The GOLIATH Survey: OVI Absorption Reveals CGM Evolution through the Starburst-to-Quiescent Transition in Massive Galaxies

arXiv:2607.19473 · astro-ph.GA · Submitted 2026-07-21 · Read on arXiv

Derick Flores, Rongmon Bordoloi, Jason Tumlinson, J. Christopher Howk, Nicolas Lehner, Mary Rickel, Benjamin Oppenheimer, Joseph Burchett, Ahmed Shaban, John O'Meara, Andrew Fox, J. Xavier Prochaska, Simon Xinlin Wu, Jack Higginson, Robert A. Simcoe

astro-ph.GA

Submitted: 2026-07-21

Comments: 29 pages, 10 Figures, 3 tables, Submitted to ApJ

Code: https://github.com/desihub/redrock

License: http://creativecommons.org/licenses/by/4.0/

The gist: We present the GOLIATH survey (Galaxies, Outflows, and the Lifecycle of Immense, Active, Transforming Halos), a study of the multiphase circumgalactic medium (CGM) of massive (M/M about 11), blue

Terminology

Abstract

We present the GOLIATH survey (Galaxies, Outflows, and the Lifecycle of Immense, Active, Transforming Halos), a study of the multiphase circumgalactic medium (CGM) of massive (M/M about 11), blue (u-r < 1.65) starburst and post-starburst galaxies at z about 0.43. This work characterizes the warm-hot CGM through OVI absorption in the inner halo (R/R vir at most 0.6) of these rare systems. Across the star-forming population, OVI column density rises by nearly 1 dex from M/M about 8 to about 11.5 and increases with specific star-formation rate (sSFR). Two GOLIATH galaxies with the highest sSFR show the strongest CGM OVI absorption (N O,VI[cm-2] 15). In the M/M = [11,12) inner-CGM region, massive star-forming galaxies exceed quiescent galaxies on average by a factor of about 3 in OVI column density and about 1.5 dex in CGM OVI mass ((M O, VI/M) about 7.3 versus about 5.8), with covering fractions roughly three times higher (62.5% versus 24% at N O,VI[cm-2] at least 14). The OVI line widths and column densities are consistent with feedback-driven radiative cooling, in which outflow shocks heat the CGM and the gas cools back through the OVI window; the short cooling time, t cool about 10 - 100 Myr, requires continuous replenishment by active feedback to sustain this reservoir. The residual OVI in quiescent systems may arise from ambient gas at the high-temperature end of the cooling curve. OVI thus traces feedback on short timescales and probes the star-forming--quiescent transition at M/M 11.

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