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September 20, 2025Monthly Notices of the Royal Astronomical Society4 citationsOpen Access

The halo mass dependence of physical and observable properties in the circumgalactic medium at z = 0

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ACAndrew W. S. CookFVFreeke van de VoortRPRüdiger Pakmor

Key Points

  • Median temperature and metallicity in the circumgalactic medium increase with halo mass, revealing significant patterns.
  • The study identifies that O vi and H i represent the extremes of temperature and density in the circumgalactic medium.
  • Cosmological simulations align closely with observational data for H i and C iv, suggesting reliability in mass range studied.
  • Discrepancies in O vi and Mg ii column densities indicate the need for more observational constraints, especially in lower mass halos.

Abstract

Abstract We study the dependence of the physical and observable properties of the circumgalactic medium on its halo mass in 25 high resolution cosmological ‘zoom-in’ simulations from the Auriga suite. We focus on the current epoch (z = 0) and on halo masses of 10^10\, { M } M{₂₀₀{ ₂}} 10^12 M⊙ and stellar masses of 107 M⊙ ≤ M⋆ ≤ 1011 M⊙. The mass resolution of our simulations is 5. 4 × 103 M⊙. This work analyses the temperature, density, metallicity and radial velocity of these haloes and the column density of H i, Mg ii, Si ii, C iv and O vi. We find median temperature and metallicity increase with halo mass as expected. We find a larger scatter in temperature at higher halo masses, suggesting that the multiphase nature of the CGM is halo mass dependent. Our H i column densities show good agreement with observations at all radii. Mg ii and Si ii match observations between 0. 1R200c-0. 3R200c, but decrease steeply with radius. O vi column densities are underpredicted by our simulations for stellar masses between 109. 5 M⊙ ≤ M⋆ 1010. 2 M⊙ at large radii with reasonable agreement at 1011 M⊙. C iv column densities agree with observational detections above a halo mass of 109. 5M⊙. We find that O vi (H i) traces the highest (lowest) temperatures, and lowest (highest) density and metallicity. O vi (C iv) is photo-ionized (collisionally ionized) at low (high) halo masses with a transition to higher temperatures at 1011 M⊙. Our results demonstrate similarities and discrepancies between simulations of Milky Way-mass haloes and observations. They also show further observational constraints are needed in less massive haloes.

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Cite This Study

Cook et al. (2025) studied this question.

synapsesocial.com/papers/68d46fc631b076d99fa69aa8https://doi.org/10.1093/mnras/staf1537
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