The Nature of CO Emission From z~6 Quasars
Desika Narayanan (1), Yuexing Li (2), Thomas J. Cox (2), Lars, Hernquist (2), Philip Hopkins (2), Sukanya Chakrabarti (2), Romeel Dave (1),, Tiziana Di Matteo (3), Liang Gao (4), Craig Kulesa (1), Brant Robertson (5),, Christopher Walker (1) ((1) Arizona, (2) CfA

TL;DR
This study models CO emission in z~6 quasars using cosmological simulations, revealing how merger-driven processes influence CO excitation, morphology, and line widths, and how these relate to host galaxy properties.
Contribution
It introduces a combined approach of non-LTE radiative transfer and merger-driven galaxy formation models to explain CO emission characteristics in high-redshift quasars.
Findings
CO emission peaks between J=5-8 due to dense nuclear gas.
Quasar CO morphology often shows multiple emission peaks.
Line widths depend on sightline orientation and halo circular velocity.
Abstract
We investigate the nature of CO emission from z~6 quasars by combining non-LTE radiative transfer calculations with merger-driven models of z~6 quasar formation that arise naturally in LCDM cosmological simulations. We consider four model quasars formed in 10^12-10^13 M_sun halos from different merging histories. Our main results follow. Owing to massive starbursts and funneling of dense gas into the nuclear regions of merging galaxies, the CO is highly excited and the flux density peaks between J=5-8. The CO morphology of z~6 quasars often exhibits multiple emission peaks which arise from H2 concentrations which have not yet fully coalesced. Quasars at z~6 display a large range of sightline dependent line widths such that the lines are narrowest when the rotating H2 gas associated with the quasar is viewed face-on (when L_B is largest), and broadest when the gas is seen edge-on (when…
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Taxonomy
TopicsGalaxies: Formation, Evolution, Phenomena · Astrophysics and Star Formation Studies · Stellar, planetary, and galactic studies
