A&A 412, 707-709 (2003)
DOI: 10.1051/0004-6361:20034339
Research Note
A. I. Ryabinkov - A. D. Kaminker - D. A. Varshalovich
Ioffe Physical Technical Institute, Politekhnicheskaya 26, 194021 St. Petersburg, Russia
Received 12 September 2003 / Accepted 26 September 2003
Abstract
We present a new catalog of absorption-line systems
identified in the quasar spectra.
It contains data on 821 QSOs
and 8558 absorption systems comprising
16 139 absorption lines
with measured redshifts
in the QSO spectra.
The catalog includes
absorption-line systems consisting of
lines of heavy elements,
lines of neutral hydrogen,
Lyman limit systems,
damped Ly absorption systems,
and broad absorption-line systems.
Using the data of the present catalog
we also discuss
redshift distributions of absorption-line systems.
Key words: galaxies: quasar: absorption lines - galaxies: high-redshift
Absorption lines and absorption-line systems (ALSs) observed in the spectra of QSOs contain fundamental information on the distribution of matter between the observer and the QSO, and on physical processes in the Universe in different epochs of the cosmological evolution. To date, thousands of ALSs have been identified and their number grows persistently, scattered over numerous sources. This stimulates the creation of catalogs of ALSs comprising the most complete data on the absorption lines and their systems.
Catalogs of ALSs have been compiled many times.
We mention
the early catalogs of Perry et al. (1978)
and Ellis & Phillips (1978),
and the later vast QSO catalogs
of Hewitt & Burbidge
(1980, 1987, 1989, 1993)
which include also
data on the ALSs
detected in the QSO spectra.
Junkkarinen et al. (1991) and
York et al. (1991)
created special ALS catalogs
most complete for that time.
The new generation of telescopes (Keck, VLT, etc.)
has yielded a great amount of new spectroscopic data.
Some have been collected
in special catalogs including either
the results
of certain spectral investigations or
the definite types of ALSs
(e.g., Lyman limit systems - LLS,
damped Ly absorption systems - DLA,
broad absorption-line systems - BAL,
etc.).
For example, the catalog by
Outram et al. (2001) of the ALSs detected
in the 2dF QSO Redshift Survey or
the catalogue of DLAs compiled by
Curran et al. (2002).
However, as far as we know, there are no
modern catalogs comprising comprehensive data on
the ALSs registered to date.
Our new catalog is an attempt to collect the basic information on the ALSs in QSO spectra. The data are taken from publications available up to January 2002. The catalog includes, in particular, all the data of the catalogs of Junkkarinen et al. (1991) and York et al. (1991). The catalog consists of introduction (ReadMe), Tables 1 and 2, and list of references, which are available in electronic form at www.ioffe.ru/astro/QC and at the CDS.
Table 1 (Quasars) contains data on
821 QSOs whose characteristics
of spectral observations are collected in Table 2.
The QSO data are based on the
catalog of Veron-Cetty & Veron (2001).
The following information on the QSOs is given:
the QSO's name (J2000)
identical to the name in Table 2 (see below)
and the name given
in the catalog of Veron-Cetty & Veron
(2001); equatorial coordinates at 2000 and 1950,
right ascensions
and
,
and declinations
and
in the order of increasing right ascensions; emission-line redshift
;
apparent magnitude V; absolute magnitude M.
Table 2 (Absorption systems)
contains the following information
on spectral observations of the QSOs
and on the detected ALSs:
(i) the name of QSOs (J2000 and Q1950)
which spectral observations
are presented in literature;
(ii) parameters of spectral observations (see below);
(iii) characteristics of absorption lines
combined in the systems.
The parameters of spectral observations of 821 QSOs
contain the following data:
the interval of wavelengths (Å)
covered by the cited observations;
spectral resolution
(Å);
signal-to-noise ratio
,
averaged over the entire spectral
interval of observations;
in some cases, the threshold (minimal) value
of the absorption equivalent width in Å
(
or
the observer or the rest reference
frame) used by the cited authors
as the criterion of line detection;
the emission-line redshift
;
references.
Table 2 includes the characteristics of 16 139 absorption lines
detected in the spectra of 735 QSOs.
These lines form 8558 absorption systems.
In the spectra of 14 QSOs
only Galactic interstellar lines
have been detected;
characteristics of
these lines are excluded.
In the spectra of 72 QSOs
the absorption lines
have not been detected or identified.
Table 2 comprises
3039 absorption-line systems
including lines of heavy elements.
For instance, we present 2871 resonance doublets
of ions Mg II, Al III, C IV, Si IV, N V,
and O VI. The table comprises also
6063 systems containing
lines of neutral hydrogen (HI).
In particular, there are 5554 systems
including only lines of HI,
146 LLSs, 195 DLA systems,
and 39 BAL systems.
LLSs are optically thick
at the HI Lyman limit (912 Å).
They correspond to HI column densities N(HI)
.
DLA systems correspond to high HI column densities N(HI)
.
BAL systems are characterized
by wide absorption troughs produced by
ions with an outflow velocity
extending up to 60 000 km s-1relative to the QSO's.
We rule out absorption systems consisting
only of one heavy-element
absorption line.
The data are listed in the order of increasing absorption-system redshifts.
For heavy-element and HI systems
we present the following information:
the absorption-system redshift
,
name of the ion identified,
laboratory wavelength
in Å,
observed wavelength
in Å,
error
of the value
at 1
significance level,
absorption-line equivalent width
(Å)
(measured in the observer frame)
or column density of the ion
(cm-2),
error
(or
)
of the values
or
(cm-2), respectively.
For the LLSs we give only
the redshift
of the absorption edge (912 Å).
For the DLA systems we present:
,
the observational equivalent width
(Å)
or HI column density
(HI) (cm-2).
For the BAL systems:
the averaged value of
,
names of identified ions,
width of the trough
.
Table 2 contains also a few sets of observational data on spectra of the QSOs registered in different observations and presented by different authors. Special signs indicate the cases where absorption lines are blended by unidentified lines.
All relevant notations and comments for users are given in the introduction (ReadMe). The list of references contains literature sources quoted in Table 2.
The authors are planning to replenish the catalog regularly. Any remarks and comments would be greatly appreciated.
All absorption-line systems
collected in the catalog belong to
the redshift interval from
to
.
As an illustration, we
compare (Fig. 1) two z-distributions
of the absorption systems including heavy-elements lines
within the redshift interval z=0-3.7.
One of them
is obtained using the data of the catalog
of Junkkarinen et al. (1991)
and the other is based on
the present catalog.
In accordance with the data
of Junkkarinen et al. (1991) all
absorption redshifts
fallen within an interval of 500 km s-1are treated as a single system
with a single
.
We have compiled 2003 absorption systems
versus 847 systems from the catalog of
Junkkarinen et al. (1991).
Both distributions
are obtained using the so-called
sliding-average approach, in which
a set of consecutive displacements of
the averaging
bin
is performed
along the z axis with the step
.
![]() |
Figure 1: Two z-distributions of absorption systems observed in QSO spectra containing heavy-elements lines within the redshift interval z=0-3.7: 847 systems are obtained from the data of Junkkarinen et al. (1991) and 2003 systems are obtained from the present catalogue (see text). |
Open with DEXTER |
As shown by Ryabinkov et al. (2001) from the data of Junkkarinen et al. (1991) the z-distribution of absorption-line systems displaces a pattern of alternating maxima (peaks) and minima (dips) relative to a smooth curve. It is essential that their positions turn out to be independent of observation directions. Additionally, the data revealed a regularity (sort of periodicity) of the distribution with respect to some rescaled functions of z. This suggests that the derived distribution of absorption matter is not only spatial but also temporal in nature. A comparison of the two z-distributions (Fig. 1) indicates that the positions of all main peaks and dips remain the same after the expansion of statistics some of them are now more significant.
These conclusions confirm the results of earlier statistical analyses (Ryabinkov et al. 1998; Kaminker et al. 2000) of z-distributions of C IV and Mg II absorption systems. Detailed statistical analysis of such distributions based on the present catalogue will be done elsewhere.
Acknowledgements
We are grateful to D.G. Yakovlev for useful remarks. The work was partly supported by RFBR grants No. 02-02-16278 and 03-07-90200.