Weekly issue

Week 33, 2026

Aug 10–12, 2026

Week 33, 2026 includes 2 curated papers, centered on JWST AGN, spectroscopy, LRD.

2608.10832v1

ATLAS. III. Dust Around Little Red Dots: Hydrogen Line Ratios beyond Dust-free Non-Case B Models

Tomokazu Kiyota, Masami Ouchi, Hiroto Yanagisawa, Makoto Ando, Yuichi Harikane, Yuta Kageura, Minami Nakane, Yurina Nakazato, Yoshiaki Ono, Yui Takeda

Theme match 3/5

Digest

This ATLAS installment measures broad Balmer decrements in 20 LRDs, comprising five JWST/NIRSpec high-redshift sources and 15 local analogues, with careful fits that account for absorption and blended neighboring lines. Broad Hα/Hβ spans 6–30, far above Case B; joint Balmer–Paschen Cloudy modeling shows that high density can explain one local LRD, but the other two systems with Paschen constraints require substantial additional extinction even after non-Case-B radiative-transfer effects are included. Because the narrow-line decrements do not imply comparably strong reddening, the paper places the obscuring dust near the broad-line region and argues that dust obscuration may occur in at least roughly half of LRDs, potentially as a lower-column counterpart to an AGN dusty torus.

Key figures to inspect

  • Figure 3. This is the population-level measurement that establishes the central anomaly: LRD broad Hα/Hβ ratios reach 6–30 and several exceed the maximum attainable in the dust-free Cloudy grid. It also places the high-redshift JWST sample, local LRDs, lower limits, and comparison SDSS AGNs on the same diagnostic.
  • Figure 5. The Balmer–Paschen diagnostic directly breaks the dust-versus-density degeneracy. Comparing the three Paschen-measured LRDs with the dust-free Cloudy grid and reddening vector shows why non-Case-B gas alone succeeds for only one source while others require extinction.
  • Figure 9. This figure connects the line-ratio inference to the available infrared evidence in the three local LRDs. Its comparison of inferred minimum broad-line attenuation, narrow-line attenuation, dust-template temperatures, and line widths supports dust associated with the compact broad-line-region environment rather than galaxy-scale reddening.
  • Figure 10. The concluding schematic distills the paper's physical interpretation: an LRD can retain visible broad lines while line-of-sight dusty material attenuates the broad-line and continuum emission. It provides the clearest visual synthesis of the proposed lower-column-density analogue of a classical AGN torus.

Tags

  • LRD

2608.08369v1

GATOS: Distinct Feedback Modes in AGN Central Regions Revealed by Spatially Resolved JWST Spectroscopy

Lulu Zhang, Chris Packham, Erin K. S. Hicks, Ismael García-Bernete, Almudena Alonso-Herrero, Ric I. Davies, Martin J. Ward, Daniel E. Delaney, Takuma Izumi, Dimitra Rigopoulou, Cristina Ramos Almeida, Omaira González-Martín, Rogemar A. Riffel, Claudio Ricci, Montserrat Villar-Martín, Francoise Combes, Miguel Pereira-Santaella, Sebastian F. Hoenig, Andrew J. Bunker, Peter G. Boorman, Enrica Bellocchi, Nancy A. Levenson, Santiago García-Burillo, Fergus R. Donnan, Anelise Audibert, Lindsay Fuller, Tanio Díaz-Santos, David J. Rosario

Theme match 3/5

Digest

Using JWST/MIRI MRS spectroscopy at 4–24 pc resolution, GATOS maps PAH bands alongside H₂ and ionized-gas diagnostics across the nuclei of five AGN spanning a broad luminosity range. The study finds that nuclear PAH suppression reflects two distinct feedback channels: AGN irradiation, which heats and ionizes PAHs before preferentially destroying smaller grains, and shock processing from jets or outflows, which preferentially removes ionized PAHs. Their coexistence explains the observed bimodality in PAH band ratios and helps reconcile conflicting PAH-based AGN results, while cautioning that PAH star-formation calibrations in AGN require feedback-aware treatment; the conclusions are based on a limited sample.

Key figures to inspect

  • Figure 1. This figure establishes the observational problem by comparing resolved 6.2, 7.7, and 11.3 μm PAH surface brightness with neon-based SFR surface density in the five AGN nuclei. It shows where the usual star-forming PAH–SFR calibration fails on parsec scales, motivating the feedback-based interpretation.
  • Figure 4. The central diagnostic figure links PAH 6.2/7.7 and 11.3/7.7 ratios to independent indicators of shock processing and AGN irradiation, while placing the measurements against star-forming spaxels and PAH models. It directly visualizes the two PAH-ratio regimes that underpin the paper’s claim of distinct radiative and kinetic feedback modes.
  • Figure 5. This alternate-diagnostic version of the PAH-ratio analysis tests the conclusion using [Fe II]/[Ar II] for shocks and [Ne V]/[Ne III] for AGN irradiation. It matters because it demonstrates that the feedback interpretation is not tied to a single choice of line-ratio proxy.
  • Figure 6. The schematic distills the paper’s bottom-line physical picture: irradiation leaves a population weighted toward larger, more ionized PAHs, whereas shocks preferentially destroy ionized PAHs and favor large, neutral survivors. It is the clearest synthesis of why mixed feedback modes can produce bimodal PAH ratios and complicate PAH-based SFR estimates near AGN.

Tags

  • JWST AGN
  • spectroscopy