2005MNRAS.364.1467Z


Query : 2005MNRAS.364.1467Z

2005MNRAS.364.1467Z - Mon. Not. R. Astron. Soc., 364, 1467-1487 (2005/December-3)

Reconciling the local galaxy population with damped Lyman α cross-sections and metal abundances.

ZWAAN M.A., VAN DER HULST J.M., BRIGGS F.H., VERHEIJEN M.A.W. and RYAN-WEBER E.V.

Abstract (from CDS):

A comprehensive analysis of 355 high-quality Westerbork Synthesis Radio Telescope (WSRT) Hi 21-cm line maps of nearby galaxies shows that the properties and incident rate of damped Lyman α absorption systems (DLAs) observed in the spectra of high-redshift QSOs are in good agreement with DLAs originating in gas discs of galaxies like those in the z~ 0 population. Comparison of low-z DLA statistics with the Hi incidence rate and column density distribution f(NHi) for the local galaxy sample shows no evidence for evolution in the integral `cross-section density'<nσ≥l–1 (l= mean free path between absorbers) below z~ 1.5, implying that there is no need for a hidden population of galaxies or Hi clouds to contribute significantly to the DLA cross-section. Compared with z~ 4, our data indicate evolution of a factor of 2 in the comoving density along a line of sight. We find that dN/dz(z= 0) = 0.045±0.006. The idea that the local galaxy population can explain the DLAs is further strengthened by comparing the properties of DLAs and DLA galaxies with the expectations based on our analysis of local galaxies. The distribution of luminosities of DLA host galaxies, and of impact parameters between QSOs and the centres of DLA galaxies, is in good agreement with what is expected from local galaxies. Approximately 87 per cent of low-z DLA galaxies are expected to be fainter than L*, and 37 per cent have impact parameters less than 1 arcsec at z= 0.5. The analysis shows that some host galaxies with very low impact parameters and low luminosities are expected to be missed in optical follow-up surveys. The well-known metallicity-luminosity relation in galaxies, in combination with metallicity gradients in galaxy discs, causes the expected median metallicity of low-z DLAs to be low (∼1/7 solar), which is also in good agreement with observations of low-z DLAs. We find that f(NHi) can be fitted satisfactorily with a gamma distribution, a single power law is not a good fit at the highest column densities NHi> 1021/cm2. The vast majority (~81 per cent) of the Hi gas in the local Universe resides in column densities above the classical DLA limit (NHi> 2x1020/cm2), with NHi∼ 1021/cm2 dominating the cosmic Hi mass density.

Abstract Copyright: 2005 The Authors. Journal compilation © 2005 RAS

Journal keyword(s): surveys - galaxies: ISM - quasars: absorption lines - galaxies: statistics - radio lines: galaxies

Simbad objects: 36

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Number of rows : 36
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 [LBS2003] FBQS J0051+0041 A G 00 51 30.5 +00 41 50           ~ 3 0
2 LBQS 0058+0155 QSO 01 00 54.1201107072 +02 11 36.331220364   17.48 17.16     ~ 166 0
3 QSO B0235+1624 BLL 02 38 38.93010450 +16 36 59.2745528   16.46 15.50 15.92   ~ 1614 2
4 YYG A G 02 38 38.94 +16 36 57.4   20.31       ~ 38 0
5 UGC 2459 AG? 03 00 36.786 +49 02 38.45   18       ~ 43 0
6 [CL2003] PKS 0439-433 1 G 04 41 17.2967 -43 13 43.405           ~ 11 0
7 QSO J0441-4313 Bla 04 41 17.3385563928 -43 13 45.488722116   16.64 16.36 16.54 16.26 ~ 111 1
8 QSO B0454+0356 Bla 04 56 47.1747907776 +04 00 52.946102484   16.76 16.53 16.26   ~ 247 1
9 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
10 Z 285-16 GiG 07 09 05.9246956320 +61 35 44.062687680   13.1       ~ 57 0
11 6C 073759+311929 Bla 07 41 10.70330407 +31 12 00.2291151   17.02 16.89 16.322   ~ 468 1
12 3C 196 Sy1 08 13 36.0561170112 +48 13 02.644966020   18.36 17.79     ~ 578 2
13 7C 082754.29+242103.00 Bla 08 30 52.08619250 +24 10 59.8202919   17.62 17.26 16.30   ~ 563 1
14 SDSS J083052.50+241101.9 G 08 30 52.44800 +24 11 01.1197   20.64       ~ 18 0
15 QSO B0952+179 QSO 09 54 56.82361677 +17 43 31.2221518   17.31 17.23     ~ 222 1
16 QSO B1122-168 QSO 11 24 42.8658917592 -17 05 17.389038732   16.5 16.5 16.1   ~ 132 1
17 QSO J1130-1449 Bla 11 30 07.0523452128 -14 49 27.388021944   17.17 16.90 16 16.97 ~ 739 1
18 [LBS2003] FBQS J1137+3907 C G 11 37 09.5 +39 07 23           ~ 2 0
19 NGC 4068 AG? 12 04 03.265 +52 35 26.05   13.29   12.77   ~ 189 0
20 Z 215-23 GiP 12 05 57.746 +43 08 36.08   14.40       ~ 123 1
21 LBQS 1209+1046 QSO 12 11 40.6043132184 +10 30 02.074373208   18.52 18.37     ~ 122 0
22 NGC 4203 LIN 12 15 05.0549203560 +33 11 50.383965120   12.98 11.99     ~ 514 2
23 Ton 1480 QSO 12 15 09.2309649888 +33 09 55.239405012   16.56 16.45     ~ 59 0
24 NGC 4395 Sy2 12 25 48.8633109888 +33 32 48.700168152 10.84 10.54 10.11 9.98   ~ 1286 1
25 MCG+07-26-010 EmG 12 28 44.078 +43 13 25.79   16.0       ~ 106 0
26 4C -02.55 Bla 12 32 00.0159535440 -02 24 04.793069304   17.41 17.06 16.4   ~ 440 1
27 NGC 4559 H2G 12 35 57.6402869976 +27 57 35.859278160   10.46 10.01     ~ 667 1
28 Z 316-9 AG? 13 06 24.85 +67 42 25.0 14.08 13.61 13.08 12.98   ~ 268 1
29 3C 286 Sy1 13 31 08.2883506368 +30 30 32.960091564   17.51 17.25     ~ 4558 2
30 QSO B1331+170 Bla 13 33 35.7827544072 +16 49 04.013500728   16.84 16.71 16.41   ~ 469 1
31 Z 272-13 AG? 13 54 45.602 +53 54 20.06   14.2       ~ 219 0
32 NAME Ursa Major Cluster ClG 15 08.8 +67 07           ~ 424 1
33 QSO B1543+5921 QSO 15 44 20.2979128848 +59 12 27.082778112   16.1 17.63 16.4   ~ 53 0
34 SBSG 1543+593 LSB 15 44 20.30 +59 12 24.2   17.5 16.9     ~ 55 2
35 4C 23.43 Bla 16 24 39.0838297968 +23 45 12.223370412   17.91 17.47     ~ 343 1
36 4C 12.59 QSO 16 31 45.1708807968 +11 56 03.203387592   18.38 18.40     ~ 122 1

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