TY - JOUR
T1 - CGM properties in VELA and NIHAO simulations; the OVI ionization mechanism
T2 - Dependence on redshift, halo mass, and radius
AU - Roca-Fàbrega, S.
AU - Dekel, A.
AU - Faerman, Y.
AU - Gnat, O.
AU - Strawn, C.
AU - Ceverino, D.
AU - Primack, J.
AU - Macciò, A. V.
AU - Dutton, A. A.
AU - Prochaska, J. X.
AU - Stern, J.
N1 - Funding Information:
We would like to thank Amiel Sternberg for his valuable comments which helped to improve the manuscript. This work was partly supported by the grants ISF 124/12, I-CORE Program of the PBC/ISF 1829/12, BSF 2014-273, PICS 2015-18, GIF I-1341-303.7/2016, NSF AST-1405962, and by DFG/DIP grant STE 1869/2-1 GE 625/17-1. SFR acknowledges support from a Spanish postdoctoral fellowship ‘Ayudas para la atracción del talento investigador. Modalidad 2: jóvenes investigadores, financiadas por la Comunidad de Madrid’ under grant number 2017-T2/TIC-5592. SRF acknowledges financial support from the Spanish Ministry of Economy and Competitiveness (MINECO) under grant number AYA2016-75808-R. The VELA simulations were performed at the National Energy Research Scientific Computing Center (NERSC) at Lawrence Berkeley National Laboratory, and at NASA Advanced Supercomputing (NAS) at NASA Ames Research Center. DC has been funded by the ERC Advanced Grant, STARLIGHT: Formation of the First Stars (project number 339177). NIHAO simulations were carried out on the High Performance Computing resources at New York University Abu Dhabi; on the theo cluster of the Max-Planck-Institut fuer Astronomie and on the hydra clusters at the Rechenzentrum in Garching.
Publisher Copyright:
© 2019 The Author(s).
PY - 2019/4/11
Y1 - 2019/4/11
N2 - 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 ∼ 2. In haloes of ∼1012 M 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 Mv > 3 × 1011 M, at z ∼ 0 most of the photoionized OVI is in a warm, not cool, gas phase (T 3 × 105 K). We also find that collisions are dominant in the central regions of haloes, while photoionization is more significant at the outskirts, around Rv, even in massive haloes. This too may be explained by the presence of warm gas or, in lower mass haloes, by cool gas inflows.
AB - 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 ∼ 2. In haloes of ∼1012 M 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 Mv > 3 × 1011 M, at z ∼ 0 most of the photoionized OVI is in a warm, not cool, gas phase (T 3 × 105 K). We also find that collisions are dominant in the central regions of haloes, while photoionization is more significant at the outskirts, around Rv, even in massive haloes. This too may be explained by the presence of warm gas or, in lower mass haloes, by cool gas inflows.
KW - Galaxies: evolution
KW - Galaxies: formation
KW - Methods: numerical
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U2 - 10.1093/mnras/stz063
DO - 10.1093/mnras/stz063
M3 - Article
AN - SCOPUS:85067019874
SN - 0035-8711
VL - 484
SP - 3625
EP - 3645
JO - Monthly Notices of the Royal Astronomical Society
JF - Monthly Notices of the Royal Astronomical Society
IS - 3
ER -