A&A 428, 1043-1049 (2004)
DOI: 10.1051/0004-6361:20048072
O. Le Fèvre1 - G. Vettolani2 - S. Paltani1 - L. Tresse 1 - G. Zamorani 5 - V. Le Brun1 - C. Moreau1 - D. Bottini3 - D. Maccagni3 - J. P. Picat4 - R. Scaramella2 - M. Scodeggio3 - A. Zanichelli2 - C. Adami1 - S. Arnouts1 - S. Bardelli5 - M. Bolzonella6 - A. Cappi5 - S. Charlot7,10 - T. Contini4 - S. Foucaud3 - P. Franzetti3 - B. Garilli3 - I. Gavignaud4,11 - L. Guzzo8 - O. Ilbert1 - A. Iovino8 - H. J. McCracken7,12 - D. Mancini9 - B. Marano6 - C. Marinoni1 - G. Mathez4 - A. Mazure1 - B. Meneux1 - R. Merighi5 - R. Pellò4 - A. Pollo8 - L. Pozzetti5 - M. Radovich9 - E. Zucca 5 - M. Arnaboldi9 - M. Bondi2 - A. Bongiorno6 - G. Busarello9 - P. Ciliegi5 - L. Gregorini2 - Y. Mellier7,12 - P. Merluzzi9 - V. Ripepi9 - D. Rizzo4
1 - Laboratoire d'Astrophysique de Marseille - UMR 6110, OAMP, Université de
Provence, Traverse du Siphon-Les trois Lucs, BP 8, 13376 Marseille
Cedex 12, France
2 -
IRA-INAF, via Gobetti 101, 40129 Bologna, Italy
3 -
IASF-INAF, via Bassini 15, 20133 Milano, Italy
4 -
Laboratoire d'Astrophysique de l'Observatoire Midi-Pyrénées - UMR 5572,
14 avenue E. Belin, 31400 Toulouse, France
5 -
INAF - Osservatorio Astronomico di Bologna, via Ranzani 1, 40127 Bologna,
Italy
6 -
Università di Bologna, Dipartimento di Astronomia, via Ranzani 1,
40127 Bologna, Italy
7 -
Institut d'Astrophysique de Paris - UMR 7095, 98bis bd Arago, 75014 Paris,
France
8 -
INAF - Osservatorio Astronomico di Brera, via Brera 28, 20121 Milano, Italy
9 -
INAF - Osservatorio Astronomico di Capodimonte, Salita Moiariello 16, 80131
Napoli, Italy
10 -
Max Planck Institut für Astrophysik, Karl-Schwarzschild-Strasse 1, 85741
Garching, Germany
11 -
European Southern Observatory, Karl-Schwarzschild-Strasse 2, 85748
Garching, Germany
12 -
Observatoire de Paris, LERMA - UMR 8112, 61 avenue de l'Observatoire,
75014 Paris, France
Received 10 April 2004 / Accepted 6 August 2004
Abstract
This paper presents the VIMOS VLT Deep Survey
around the Chandra Deep Field South (CDFS). We have measured
1599 new redshifts with VIMOS on the European Observatory
Very Large Telescope - UT3,
in an area
arcmin2, including 784
redshifts in the Hubble Space Telescope - Advanced Camera
for Surveys GOODS area. 30% of all objects with IAB=24 have been observed independently of magnitude, indicating
that the sample is purely
magnitude limited. We have reached
an unprecedented completeness level of 84% in terms of
the ratio of secure measurements vs. observed objects,
while 95% of all objects have a redshift measurement.
A total of 1452 galaxies, 139 stars, 8 QSOs have a
redshift identification, 141 of these being unsecure
measurements. The redshift distribution down to IAB=24is peaked at a median redshift z=0.73, with a significant
high redshift tail extending up to
4. Several high
density peaks in the distribution of galaxies are
identified. In particular, the strong peak at z=0.735
contains more than 130 galaxies in a velocity range
km s-1 distributed all across the transverse
20 h-1 Mpc of the survey. We are releasing all redshifts
to the community, along with the cross identification
with HST-ACS GOODS sources on the CENCOS database environment
http://cencosw.oamp.fr.
Key words: surveys - galaxies: high-redshift - galaxies: distances and redshifts - cosmology: observations - galaxies: evolution - cosmology: large scale structure of Universe
Understanding the major steps in the evolution of galaxies still remains a major challenge to modern astrophysics. While the general theoretical framework of the hierarchical growth of structures in the universe including the build up of galaxies is well in place (e.g. Peacock et al. 2004), at high redshifts this picture remains largely unconstrained by observations. The detailed properties of the main population of galaxies from large samples representative of the universe at various epochs remain to be established across most of the life of the universe beyond the large local volumes explored by the 2dFGRS (Colless et al. 2001) and the SDSS (Schneider et al. 2003), and expanding from smaller exploratory surveys (Lilly et al. 1995; Le Fèvre et al. 1995; Steidel et al. 2003; Cimatti et al. 2002).
The VIMOS VLT Deep Survey (VVDS) is a deep redshift survey aimed at studying the evolution of galaxies, large scale structures and AGNs over more than 90% of the current age of the universe. The unique feature of the VVDS is the simple magnitude selection applied to define a complete magnitude limited sample of distant galaxies, with a goal of more than 100 000 objects observed in multi-object spectroscopy. The VVDS rests on the observations of 5 different fields to smooth out the effects of cosmic variance when building the statistical properties of the galaxy population (Le Fèvre et al. 2004).
This paper presents the redshift survey observations of 1599
objects with
conducted by the VVDS team around the Chandra Deep Field South
(CDFS). The CDFS is field particularly
rich of deep observations, starting from 1 Ms Chandra observations
(Giacconi et al. 2002), including the HST-GOODS area (Giavalisco et al. 2004), as well as optical
spectroscopy (Szokoly et al. 2003). The observations have been carried out
with the VIsible Multi-Object Spectrograph (VIMOS) on the 8.2 m
Melipal telescope of the European Southern Observatory
Very Large Telescope. We are describing the processing
steps and redshift measurements, and the associated quality
control we have applied to these data. The content of the final
catalog is detailed, as well as the cross identification
with the Hubble Space Telescope Advanced Camera for Surveys GOODS
images, and we present
the main entries available from our interactive database.
The main properties of the sample are briefly
presented, including the redshift distribution of the sample.
Spectroscopic observations have been conducted with
VIMOS on the VLT-UT3 Melipal (Le Fèvre et al. 2003).
The low resolution red grism LRRED has been used with slits
of 1 arcsec width. The spectral resolution in this mode
is 34 Å at 7500 Å or
.
The spectral length
has been limited by the red bandpass filter to 5500-9500 Å.
Slits placed on objects have a typical length
10 arcsec each.
A complete VIMOS pointing is a combination of observations
with the 4 quadrants of the instrument, each separated by a
cross about 2 arcmin wide. With the above setup and the
projected sky density of objects down to IAB=24,
one VIMOS pointing allows to observe
450 targets
in one single observation (Le Fèvre et al. 2003).
We have set a total of 5 pointings around the
Chandra Deep Field South, the positions are listed
in Table 1. Together, they cover a total area
of
453
including the complete HST-GOODS survey
field (Giavalisco et al. 2004).
The layout of observed galaxies is presented in
Fig. 1.
Table 1: Observed VIMOS pointings.
![]() |
Figure 1: Objects observed with VIMOS-VLT around the Chandra Deep Field South. Black circles are objects in the HST-ACS GOODS area. |
| Open with DEXTER | |
The preparation of slit masks for VIMOS observations has been done using the photometric catalog produced by the ESO Imaging Survey (EIS, Arnouts et al. 2001), and short images taken with VIMOS. The VIMOS images are used to produce a catalog of source positions in the VIMOS instrument coordinate system, which are then cross-correlated with the EIS catalog to compute the transformation matrix from the EIS catalog astrometric system to the VIMOS focal plane where slit masks are located. The VMMPS code was then run on the EIS catalog for all sources brighter than IAB=24 to optimize the number and positions of slits for each of the 4 masks per pointing. Masks have been cut by ESO Paranal Staff using the Mask Manufacturing Unit (Conti et al. 2001).
Observations with VIMOS have been obtained between October 31 and December 6, 2002. Observing conditions were photometric with an image quality between 0.6 and 1.2 arcsec FWHM. We have moved the telescope, hence the objects along the slits, in a sequence of 5 positions with offsets -1.4, -0.7, 0, +0.7, +1.4 arcsec from the reference pointing position. This is necessary to compute the fringing pattern produced above 8300 Å by the thinned EEV CCDs used in VIMOS, and remove it during processing.
Wavelength calibrations have been obtained during the day, observing Helium and Argon arc lamps through the observed masks. The spectrophotometric standard star LTT3218 has been used to derive the absolute flux calibration.
Data processing has been conducted under the VIPGI environment
developed by our team (Franzetti et al. 2004). VIPGI has been
used to organize the multiple files and process all data
from the raw 2D images and calibration to the production
of sky subtracted, wavelength and flux calibrated 1D spectra.
Because of instrument flexures not yet minimized at the time
of these observations, the fringing pattern has been occasionally
hard to remove. The quality control performed on these steps
is described in Le Fèvre et al. (2004). The wavelength accuracy is
better than
1 Å rms all over the wavelength range,
and the spectrophotometry is accurate to about 10%.
Measuring redshifts for a complete magnitude limited sample
down to IAB=24 had never been attempted before our
observations. The challenge is to measure redshifts
over a large possible range
5, without any other
a priori information than the magnitude selection. The approach we have followed
involves an iterative build up of galaxy templates
as observed with VIMOS, coupled to the powerful redshift measuring
machine KBRED (Scaramella et al. 2004), based on cross correlation
and principal component analysis methods. This approach has
been applied and tuned on the more than 20 000 spectra obtained
for the VVDS in the fall of 2002, and remained until recently
very manpower intensive. On this critical step, we have
enforced a very strict quality control.
Each spectrum has been measured independently
by 2 VVDS team members, and then compared. A final check
has been done by a third team member prior to
release into the database.
Each spectrum is assigned a redshift, and a flag indicating
the reliability level of the measurement, as defined in Le Fèvre et al. (1995)
and described in Sect. 6.
Flags 2, 3, 4 are the most secure,
flag 1 is an indicative measurement based on
continuum and few supporting features,
and flag 0
indicates a measurement failure with no features identified.
Flag 9 indicates
that there is only one secure emission line tentatively
assigned to the listed redshift (e.g. [OII]3727 Å or
H
).
![]() |
Figure 2:
Redshift difference between objects observed
twice or more in independent VIMOS observations. The
distribution has a velocity dispersion
|
| Open with DEXTER | |
The redshift accuracy can be estimated from a sample
of 160 galaxies which have been observed twice with
VIMOS within the 5 CDFS pointings.
These galaxies have been included in two
or more different mask sets, and observed
independently at different times. The distribution
of measured redshift differences is presented in
Fig. 2. The dispersion of the redshift
difference distribution is
,
or 360 km s-1, hence the accuracy of
a single redshift measurement is
km s-1.
We have compared our redshift measurements with the
measurements of the K20 survey (Cimatti et al. 2002)
and VLT-FORS2 measurements conducted by the ESO-GOODS team
(www.eso.org/science/goods). A total of 70 objects
have been observed both by the VVDS and the K20.
For the 63 VVDS objects with flags
,
the redshifts agree for
87% of the sample
with a
and
,
with the main disagreement concentrated on flag 1,
as expected. The comparison with the ESO-GOODS data
yields 46 objects in common, of which 42 have
a VVDS flag
1. The VVDS vs. ESO-GOODS redshift
agree for 66% of the sample with
and
.
There are 48 objects in common
between our observation an the observations of
X-ray sources by Szokoly et al. (2003), and our redshifts agree
on 85% of this special class of objects (Hasinger, private communication).
The detailed comparison of VVDS redshift measurements with
the measurements from these other teams will be presented in Le Fèvre et al. (2004)
.
![]() |
Figure 3:
Completeness of the
|
| Open with DEXTER | |
![]() |
Figure 4: ( Top panel) IAB magnitude distribution of objects observed with VIMOS in the Chandra Deep Field South (filled histogram), compared to the distribution of all objects in the area in the EIS photometric catalog (open histogram). ( Bottom panel) The ratio of observed vs. all objects is 0.3. |
| Open with DEXTER | |
We have defined the completeness of the measurements as the ratio between the actual redshifts measurements and the observed spectra. We have removed from the list of observed spectra those which have a clearly identified instrumental or data processing problem affecting the measurement, like e.g. the slit is behind the guide probe of the VLT-UT3, or the data processing with VIPGI failed to properly detect the object because of strong residual features from the sky/fringing corrections. This will be described in details in Le Fèvre et al. (2004).
We are presenting in Fig. 3 the completeness in redshift measurement vs. IAB magnitude for all objects (galaxies, stars, QSOs), and the magnitude distribution of objects with flags 0, 1, 2, 3, 4, 9. The completness is computed taking into account the fraction of objects with a good redshift measurement for each of our quality flags listed in Sect. 7 (see Le Fèvre et al. 2004 for a detailed discussion on completness).
The overall redshift measurement completeness reaches 84%. The objects with a redshift measurement listed in the catalogs, flags 1, 2, 3, 4, 9, 11, 12, 13, 14, 19, represent 95% of the sample, excluding objects with flags 0.
The cross identification of the objects observed from the EIS catalog and the objects detected by HST-ACS has been performed running a cross correlation of our target list with the list of objects published in the version r1.0, December 22, 2003, of the GOODS survey multi-band catalog. The relative astrometry of the EIS vs. GOODS catalogs has been found to be extremely good, to within 0.1 arcsec over our survey field. A search circle with radius 0.3 arcsec has been used to search for HST sources corresponding to the ground based sources. This produced a matched list with only one to one identifications, and no double identifications.
The magnitude distribution of objects observed in
our survey is shown in Fig. 4
compared to the distribution of all objects
in the EIS photometric catalog over the
same area.
We have observed 30% of all objects with
in the
area covered by the survey, independently
of magnitude, as shown in
Fig. 4.
This demonstrates that there is no
magnitude - dependent bias in our object selection and
that our sample is purely magnitude selected
even after the complex target selection in
the making of the VIMOS multi-slit masks.
The redshift distribution (up to z=2) of the full sample of
galaxies and QSOs
is presented in Fig. 5. The median of the redshift
distribution is
.
Galaxies are identified up to
z=4.63. As described in Le Fèvre et al. (2004) and Paltani et al. 2004,
we have been successful in breaking into the
"redshift desert'' artificially produced by the
difficulty to identify redshifts in the range
due to our instrumental set-up, through
extensive work on galaxy templates based on
the high redshift galaxies measured in the VVDS
(Paltani et al. 2004).
We extensively discuss the incompleteness of
the VVDS sample vs. redshift in Le Fèvre et al. (2004).
The strongest peaks in the
distribution are at redshifts
z=0.667, and z=0.735, confirming with better statistics the observations of Gilli et al. (2003). A total of 149 galaxies are measured
in the z=0.667 peak and 116 galaxies z=0.735 peak.
These structures are extending all
across transverse
16 Mpc of this survey
(
CDM with H0=70,
,
)
in a wall-like pattern rather than in clusters.
These peaks are also traced by X-ray sources as discussed
by Szokoly et al. (2003).
![]() |
Figure 5:
Redshift distribution of galaxies
with
|
| Open with DEXTER | |
The absolute magnitude MB vs. redshift distribution is presented in Fig. 6. The absolute magnitudes have been computed based on k(z) corrections derived from the fitting of the broad band photometry using rest frame galaxy templates (see Ilbert et al. 2004). The BAB-IAB vs. redshift distribution is presented in Fig. 7
![]() |
Figure 6: Absolute MBAB magnitude - redshift distribution for the full VVDS-CDFS sample |
| Open with DEXTER | |
![]() |
Figure 7: BAB-IAB vs. redshift distribution for the full VVDS-CDFS sample |
| Open with DEXTER | |
![]() |
Figure 8: Output from the VVDS-CDFS CENCOS database output panel for one single object. All information is presented, including the EIS and HST-GOODS identifiers, the ground based and HST-ACS magnitudes, the VVDS redshift and quality flag, and the HST-GOODS images and VVDS spectrum are displayed. |
| Open with DEXTER | |
Our catalog contains 1599 spectra including 1452 galaxies, 139 stars, and 8 QSOs. We have listed for each observed object:
We are publicly releasing all redshift measurements through the CENCOS (CENtre de COSmologie) database environment on our web site http://cencosw.oamp.fr with access to the database built under the Oracle environment. The catalog can be searched by coordinates, redshift interval, identification number in the EIS or GOODS catalogs, in combination with the spectra quality flags. Upon query, the database engine returns a list of targets, each of them can be examined in one single summary panel with all the VVDS spectroscopy information including the spectra, as well as the EIS and B, V, I, z HST-GOODS images, and associated photometry as shown in Fig. 8.
In the framework of the VIMOS VLT Deep Survey (VVDS),
we have observed a large sample of galaxies around
the Chandra Deep Field South, and are releasing the
redshift data to the community. A total of 1599
objects with
have a measured redshift.
The completeness in redshift measurement for the targeted
objects is high, above 84%. We find that the
redshift distribution has a median of z=0.73,
with strong high density peaks observed across the field.
The combination of this redshift survey and the HST-ACS GOODS survey enables detailed studies of the evolution of galaxies in the Chandra Deep Field South.
Acknowledgements
We are grateful to A. Cimatti and the K20 team for releasing their redshift measurements to us for comparison, and we thank G. Hasinger for communicating to us a comparison with the Szokoly et al. spectroscopy. The VLT-VIMOS observations have been carried out on garanteed time (GTO) allocated by the European Southern Observatory to the VIRMOS consortium, under a contractual agreement between the Centre National de la Recherche Scientifique of France, heading a consortium of French and Italian institutes, and ESO, to design, manufacture and test the VIMOS instrument.