MNRAS 000, 120 (0000) Preprint 12 May 2021 Compiled using MNRAS L A T E X style file v3.0 A partial Lyman limit system tracing intragroup gas at 0. 8 towards HE 1003 + 0149 Anand Narayanan 1 , Sameer 2 , Sowgat Muzahid 3,4 , Sean D. Johnson 5 , Purvi Udhwani 1 , Jane C. Charlton 2 , Valentin Mauerhofer 6,7 , Joop Schaye 8 , Mathin Yadav 1 , 1 Department of Earth and Space Sciences, Indian Institute of Space Science & Technology, Thiruvananthapuram 695547, Kerala, INDIA 2 Department of Astronomy & Astrophysics, The Pennsylvania State University, 525 Davey Laboratory University Park, PA, 16802, USA 3 Inter-University Centre for Astronomy & Astrophysics, Post Bag 4, Ganeshkhind, Savitribai Phule Pune University Campus, Pune 411 007, India 4 Leibniz-Institut fuÜr Astrophysik Potsdam (AIP), An der Sternwarte 16, D-14482 Potsdam, Germany 5 Department of Astronomy, 1085 S. University, 323 West Hall, Ann Arbor, MI 48109-1107, USA 6 Observatoire de Genéve, Université de Genéve, Chemin Pegasi 51, 1290 Versoix, Switzerland 7 Univ Lyon, Univ Lyon1, ENS de Lyon, CNRS, Centre de Recherche Astrophysique de Lyon UMR5574, 69230 Saint-Genis-Laval, France 8 Leiden Observatory, Leiden University, P.O. Box 9513, 2300 RA Leiden, the Netherlands. 12 May 2021 ABSTRACT We present analysis of the galaxy environment and physical properties of a partial Lyman limit system at = 0.83718 with H i and metal line components closely separated in redshift space ( | Δ|≈ 400 km s 1 ) towards the background quasar HE 1003 + 0149. The  /COS far- ultraviolet spectrum providescoverage of lines of oxygen ions from O i to O v. Comparison of observed spectral lines with synthetic profiles generated from Bayesian ionization modeling reveals the presence of two distinct gas phases in the absorbing medium. The low-ionization phase of the absorber has sub-solar metallicities (1/10 solar) with indications of [C/O] < 0 in each of three components. The O iv and O v trace a more diffuse higher-ionization medium with predicted H i column densities that are 2 dex lower. The quasar field observed with  /MUSE reveals three dwarf galaxies with stellar masses of 10 8 10 9 M , and with star formation rates of 0.5 1Myr 1 , at projected separations of / vir 1.8 3.0 from the absorber. Over a wider field with projected proper separation of 5 Mpc and radial velocity offset of | Δ|≤ 1000 km s 1 from the absorber, 21 more galaxies are identified in the  /VIMOS and Magellan deep galaxy redshift surveys, with 8 of them within 1 Mpc and 500 km s 1 , consistent with the line of sight penetrating a group of galaxies. The absorber presumably traces multiple phases of cool ( 10 4 K) photoionized intragroup medium. The inferred [C/O] < 0 hint at preferential enrichment from core-collapse supernovae, with such gas displaced from one or more of the nearby galaxies, and confined to the group medium. Key words: (galaxies:) quasars: absorption lines, galaxies: haloes, galaxies: groups: general, (galaxies:) intergalactic medium 1 INTRODUCTION The gaseous halos of galaxies and the regions where they connect with the filaments of the intergalactic medium hold substantial bary- onic mass in the form of metals and H i, comparable to the gaseous disks of galaxies. These regions bear the imprint of large-scale gas flows in and out of galaxies which in turn regulates galaxy evolution. Among the different classes of quasar absorbers, the partial Lyman limit and Lyman limit systems (pLLS and LLS) trace halo gas bound to galaxies and in the extended unbound medium referred to as the circumgalactic medium (CGM; Shull et al. 2014). These absorption E-mail: anand@iist.ac.in systems, are defined to be partially or fully optically thick at the Lyman limit, which corresponds to neutral gas column densities of 16 log [ ( H i)/cm 2 ]≤ 17.2, and log [ ( H i)/cm 2 ]≥ 17.2 respectively. Recently, several authors have also highlighted the importance of pLLS and LLS as a means to discern inflows and outflows from galaxies. Lehner et al. (2013) found a bimodal- ity in the metallicity distribution for a sample of low redshift (1) absorbers having 16.2 log [ ( H i)/cm 2 ] 18.5 with distinct peaks at log( / ) = 0.3, and 1.6, and a dip at log( / )≈−1. The metal enriched portion of this sample is seen as tracing gas outflows from galaxies while the low metallicity portion is interpreted as accretion of cool gas from the IGM onto galaxies (Wotta et al. 2016). A higher fraction of this metal-poor © 0000 The Authors arXiv:2105.04841v1 [astro-ph.GA] 11 May 2021