4.7 Article

CGM properties in VELA and NIHAO simulations; the OVI ionization mechanism: dependence on redshift, halo mass, and radius

Journal

MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY
Volume 484, Issue 3, Pages 3625-3645

Publisher

OXFORD UNIV PRESS
DOI: 10.1093/mnras/stz063

Keywords

methods: numerical; galaxies: evolution; galaxies: formation

Funding

  1. I-CORE Program of the PBC/ISF [1829/12, BSF 2014-273, PICS 2015-18, GIF I-1341-303.7/2016]
  2. NSF [AST-1405962]
  3. DFG/DIP grant [STE 1869/2-1 GE 625/17-1]
  4. Spanish postdoctoral fellowship 'Ayudas para la atraccion del talento investigador. Modalidad 2: jovenes investigadores, financiadas por la Comunidad deMadrid' [2017-T2/TIC-5592]
  5. Spanish Ministry of Economy and Competitiveness (MINECO) [AYA2016-75808-R]
  6. ERC Advanced Grant, STARLIGHT: Formation of the First Stars [339177]
  7. [ISF 124/12]

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We study the components of cool and warm/hot gas in the circumgalactic medium (CGM) of simulated galaxies and address the relative production of OVI by photoionization versus collisional ionization, as a function of halo mass, redshift, and distance from the galaxy halo centre. This is done utilizing two different suites of zoom-in hydro-cosmological simulations, VELA (6 haloes; z > 1) and NIHAO (18 haloes; to z = 0), which provide a broad theoretical basis because they use different codes and physical recipes for star formation and feedback. In all haloes studied in this work, we find that collisional ionization by thermal electrons dominates at high redshift, while photoionization of cool or warm gas by the metagalactic radiation takes over near z similar to 2. In haloes of similar to 10(12 )M(circle dot) and above, collisions become important again at z < 0.5, while photoionization remains significant down to z = 0 for less massive haloes. In haloes with M-v > 3 x 10(11) M-circle dot, at z similar to 0 most of the photoionized OVI is in a warm, not cool, gas phase (T less than or similar to 3 x 10(5) K). We also find that collisions are dominant in the central regions of haloes, while photoionization is more significant at the outskirts, around R-v, even in massive haloes. This too may be explained by the presence of warm gas or, in lower mass haloes, by cool gas inflows.

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