TY - JOUR
T1 - Does Circumgalactic O vi Trace Low-pressure Gas beyond the Accretion Shock? Clues from H i and Low-ion Absorption, Line Kinematics, and Dust Extinction
AU - Stern, Jonathan
AU - Faucher-Giguere, Claude André
AU - Hennawi, Joseph F.
AU - Hafen, Zachary
AU - Johnson, Sean D.
AU - Fielding, Drummond
N1 - Funding Information:
S. D. J. is supported by a NASA Hubble Fellowship (HST-HF2-51375.001-A).
Funding Information:
We thank the anonymous referee for a thorough report that significantly improved the paper. We also wish to thank Matthew McQuinn and Hsiao-Wen Chen for reading and sending insightful comments on a draft version of this manuscript. We thank MatthewMcQuinn also for providing the NNeVIII/NOVI ratios in the high-pressure scenario. J. S. thanks J. X. Prochaska, William Mathews, Amiel Sternberg, Yakov Faerman, Ben Oppenheimer, Avishai Dekel, Frank van den Bosch, and Jose Oñorbe for useful discussions. J. S. acknowledges support from the Alexander von Humboldt Foundation in the form of the Humboldt Postdoctoral Fellowship. The Humboldt Foundation is funded by the German Federal Ministry for Education and Research. C.-A. F.-G. and Z. H. were supported by NSF through grants AST-1412836, AST-1517491, AST-1715216, and CAREER award AST-1652522; by NASA through grant NNX15AB22G; by STScI through grants HST-GO-14681.011, HST-GO-14268.022-A, and HST-AR-14293.001-A; and by a Cottrell Scholar Award from the Research Corporation for Science Advancement.
PY - 2018/10/1
Y1 - 2018/10/1
N2 - Large O vi columns are observed around star-forming low-redshift galaxies, with a dependence on impact parameter indicating that most particles reside beyond half the halo virial radius (). In order to constrain the nature of the gas traced by , we analyze additional observables of the outer halo, namely to O vi column ratios of 1-10, an absence of low-ion absorption, a mean differential extinction of , and a linear relation between the O vi column and the O VI velocity width. We contrast these observations with two physical scenarios: (1) O vi traces high-pressure () collisionally ionized gas cooling from a virially shocked phase, and (2) O vi traces low-pressure () gas beyond the accretion shock, where the gas is in ionization and thermal equilibrium with the UV background. We demonstrate that the high-pressure scenario requires multiple gas phases to explain the observations and a large deposition of energy at to offset the energy radiated by the cooling gas. In contrast, the low-pressure scenario can explain all considered observations with a single gas phase in thermal equilibrium, provided that the baryon overdensity is comparable to the dark-matter overdensity and that the gas is enriched to with an ISM-like dust-to-metal ratio. The low-pressure scenario implies that O vi traces a cool flow with a mass flow rate of , comparable to the star formation rate of the central galaxies. The O vi line widths are consistent with the velocity shear expected within this flow. The low-pressure scenario predicts a bimodality in absorption line ratios at , due to the pressure jump across the accretion shock.
AB - Large O vi columns are observed around star-forming low-redshift galaxies, with a dependence on impact parameter indicating that most particles reside beyond half the halo virial radius (). In order to constrain the nature of the gas traced by , we analyze additional observables of the outer halo, namely to O vi column ratios of 1-10, an absence of low-ion absorption, a mean differential extinction of , and a linear relation between the O vi column and the O VI velocity width. We contrast these observations with two physical scenarios: (1) O vi traces high-pressure () collisionally ionized gas cooling from a virially shocked phase, and (2) O vi traces low-pressure () gas beyond the accretion shock, where the gas is in ionization and thermal equilibrium with the UV background. We demonstrate that the high-pressure scenario requires multiple gas phases to explain the observations and a large deposition of energy at to offset the energy radiated by the cooling gas. In contrast, the low-pressure scenario can explain all considered observations with a single gas phase in thermal equilibrium, provided that the baryon overdensity is comparable to the dark-matter overdensity and that the gas is enriched to with an ISM-like dust-to-metal ratio. The low-pressure scenario implies that O vi traces a cool flow with a mass flow rate of , comparable to the star formation rate of the central galaxies. The O vi line widths are consistent with the velocity shear expected within this flow. The low-pressure scenario predicts a bimodality in absorption line ratios at , due to the pressure jump across the accretion shock.
KW - galaxies: halos
KW - intergalactic medium
KW - quasars: absorption lines
UR - http://www.scopus.com/inward/record.url?scp=85054851294&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=85054851294&partnerID=8YFLogxK
U2 - 10.3847/1538-4357/aac884
DO - 10.3847/1538-4357/aac884
M3 - Article
AN - SCOPUS:85054851294
VL - 865
JO - Astrophysical Journal
JF - Astrophysical Journal
SN - 0004-637X
IS - 2
M1 - 91
ER -