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Published September 10, 2022 | public
Journal Article

KODIAQ-Z: Metals and Baryons in the Cool Intergalactic and Circumgalactic Gas at 2.2 ≲ z ≲ 3.6

Abstract

We present the KODIAQ-Z survey aimed to characterize the cool, photoionized gas at 2.2 ≲ z ≲ 3.6 in 202 H I-selected absorbers with 14.6 ≤ log N_HI < 20 that probe the interface between galaxies and the intergalactic medium (IGM). We find that gas with 14.6 ≤ log N_HI < 20 at 2.2 ≲ z ≲ 3.6 can be metal-rich (−1.6 ≲ [X/H] ≲ − 0.2) as seen in damped Lyα absorbers (DLAs); it can also be very metal-poor ([X/H] < − 2.4) or even pristine ([X/H] < − 3.8), which is not observed in DLAs but is common in the IGM. For 16 < log N_HI < 20 absorbers, the frequency of pristine absorbers is about 1%–10%, while for 14.6 ≤ log N_HI ≤ 20 absorbers it is 10%–20%, similar to the diffuse IGM. Supersolar gas is extremely rare (<1%) at these redshifts. The factor of several thousand spread from the lowest to highest metallicities and large metallicity variations (a factor of a few to >100) between absorbers separated by less than Δv < 500 km s−1 imply that the metals are poorly mixed in 14.6 ≤ log N_HI < 20 gas. We show that these photoionized absorbers contribute to about 14% of the cosmic baryons and 45% of the cosmic metals at 2.2 ≲ z ≲ 3.6. We find that the mean metallicity increases with N_HI, consistent with what is found in z < 1 gas. The metallicity of gas in this column density regime has increased by a factor ∼8 from 2.2 ≲ z ≲ 3.6 to z < 1, but the contribution of the 14.6 ≤ log N_HI < 19 absorbers to the total metal budget of the universe at z < 1 is a quarter of that at 2.2 ≲ z ≲ 3.6. We show that FOGGIE cosmological zoom-in simulations have a similar evolution of [X/H] with N_HI, which is not observed in lower-resolution simulations. In these simulations, very metal-poor absorbers with [X/H] < − 2.4 at z ∼ 2–3 are tracers of inflows, while higher-metallicity absorbers are a mixture of inflows and outflows.

Additional Information

We thank the referee for constructive comments that improved our manuscript. We are grateful to Anna Wright for providing the satellite catalogs used in Figure 31 based on the methods of Pontzen & Tremmel (2018). We are grateful to Saloni Deepak for identifying a few typographical errors in the cosmic baryon and metal budget sections prior to publication. The main support for this research was made by NASA through the Astrophysics Data Analysis Program (ADAP) grant NNX16AF52G. Additional support was provided by NSF grant award No. 1516777. Support for the development of the CLOUDY ionization models was provided by NASA through grants HST-AR-12854 and HST-AR-15634 from the Space Telescope Science Institute, which is operated by the Association of Universities for Research in Astronomy, Incorporated, under NASA contract NAS5-26555. C.C. and B.W.O. acknowledge support by NSF grants no. AST-1517908 and AST-1908109 and NASA ATP grants NNX15AP39G and 80NSSC18K1105. This project has received funding from the European Research Council (ERC) under the European Union's Horizon 2020 research and innovation program (grant agreement No. 757535). This work has been supported by Fondazione Cariplo, grant No. 2018-2329. All the data presented in this work were obtained from KODIAQ DR1 and DR2, which were funded through NASA ADAP grants NNX10AE84G and NNX16AF52G, along with NSF award No. 1516777. This research has made use of the Keck Observatory Archive (KOA), which is operated by the W. M. Keck Observatory and the NASA Exoplanet Science Institute (NExScI), under contract with the National Aeronautics and Space Administration. The authors wish to recognize and acknowledge the very significant cultural role and reverence that the summit of Maunakea has always had within the indigenous Hawaiian community. The photoionization modeling was supported by the Notre Dame Center for Research Computing through the Grid Engine software and, together with the Notre Dame Cooperative Computing Lab, through the HTCondor software. Analysis of the FOGGIE simulations used the resources of the Michigan State University High Performance Computing Center, operated by the Institute for Cyber-Enabled Research. The FOGGIE calculations were performed using the publicly available Enzo code (Bryan et al. 2014; Brummel-Smith et al. 2019) and analyzed using yt (Turk et al. 2011), both of which are the products of the collaborative effort of many independent scientists from numerous institutions around the world.

Additional details

Created:
August 22, 2023
Modified:
October 24, 2023