2023ApJ...944..101B


Query : 2023ApJ...944..101B

2023ApJ...944..101B - Astrophys. J., 944, 101 (2023/February-2)

The Bimodal Absorption System Imaging Campaign (BASIC). I. A Dual Population of Low-metallicity Absorbers at z < 1.

BERG M.A., LEHNER N., HOWK J.C., O'MEARA J.M., SCHAYE J., STRAKA L.A., COOKSEY K.L., TRIPP T.M., PROCHASKA J.X., OPPENHEIMER B.D., JOHNSON S.D., MUZAHID S., BORDOLOI R., WERK J.K., FOX A.J., KATZ N., WENDT M., PEEPLES M.S., RIBAUDO J. and TUMLINSON J.

Abstract (from CDS):

The bimodal absorption system imaging campaign (BASIC) aims to characterize the galaxy environments of a sample of 36 H I-selected partial Lyman limit systems (pLLSs) and Lyman limit systems (LLSs) in 23 QSO fields at z ≲ 1. These pLLSs/LLSs provide a unique sample of absorbers with unbiased and well-constrained metallicities, allowing us to explore the origins of metal-rich and low-metallicity circumgalactic medium (CGM) at z < 1. Here we present Keck/KCWI and Very Large Telescope/MUSE observations of 11 of these QSO fields (19 pLLSs) that we combine with Hubble Space Telescope/Advanced Camera for Surveys imaging to identify and characterize the absorber-associated galaxies at 0.16 ≲ z ≲ 0.84. We find 23 unique absorber-associated galaxies, with an average of one associated galaxy per absorber. For seven absorbers, all with <10% solar metallicities, we find no associated galaxies with $\mathrm{log}{M}_{\star }\gtrsim 9.0$ within ρ/Rvir and ∣Δv∣/vesc ≤ 1.5 with respect to the absorber. We do not find any strong correlations between the metallicities or H I column densities of the gas and most of the galaxy properties, except for the stellar mass of the galaxies: the low-metallicity ([X/H] ≤ -1.4) systems have a probability of ${0.39}_{-0.15}^{+0.16}$ for having a host galaxy with $\mathrm{log}{M}_{\star }\geqslant 9.0$ within ρ/Rvir ≤ 1.5, while the higher metallicity absorbers have a probability of ${0.78}_{-0.13}^{+0.10}$. This implies metal-enriched pLLSs/LLSs at z < 1 are typically associated with the CGM of galaxies with $\mathrm{log}{M}_{\star }\gt 9.0$, whereas low-metallicity pLLSs/LLSs are found in more diverse locations, with one population arising in the CGM of galaxies and another more broadly distributed in overdense regions of the universe. Using absorbers not associated with galaxies, we estimate the unweighted geometric mean metallicity of the intergalactic medium to be [X/H] ≲ -2.1 at z < 1, which is lower than previously estimated.

Abstract Copyright: © 2023. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Circumgalactic medium - Galaxy spectroscopy - Intergalactic medium - Lyman limit systems - Metallicity - Quasar absorption line spectroscopy

Nomenclature: Figs A1-A10, Tables 5+A1+A2: [BLH2023] HEHHMM+DDMM NNNN N=9, [BLH2023] JHHMM+DDMM NNNN N=14, [BLH2023] PGHHMM+DDd NNNN N=4, [BLH2023] PKSHHMM+DDd NNNNN N=6.

Status at CDS : Acronym for new objects described in the dictionary of nomenclature and being created in SIMBAD.

Simbad objects: 47

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Number of rows : 47
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 M 31 AGN 00 42 44.330 +41 16 07.50 4.86 4.36 3.44     ~ 13622 1
2 [BLH2023] HE0153-4520 966 G 01 55 12.9428229384 -45 06 34.525340784           ~ 2 0
3 QSO J0155-4506 QSO 01 55 13.2179169408 -45 06 11.577944484   15.1       ~ 54 0
4 4C -04.06 QSO 02 35 07.3418452008 -04 02 05.317096956   16.61 16.46 16.2   ~ 222 1
5 [BLH2023] PKS0405-123 3207 G 04 07 48.310 -12 11 02.35           ~ 1 0
6 PKS 0405-123 Bla 04 07 48.4309841856 -12 11 36.659928408   15.09 14.86 14.7   ~ 531 1
7 [BLH2023] PKS0405-123 1822 G 04 07 51.1961810568 -12 11 37.115573028       17.430   ~ 17 0
8 [BLH2023] HE0439-5254 1309 G 04 40 10.520 -52 48 10.81           ~ 1 0
9 QSO J0440-5248 QSO 04 40 12.0482632416 -52 48 17.514120888     16.10     ~ 42 0
10 [BLH2023] HE0439-5254 1083 G 04 40 12.740 -52 48 20.26           ~ 1 0
11 [BLH2023] HE0439-5254 1009 G 04 40 13.960 -52 48 10.15           ~ 1 0
12 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
13 [BLH2023] PKS0552-640 6085 G 05 52 20.300 -64 02 05.19           ~ 1 0
14 [BLH2023] PKS0552-640 6264 G 05 52 22.960 -64 02 24.04           ~ 1 0
15 [BLH2023] PKS0552-640 5939 G 05 52 23.140 -64 02 36.68           ~ 1 0
16 2MASS J05522451-6402108 Sy1 05 52 24.5023213488 -64 02 10.757771160     15.04     ~ 55 1
17 [BLH2023] PKS0552-640 78334 G 05 52 26.660 -64 02 17.29           ~ 1 0
18 [BLH2023] HE1003+0149 974 G 10 05 34.010 +01 34 57.24           ~ 1 0
19 [BLH2023] HE1003+0149 997 G 10 05 34.120 +01 35 00.11           ~ 1 0
20 [BLH2023] HE1003+0149 1001 G 10 05 34.190 +01 34 57.91           ~ 1 0
21 QSO J1005+0134 QSO 10 05 35.2474303944 +01 34 45.713350380   17.21 16.89     ~ 59 0
22 [BLH2023] HE1003+0149 1229 G 10 05 36.760 +01 34 53.65           ~ 1 0
23 [BLH2023] HE1003+0149 1206 G 10 05 37.260 +01 34 26.65           ~ 1 0
24 PG 1216+069 Sy1 12 19 20.9318278680 +06 38 38.467059252   15.68 15.65     ~ 302 0
25 Ton 153 QSO 13 19 56.2320886176 +27 28 08.186323080   16.12 15.98     ~ 156 0
26 QSO J1341+4123 QSO 13 41 00.7893930432 +41 23 14.130152880   17.04 16.76     ~ 131 0
27 [BLH2023] PG1338+416 1118 G 13 41 01.390 +41 22 56.66           ~ 2 0
28 PB 2049 QSO 14 19 10.2069131136 +42 07 46.911715896   16.9 17.31 17.1   ~ 50 0
29 [BLH2023] J1419+4207 1003 G 14 19 10.960 +42 07 55.67           ~ 1 0
30 [BLH2023] J1419+4207 1066 G 14 19 11.410 +42 07 47.82           ~ 1 0
31 [BLH2023] J1419+4207 1163 G 14 19 12.210 +42 07 36.77           ~ 1 0
32 QSO J1435+3604 QSO 14 35 11.5257590496 +36 04 37.175594052   17.30 17.22     ~ 63 0
33 [BLH2023] J1435+3604 1060 G 14 35 13.010 +36 04 25.67           ~ 1 0
34 [BLH2023] J1435+3604 1042 G 14 35 14.010 +36 04 25.23           ~ 1 0
35 [BLH2023] J1435+3604 1063 G 14 35 14.160 +36 04 19.99           ~ 1 0
36 [BLH2023] J1435+3604 955 G 14 35 14.540 +36 04 37.93           ~ 1 0
37 [BLH2023] PG1522+101 1151 G 15 24 22.900 +09 58 15.57           ~ 1 0
38 QSO B1521+1009 QSO 15 24 24.5234088744 +09 58 29.087917572   15.74 16.2     ~ 145 0
39 [BLH2023] PG1522+101 934 G 15 24 26.140 +09 58 33.11           ~ 1 0
40 [BLH2023] PG1522+101 1077 G 15 24 26.160 +09 58 17.63           ~ 1 0
41 [BLH2023] J1619+3342 1006 G 16 19 15.950 +33 42 35.11           ~ 1 0
42 [BLH2023] J1619+3342 946 G 16 19 16.030 +33 42 48.72           ~ 1 0
43 [BLH2023] J1619+3342 1028 G 16 19 16.100 +33 42 32.04           ~ 1 0
44 QSO J1619+3342 QSO 16 19 16.5426908544 +33 42 38.375748828   17.30 17.26     ~ 61 0
45 [BLH2023] J1619+3342 1180 G 16 19 17.260 +33 42 33.35           ~ 1 0
46 [BLH2023] J1619+3342 1179 G 16 19 17.690 +33 42 33.86           ~ 1 0
47 [BLH2023] J1619+3342 1137 G 16 19 18.380 +33 42 35.78           ~ 1 0

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