin 1994) with the transmission curve of the filter + detector. Column (3): limiting AB magnitude. Column (4): source from where the data were obtained.
Band $\lambda_{\rm eff}(\mu {\rm m})$ $m_{\lim}$ Source
(1) (2) (3) (4)
IRAC-3.6.. 3.561 21.6 Spitzer GTO
IRAC-4.5.. 4.510 21.8 Spitzer GTO
IRAC-5.8.. 5.689 21.8 Spitzer GTO
IRAC-8.0.. 7.958 21.7 Spitzer GTO
U......... 0.358 25.2 Subaru deep imaginga
B......... 0.442 25.2 Subaru deep imaginga
V......... 0.546 24.9 Subaru deep imaginga
R......... 0.652 24.4 Subaru deep imaginga
I......... 0.795 23.9 Subaru deep imaginga
z......... 0.909 23.6 Subaru deep imaginga
b......... 0.430 25.7 GOODSb
v......... 0.592 24.9 GOODSb
i......... 0.770 24.3 GOODSb
z......... 0.906 23.9 GOODSb
$HK_{\rm s}$ .. 2.127 21.3 QUIRC deep imaginga
b, spectra.. 0.430 24.4 TKRSc
a Publicly available ultra-deep optical and NIR data from Capak et al. (2004); b the Great Observatories Origins Deep Survey (GOODS; Giavalisco et al. (2004); c team Keck Treasury Redshift Survey (TKRS; Wirth et al. 2004) and Cowie et al. (2004).

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