2507.05354v1
JWST MIRI/MRS observations of hot molecular gas in an AGN host galaxy at Cosmic Noon
First listed 2025-07-07 | Last updated 2025-07-07
Abstract
Active Galactic Nuclei (AGN) are believed to play a central role in quenching star formation by removing or destroying molecular gas from host galaxies via radiation-pressure driven outflows and/or radio jets. Some studies of cold molecular gas in galaxies at Cosmic Noon ($z\sim2$) show that AGN have less cold gas ($<$100 K) compared to mass-matched star-forming galaxies. However, cold gas could also be shock-heated to warmer phases, detectable via H$_{2}$ transitions in the rest-frame near- and mid-infrared spectra. The Medium Resolution Spectrograph (MRS) of the Mid-infrared Instrument (MIRI) aboard JWST has opened a unique window to observe these emission lines in galaxies at Cosmic Noon. We present the first detection of hot molecular gas in cid_346, an X-ray AGN at $z\sim2.2$, via the H$_{2}$ ro-vibrational transition at 2.12 $μ$m. We measure a hot molecular gas mass of $\sim 8.0 \times 10^{5}$ M$_{\odot}$, which is $\sim 10^{5}-10^{6}$ times lower than the cold molecular gas mass. cid_346 is located in an environment with extended gas structures and satellite galaxies. This is supported by detection of hot and cold molecular gas out to distances $>$10 kpc in MIRI/MRS and ALMA data, respectively and ancillary NIRCam imaging that reveals two satellite galaxies at distances of $\sim$0.4 arcsec (3.3 kpc) and $\sim$0.9 arcsec (7.4 kpc) from the AGN. Our results tentatively indicate that while the CO(3-2)-based cold gas phase dominates the molecular gas mass at Cosmic Noon, H$_{2}$ ro-vibrational transitions are effective in tracing hot molecular gas locally in regions that may lack CO emission.
Short digest
Using JWST/MIRI MRS, the authors detect ro‑vibrational H2 in the z≈2.2 X‑ray AGN cid_346, measuring 1‑0 S(1) (and S(0)) and inferring a hot H2 mass of ≈8×10^5 M⊙. They map hot molecular emission and CO(3‑2) to >10 kpc, and NIRCam imaging reveals two nearby satellites at ≈3.3 and 7.4 kpc, pointing to an interacting environment. The hot phase is 10^5–10^6× less massive than the cold reservoir, but the authors argue H2 ro‑vibrational lines effectively trace locally heated/shocked gas where CO may be faint. Ionized gas shows [O III] extension and a blue wing toward the SE, consistent with outflow activity shaping the multiphase medium.
Key figures to inspect
- Figure 1: Use the four context panels to place cid_346 on the star‑forming main sequence, above the local MBH–M* relation, and within the Fabian (2008) NH–λEdd outflowing regime—together arguing it can drive winds at Cosmic Noon.
- Figure 2: Compare the [O III] flux map and blue‑wing spectrum with the ALMA CO(3‑2) map/spectrum to judge the geometry and kinematics of the ionized outflow (SE extension) relative to the cold molecular gas.
- Figure 3: Inspect the 1‑0 S(1) and 1‑0 S(0) line fits (centroids, widths, and 95% flux windows) that underpin the hot‑H2 detection and mass estimate; check S/N and any velocity offset from systemic.
- Figure 4: Read the 1‑0 S(1)/1‑0 S(0) ratio versus Lbol placement of cid_346 against low‑z Seyferts to assess the likely excitation (thermal/shock vs fluorescent) in this source.
Discussion
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