SQuIGG E: Spatially resolved NIRSpec Pa alpha reveals that the most CO-luminous, z about0.7 post-starburst galaxies exhibit falling---but still active---star formation behind optically thick dust
astro-ph.GA
Submitted: 2026-09-25
Updated: 2026-09-25
Comments: 24 pages, 8 figures. Submitted to ApJ. See also Luo et al., submitted today. Comments welcome!
License: http://creativecommons.org/licenses/by/4.0/
The gist: One of the fundamental uncertainties in the study of galaxies at the interface between star formation and quiescence--post-starburst galaxies--is their instantaneous star formation rate.
Terminology
Abstract
One of the fundamental uncertainties in the study of galaxies at the interface between star formation and quiescence--post-starburst galaxies--is their instantaneous star formation rate. While these galaxies appear quiescent in the rest UV-optical, many of the youngest systems are highly CO luminous, implying dense molecular gas, and potentially star formation. However, their instantaneous star formation rates have proved elusive, as measurements with rest-optical emission lines or UV-to-IR SED fitting yield order-of-magnitude uncertainty. Here, we present JWST/NIRSpec G395M/170LP integral field spectroscopy of the three most CO-luminous massive galaxies in the SQuIGG E survey, spatially resolving Pa α /Br γ /Br β to map the dust-corrected star formation rate. We find that these galaxies host star formation rates of 27-80 M yr-1, though about30-40% of the emission may arise from non-star-forming ionization (AGN or shocks), implied by high [FeII]/Pa α in central spaxels. We also find effective A Paα about1 and individual about700 pc spaxels with A Paα about2, implying significant dust obscuration of nebular regions that contribute little to the rest-optical lines. These galaxies are not consistent with total quiescence; the measured star formation rates place these galaxies on or above the main sequence. However, their star formation rates are significantly lower (about0.5-1 dex) than the peak star formation rates inferred from spectrophotometric fitting. We propose that the CO luminous post-starburst phase represents the last gasp of star formation in galaxies on the rapid quenching pathway, and that dust-obscured star formation, outflows, and (speculatively) an uncertain CO-to-H2 conversion reconcile their gas exhaustion with observed timescales of fading.
Sources
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- Calibrating Photometric Mid-Infrared Star Formation Rates for JWST
- The Nature of Post-Starburst Galaxies: Real Deal or Masquerading Impostors?
- Quenching Through Tidal Gas Removal: Molecular Gas and Star Formation in Tidal Tails of z ~ 0.7 Post-Starburst Galaxies
- Molecular Gas Excitation in z ~ 0.7 Gas-Rich Post-starburst Galaxies from SQuIGGLE
- The Prime Focus Spectrograph Galaxy Evolution Survey
- LEGGOS I: The JWST LEGGOS Survey -- LEnsing and Galaxy Growth: Observing Substructures -- Unpacks the Nature of Clumpy Star Formation and Quenching in Gravitationally Lensed Galaxies beyond Cosmic Noon
- Excavating The Ruins: an Ancient $z=2.675$ Galaxy Which Formed in the First 500 Myr
- SQuIGG$\vec{L}$E: Buried star formation cannot explain the rapidly fading CO(2-1) luminosity in massive, $z\sim0.7$ post-starburst galaxies
- Unusually High Gas-to-Dust Ratios Observed in High-Redshift Quiescent Galaxies
- Cold gas in a post-starburst pair at z ~ 1.4: major mergers as a pathway to quenching in the HeavyMetal survey
- Gas outflows in two recently quenched galaxies at z = 4 and 7
- Star Formation and Nebular Attenuation from Pa alpha, Br alpha, and Br beta in Massive Dust-obscured Galaxies at Cosmic Noon using JWST
- FRESCO: Constraining Dust Attenuation and Star-Formation Rates of $z\sim 2$ Star-Forming Galaxies with JWST Paschen and Ground-Based Balmer Emission Line Observations
- RUBIES spectroscopically confirms the high number density of quiescent galaxies from $\mathbf{2<z<5}$
- Winding Back the Clock: Recent Star Formation Histories of Massive Quiescent Galaxies Are Consistent With Their Rapid Number Density Evolution Since $\mathbf{z\sim7}$
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