2023A&A...673A..89N


Query : 2023A&A...673A..89N

2023A&A...673A..89N - Astronomy and Astrophysics, volume 673A89 (2023/5-1)

Proximate molecular quasar absorbers Chemical enrichment and kinematics of the neutral gas.

NOTERDAEME P., BALASHEV S., CUELLAR R., KROGAGER J.-K., COMBES F., DE CIA A., GUPTA N., LEDOUX C., LOPEZ S. and SRIANAND R.

Abstract (from CDS):

Proximate molecular quasar absorbers (PH2) are an intriguing population of absorption systems that was recently uncovered through strong H2 absorption at a small velocity separation from the background quasars. We performed a multi-wavelength spectroscopic follow-up of 13 such systems with VLT/X-shooter. Here, we present the observations and study the overall chemical enrichment measured from the H I, H2, and metal lines. We combined this with an investigation of the neutral gas kinematics with respect to the quasar host. We find gas-phase metallicities in the range 2% to 40% of the solar value, that is, in the upper-half range of H I-selected proximate damped Lyman-α systems, but similar to what is seen in intervening H2-bearing systems. This is likely driven by similar selection effects that play against the detection of most metal- and molecule-rich systems in absorption. Differences are seen in the abundance of dust (from [Zn/Fe]) and its depletion pattern when compared to intervening systems, however, possibly indicating different dust production or destruction close to the active galactic nucleus. We also note the almost ubiquitous presence of a high-ionisation phase traced by N V in proximate systems. In spite of the hard UV field from the quasars, we found no strong overall deficit of neutral argon, at least when compared to intervening damped Lyman-α systems. The reason likely is that argon is mostly neutral in the H2 phase, which accounts for a large fraction of the total amount of metals. We measured the quasar systemic redshifts through emission lines from both ionised gas and CO(3-2) emission, the latter being detected in all six cases for which we obtained 3 mm data from complementary NOEMA observations. For the first time, we observe a trend between the line-of-sight velocity with respect to systemic redshift and metallicity of the absorbing gas. This suggests that high-metallicity neutral and molecular gas is more likely to be located in outflows, while low-metallicity gas could be more clustered in velocity space around the quasar host, possibly with an infalling component.

Abstract Copyright: © The Authors 2023

Journal keyword(s): galaxies: active - galaxies: evolution - quasars: general - quasars: absorption lines - quasars: emission lines

Simbad objects: 15

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Number of rows : 15
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 SDSS J001514.81+184212.3 QSO 00 15 14.8208801424 +18 42 12.401174736           ~ 11 0
2 SDSS J001930.55-013708.4 QSO 00 19 30.5491980096 -01 37 08.448537828           ~ 14 0
3 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 12317 1
4 SDSS J005917.64+112407.7 QSO 00 59 17.6332835112 +11 24 07.650192672           ~ 11 0
5 SDSS J012555.11-012925.1 QSO 01 25 55.1139355704 -01 29 25.272475944           ~ 9 0
6 SDSS J013644.02+044039.0 QSO 01 36 44.0194613256 +04 40 39.109620504           ~ 15 0
7 SDSS J085859.66+174925.1 QSO 08 58 59.6647623648 +17 49 25.177561392           ~ 12 0
8 SDSS J123602.11+001024.6 QSO 12 36 02.1182718312 +00 10 24.549544740           ~ 17 0
9 SDSS J124829.50+063935.6 QSO 12 48 29.5047357120 +06 39 35.584287048           ~ 14 0
10 SDSS J125917.30+030922.5 QSO 12 59 17.3080665072 +03 09 22.537766412           ~ 11 0
11 SDSS J133111.41+020609.0 QSO 13 31 11.4096736536 +02 06 09.033476652           ~ 10 0
12 SDSS J135808.94+141053.2 QSO 13 58 08.9485980792 +14 10 53.264669880   20.74 20.13     ~ 18 0
13 SDSS J222807.36-022117.2 QSO 22 28 07.3544202408 -02 21 17.139473748           ~ 11 0
14 SDSS J232506.61+153929.3 QSO 23 25 06.6120441552 +15 39 29.387264976           ~ 7 0
15 QSO J2340-0053 QSO 23 40 23.6700032496 -00 53 27.001299696   18.26 17.93     ~ 109 1

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