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1. The CGM ² Survey: Circumgalactic O vi from Dwarf to Massive Star-forming Galaxies

   https://doi.org/10.3847/1538-4357/ac450c  

   Tchernyshyov, Kirill; Werk, Jessica K.; Wilde, Matthew C.; Prochaska, J. Xavier; Tripp, Todd M.; Burchett, Joseph N.; Bordoloi, Rongmon; Howk, J. Christopher; Lehner, Nicolas; O’Meara, John M.; et al (March 2022, The Astrophysical Journal)

   Abstract We combine 126 new galaxy-O vi absorber pairs from the CGM 2 survey with 123 pairs drawn from the literature to examine the simultaneous dependence of the column density of O vi absorbers ( N O VI ) on galaxy stellar mass, star-formation rate, and impact parameter. The combined sample consists of 249 galaxy-O vi absorber pairs covering z = 0–0.6, with host galaxy stellar masses M * = 10 7.8 –10 11.2 M ⊙ and galaxy-absorber impact parameters R ⊥ = 0–400 proper kiloparsecs. In this work, we focus on the variation of N O VI with galaxy mass and impact parameter among the star-forming galaxies in the sample. We find that the average N O VI within one virial radius of a star-forming galaxy is greatest for star-forming galaxies with M * = 10 9.2 –10 10 M ⊙ . Star-forming galaxies with M * between 10 8 and 10 11.2 M ⊙ can explain most O vi systems with column densities greater than 10 13.5 cm −2 . Sixty percent of the O vi mass associated with a star-forming galaxy is found within one virial radius, and 35% is found between one and two virial radii. In general, we find that some departure from hydrostatic equilibrium in the CGM is necessary to reproduce the observed O vi amount, galaxy mass dependence, and extent. Our measurements serve as a test set for CGM models over a broad range of host galaxy masses. 

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2. The CGM ² Survey: Quenching and the Transformation of the Circumgalactic Medium

   https://doi.org/10.3847/1538-4357/acc86a  

   Tchernyshyov, Kirill; Werk, Jessica K.; Wilde, Matthew C.; Prochaska, J. Xavier; Tripp, Todd M.; Burchett, Joseph N.; Bordoloi, Rongmon; Howk, J. Christopher; Lehner, Nicolas; O’Meara, John M.; et al (May 2023, The Astrophysical Journal)

   Abstract This study addresses how the incidence rate of strong O vi absorbers in a galaxy’s circumgalactic medium (CGM) depends on galaxy mass and, independently, on the amount of star formation in the galaxy. We use Hubble Space Telescope/Cosmic Origins Spectrograph absorption spectroscopy of quasars to measure O vi absorption within 400 projected kpc and 300 km s −1 of 52 galaxies with M * ∼ 3 × 10 10 M ⊙ . The galaxies have redshifts 0.12 < z < 0.6, stellar masses 10 10.1 M ⊙ < M * < 10 10.9 M ⊙ , and spectroscopic classifications as star-forming or passive. We compare the incidence rates of high column density O vi absorption ( N O VI ≥ 10 14.3 cm −2 ) near star-forming and passive galaxies in two narrow ranges of stellar mass and, separately, in a matched range of halo mass. In all three mass ranges, the O vi covering fraction within 150 kpc is higher around star-forming galaxies than around passive galaxies with greater than 3 σ -equivalent statistical significance. On average, the CGM of star-forming galaxies with M * ∼ 3 × 10 10 M ⊙ contains more O vi than the CGM of passive galaxies with the same mass. This difference is evidence for a CGM transformation that happens together with galaxy quenching and is not driven primarily by halo mass. 

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3. The COS-Holes Survey: Connecting Galaxy Black Hole Mass with the State of the CGM

   https://doi.org/10.3847/1538-4357/ad4ecc  

   Garza, Samantha L; Werk, Jessica K; Oppenheimer, Benjamin D; Tchernyshyov, Kirill; Sanchez, N Nicole; Faerman, Yakov; Rubin, Kate_H R; Bentz, Misty C; Davies, Jonathan J; Burchett, Joseph N; et al (July 2024, The Astrophysical Journal)

   Abstract We present an analysis of Hubble Space Telescope COS/G160M observations of CIVin the inner circumgalactic medium (CGM) of a novel sample of eightz∼ 0,L≈L^⋆galaxies, paired with UV-bright QSOs at impact parameters (R_proj) between 25 and 130 kpc. The galaxies in this stellar-mass-controlled sample (log₁₀M_⋆/M_⊙∼ 10.2–10.9M_⊙) host supermassive black holes (SMBHs) with dynamically measured masses spanning log₁₀M_BH/M_⊙∼ 6.8–8.4; this allows us to compare our results with models of galaxy formation where the integrated feedback history from the SMBH alters the CGM over long timescales. We find that the CIVcolumn density measurements (N_{C IV}; average log₁₀N_{C IV,CH}= 13.94 ± 0.09 cm⁻²) are largely consistent with existing measurements from other surveys ofN_{C IV}in the CGM (average log₁₀N_{C IV,Lit}= 13.90 ± 0.08 cm⁻²), but do not show obvious variation as a function of the SMBH mass. By contrast, specific star formation rate (sSFR) is highly correlated with the ionized content of the CGM. We find a large spread in sSFR for galaxies with log₁₀M_BH/M_⊙> 7.0, where the CGM CIVcontent shows a clear dependence on galaxy sSFR but notM_BH. Our results do not indicate an obvious causal link between CGM CIVand the mass of the galaxy’s SMBH; however, through comparisons to the EAGLE, Romulus25, and IllustrisTNG simulations, we find that our sample is likely too small to constrain such causality. 

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4. Marvelous Metals: Surveying the Circumgalactic Medium of Simulated Dwarf Galaxies

   https://doi.org/10.3847/1538-4357/ae06a0  

   Piacitelli, Daniel R; Brooks, Alyson M; Christensen, Charlotte; Sanchez, N Nicole; Faerman, Yakov; Shen, Sijing; Cruz, Akaxia; Keller, Ben; Quinn, Thomas R; Wadsley, James (November 2025, The Astrophysical Journal)

   Abstract Dwarf galaxies are uniquely sensitive to feedback processes and known to experience substantial mass and metal loss from their disks. Here, we investigate the circumgalactic medium (CGM) of 64 isolated dwarf galaxies ( $6.0<\log (M_{*}/M_{\odot })<9.5$) atz= 0 from the Marvel-ous Dwarfs and Marvelous Massive Dwarfs simulations. Our galaxies produce column densities broadly consistent with current observations. We investigate these column densities in the context of mass and metal retention rates, and CGM physical properties. We find 48% ± 11% of all baryons withinR_200creside in the CGM, with ∼70% of CGM mass existing in a warm gas phase, 10^4.5 < T < 10^5.5K, that dominates beyondr/R_200c ∼ 0.5. The warm and cool (10^4.0 < T < 10^4.5K) gas phases each retain 5%–10% of metals formed by the dwarf galaxy. The significant fraction of mass and metals residing in the warm CGM phase provides an interpretation for the lack ofz ∼ 0 low ion detections beyondb/R_200c ∼ 0.5, as the majority of mass in this region exists in higher ions. We find a weak correlation between galaxy mass and total CGM metal retention despite the fraction of metals lost from the halo increasing from ∼10% to >40% toward lower masses. Our findings highlight the CGM (particularly its warm phase) as a key reservoir of mass and metals for dwarf galaxies across stellar masses, underscoring its importance in understanding the baryon cycle in the low-mass regime. Finally, we provide individual simulated galaxy properties and quantify the fraction of UV-observable mass to support future observational programs aimed at performing a metal budget around dwarf galaxies. 

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5. Thermal instability in the CGM of L ⋆ galaxies: testing ‘precipitation’ models with the FIRE simulations

   https://doi.org/10.1093/mnras/stab1281  

   Esmerian, Clarke J; Kravtsov, Andrey V; Hafen, Zachary; Faucher-Giguère, Claude-André; Quataert, Eliot; Stern, Jonathan; Kereš, Dušan; Wetzel, Andrew (June 2021, Monthly Notices of the Royal Astronomical Society)

   null (Ed.)

   ABSTRACT We examine the thermodynamic state and cooling of the low-z circumgalactic medium (CGM) in five FIRE-2 galaxy formation simulations of Milky Way-mass galaxies. We find that the CGM in these simulations is generally multiphase and dynamic, with a wide spectrum of largely non-linear density perturbations sourced by the accretion of gas from the intergalactic medium (IGM) and outflows from both the central and satellite galaxies. We investigate the origin of the multiphase structure of the CGM with a particle-tracking analysis and find that most of the low-entropy gas has cooled from the hot halo as a result of thermal instability triggered by these perturbations. The ratio of cooling to free-fall time-scales tcool/tff in the hot component of the CGM spans a wide range of ∼1−100 at a given radius but exhibits approximately constant median values of ∼5−20 at all radii 0.1Rvir < r < Rvir. These are similar to the ≈10−20 value typically adopted as the thermal instability threshold in ‘precipitation’ models of the ICM. Consequently, a one-dimensional model based on the assumption of a constant tcool/tff and hydrostatic equilibrium approximately reproduces the number density and entropy profiles of each simulation but only if it assumes the metallicity profile and temperature boundary condition taken directly from the simulation. We explicitly show that the tcool/tff value of a gas parcel in the hot component of the CGM does not predict its probability of subsequently accreting on to the central galaxy. This suggests that the value of tcool/tff is a poor predictor of thermal stability in gaseous haloes in which large-amplitude density perturbations are prevalent. 

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