2022A&A...661A.134R


Query : 2022A&A...661A.134R

2022A&A...661A.134R - Astronomy and Astrophysics, volume 661A, 134-134 (2022/5-1)

Multi-phase gas properties of extremely strong intervening DLAs towards quasars.

RANJAN A., SRIANAND R., PETITJEAN P., SHAW G., SHEEN Y.-K., BALASHEV S.A., GUPTA N., LEDOUX C. and TELIKOVA K.N.

Abstract (from CDS):

We present the results of a spectroscopic analysis of extremely strong damped Lyα absorbers (ESDLAs; log N(HI) ≥ 21.7) observed with the medium resolution spectrograph, X-shooter at theVery Large Telescope (VLT). Recent studies in the literature indicate that ESDLAs probe gas from within the star-forming disk of the associated galaxies and thus ESDLAs provide a unique opportunity to study the interstellar medium of galaxies at high redshift. We report column densities (N), equivalent widths (w, for MgII and CaII transitions), and the kinematic spread (Δv90) of species from neutral (namely OI, ArI, ClI, NI, and NaI), singly ionised (MgII, CaII, SII, NiII, MnII, TiII, and PII), and higher ionisation (CIV, SiIV, NV, and OVI) species. We estimate the dust-corrected metallicity measured using different singly ionised gas species such as PII, SII, SiII, MnII and CrII, and ZnII. We find that, using the dust correction prescription, the measured metallicities are consistent for all mentioned species in all ESDLAs within 3σ uncertainty. We further perform a quantitative comparison of column densities, equivalent widths, and kinematic spreads of ESDLAs with other samples that are associated with galaxies and detected in absorption along the line of sight towards high-redshift quasars (QSOs). We find that the distributions of the ArI to HI column density ratio (N(ArI)/N(HI)) in DLAs and ESDLAs are similar. We further report that ESDLAs do not show a strong deficiency of ArI relative to other α-capture elements as is seen in DLAs. This supports the idea that the mentioned under-abundance of ArI in DLAs is possibly caused by the presence of background UV photons that penetrate the low N(HI) clouds to ionise ArI, but they cannot penetrate deep enough in the high N(HI) ESDLA environment. The w(MgII λ2796) distribution in ESDLAs is found to be similar to that of metal-rich CI-selected absorbers, but the velocity spread of their MgII profile is different. The dust content (measured by modelling the quasar extinction) and w(CaII λ3934) distributions are similar in ESDLAs and CaII-selected absorbers, yet we do not see any correlation between w(CaII λ3934) and dust content. The Δv90 velocity spread of singly ionised species in ESDLAs is statistically smaller than that of DLAs. For higher ionisation species (such as CIV and SiIV) that trace the warm ionised medium, Δv90 is similar in the two populations. This suggests that the ESDLAs sample a different HI region of their associated galaxy compared to the general DLA population. We further study the N(ClI) distribution in high-redshift DLA and ESDLA sightlines, as ClI is a good tracer of H2 gas. The N(ClI)-N(H2) correlation is followed by all the clouds (ESDLAs and otherwise) having log N(H2) < 22.

Abstract Copyright: © A. Ranjan et al. 2022

Journal keyword(s): quasars: absorption lines - galaxies: high-redshift - galaxies: ISM

Simbad objects: 25

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Number of rows : 25
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 SDSS J000015.17+004833.2 QSO 00 00 15.1760866776 +00 48 33.306387012           ~ 26 0
2 SDSS J001743.88+130739.8 QSO 00 17 43.8804469056 +13 07 39.807895440           ~ 10 0
3 SDSS J002409.38-072553.1 QSO 00 24 09.3843629472 -07 25 53.140357992           ~ 8 0
4 SDSS J002503.02+114547.8 QSO 00 25 03.0271311336 +11 45 47.798787276           ~ 8 0
5 QSO B0027-1836 QSO 00 30 23.6259434280 -18 19 56.117225244   18.2 17.9     ~ 53 0
6 SDSS J023011.29-033450.0 QSO 02 30 11.3058775416 -03 34 49.977569568           ~ 13 0
7 SDSS J074344.26+142134.8 QSO 07 43 44.2610789520 +14 21 34.938444420           ~ 15 0
8 SDSS J084312.72+022117.2 QSO 08 43 12.7165734816 +02 21 17.341452360           ~ 22 0
9 [VV2006] J091721.4+015448 QSO 09 17 21.3681034992 +01 54 48.121717392   20.91 20.43     ~ 31 0
10 SDSS J113520.39-001053.5 QSO 11 35 20.3944527984 -00 10 53.572769436   19.36       ~ 49 0
11 SDSS J114347.21+142021.6 QSO 11 43 47.2100460024 +14 20 21.612180156           ~ 12 0
12 SDSS J123816.04+162042.5 QSO 12 38 16.0387165680 +16 20 42.513410148   21.71 20.71     ~ 19 0
13 SDSS J125855.40+121250.2 QSO 12 58 55.4099597232 +12 12 50.181702804   20.83 20.40     ~ 26 0
14 SDSS J134910.45+044819.9 QSO 13 49 10.4501160672 +04 48 19.897506072           ~ 11 0
15 SDSS J135316.83+095636.7 QSO 13 53 16.8315821784 +09 56 36.728713932   21.11 20.23     ~ 21 0
16 SDSS J141120.51+122935.9 QSO 14 11 20.5088925840 +12 29 35.919058812           ~ 9 0
17 QSO J1418+0718 QSO 14 18 01.8581916264 +07 18 43.650871884           ~ 9 0
18 [VV2006] J151349.5+035211 QSO 15 13 49.5187990104 +03 52 11.713951128   21.51 20.98     ~ 30 0
19 SDSS J214043.02-032139.2 QSO 21 40 43.0124617776 -03 21 39.253768020           ~ 23 0
20 SDSS J220525.56+102118.6 QSO 22 05 25.5676361424 +10 21 18.637385436           ~ 11 0
21 SDSS J223250.97+124225.2 QSO 22 32 50.9797006728 +12 42 25.295955228           ~ 13 0
22 [VV2006] J224621.1+132821 QSO 22 46 21.1362193920 +13 28 21.272579940   19.22 18.85     ~ 31 0
23 SDSS J232207.30+003348.9 QSO 23 22 07.3040700048 +00 33 48.993336000           ~ 13 0
24 SDSS J235124.74-063917.7 QSO 23 51 24.7369253304 -06 39 17.769065544           ~ 9 0
25 SDSS J235916.49+135443.2 QSO 23 59 16.5013814136 +13 54 43.307476560           ~ 7 0

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