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Active galactic nuclei-heated dust revealed in "little red dots"

I. Delvecchio, E. Daddi, B. Magnelli, D. Elbaz, M. Giavalisco, A. Traina, G. Lanzuisi, H. B. Akins, S. Belli, C. M. Casey, F. Gentile, C. Gruppioni, F. Pozzi, G. Zamorani

TL;DR

This paper uses a large, uniformly selected sample of 302 little red dots (LRDs) from JWST fields to perform a median stacking analysis with NIRCam, MIRI, and ALMA data. By fitting the median stacked spectral energy distribution with and without an AGN component, the authors find clear evidence for hot-dust emission consistent with AGN-heated dust, typically around $T\approx820$ K, and they infer that many LRDs host Compton-thick gas within the dust sublimation radius, explaining their X-ray faintness. The results suggest that more than half of LRDs contain AGN-heated dust, regardless of whether the optical/UV continuum is stellar- or AGN-dominated, while the ALMA upper limits constrain the cold dust content and support a scenario in which X-ray obscuration occurs in dust-free gas inside $R_{ m sub}$. The study highlights the heterogeneity of LRDs, reconciles their multiwavelength properties, and provides empirical benchmarks for AGN–galaxy co-evolution at $z\sim4$–$8$, though a full radiative-transfer treatment and deeper individual observations are needed to fully unravel formation channels of hot dust in these systems.

Abstract

Little red dots (LRDs) are a puzzling population of extragalactic sources whose origin is highly debated. In this {work}, we performed a comprehensive stacking analysis of NIRCam, MIRI, and ALMA images of a large and homogeneously selected sample of LRDs from multiple JWST Legacy fields. We report clear evidence of hot-dust emission in the median stacked spectral energy distribution (SED) that features a rising near-infrared continuum up to rest-frame $λ_{\rm rest}$$\sim$ 3$μ$m, which is best explained by a standard dusty active galactic nucleus (AGN) structure. Although LRDs are likely to be a heterogeneous population, our findings suggest that most ($\gtrsim$50 %) LRDs show AGN-heated dust emission, regardless of whether the optical and ultraviolet (UV) continua are stellar or AGN-dominated. In either case, the best-fit dusty-AGN SED, combined with the lack of X-ray detection in the deep Chandra stacks, suggests that Compton-thick ($N_{\rm H}$$>$3$\times$10$^{24}$ cm$^{-2}$) gas obscuration is common, and likely confined within the dust sublimation radius ($R$$_{\rm sub}$$\sim$0.1 pc). Therefore, we argue that AGN-heated dust does not directly obscure either the optical-UV continuum or the broad-line region emission, in order to explain the observed blue UV slopes and prominent Balmer features. While a gas-dust displacement is in line with several models, the formation scenario (in-situ or ex-situ) of this pre-enriched hot dust remains unclear.

Active galactic nuclei-heated dust revealed in "little red dots"

TL;DR

This paper uses a large, uniformly selected sample of 302 little red dots (LRDs) from JWST fields to perform a median stacking analysis with NIRCam, MIRI, and ALMA data. By fitting the median stacked spectral energy distribution with and without an AGN component, the authors find clear evidence for hot-dust emission consistent with AGN-heated dust, typically around K, and they infer that many LRDs host Compton-thick gas within the dust sublimation radius, explaining their X-ray faintness. The results suggest that more than half of LRDs contain AGN-heated dust, regardless of whether the optical/UV continuum is stellar- or AGN-dominated, while the ALMA upper limits constrain the cold dust content and support a scenario in which X-ray obscuration occurs in dust-free gas inside . The study highlights the heterogeneity of LRDs, reconciles their multiwavelength properties, and provides empirical benchmarks for AGN–galaxy co-evolution at , though a full radiative-transfer treatment and deeper individual observations are needed to fully unravel formation channels of hot dust in these systems.

Abstract

Little red dots (LRDs) are a puzzling population of extragalactic sources whose origin is highly debated. In this {work}, we performed a comprehensive stacking analysis of NIRCam, MIRI, and ALMA images of a large and homogeneously selected sample of LRDs from multiple JWST Legacy fields. We report clear evidence of hot-dust emission in the median stacked spectral energy distribution (SED) that features a rising near-infrared continuum up to rest-frame 3m, which is best explained by a standard dusty active galactic nucleus (AGN) structure. Although LRDs are likely to be a heterogeneous population, our findings suggest that most (50 %) LRDs show AGN-heated dust emission, regardless of whether the optical and ultraviolet (UV) continua are stellar or AGN-dominated. In either case, the best-fit dusty-AGN SED, combined with the lack of X-ray detection in the deep Chandra stacks, suggests that Compton-thick (310 cm) gas obscuration is common, and likely confined within the dust sublimation radius (0.1 pc). Therefore, we argue that AGN-heated dust does not directly obscure either the optical-UV continuum or the broad-line region emission, in order to explain the observed blue UV slopes and prominent Balmer features. While a gas-dust displacement is in line with several models, the formation scenario (in-situ or ex-situ) of this pre-enriched hot dust remains unclear.

Paper Structure

This paper contains 19 sections, 6 figures, 4 tables.

Figures (6)

  • Figure 1: Redshift distribution of the final LRD sample (dashed black histogram) used in this work. The full sample is split by field (CEERS, GOODSS, PRIMER-COSMOS, PRIMER-UDS), as highlighted by the colored open histograms, while filled histograms mark the corresponding subset with spectroscopic redshifts.
  • Figure 2: Median stacked cutouts (3$^{\prime \prime}$$\times$3$^{\prime \prime}$) of LRDs in NIRCam (7; from f090w to f444w), MIRI (8; from f560w to f2550w), and ALMA/B6 (1.1 mm) bands. All NIRCam and MIRI images have the same pixel size (0.06$^{\prime \prime}$). Each cutout reports the corresponding PSF's FWHM (white circle) and the number of stacked sources. To ease visualization, a smoothing with a Gaussian kernel was applied to all MIRI images, with a larger radius for larger FWHM: two pixels for f560w, f770w, and f1000w; three pixels for f1280w and f1500w; four pixels for f1800w and f2100w, and five pixels for f2550w. The stacked ALMA/B6 image was obtained in the $uv$-plane and imaged at 0.1$^{\prime \prime}$/px scale. Except for MIRI/f2550w and ALMA/B6, all other median stacks lead to a S/N$>$3 detection.
  • Figure 3: Best SED fits obtained with CIGALE on the stacked photometry (open circles) at $z$=6.2. Top panel: Fit including only galaxy templates. Middle panel: Fit including both galaxy and AGN templates. The fitting from the AGN run is strongly favored based on $\chi^2$ arguments and ALMA constraints. Bottom panel: Decomposition of the AGN-dust template (dashed red) in three multi-temperature graybody models (dot-dashed lines). The normalized BH-star SED Naidu+2025 is overlaid for comparison (green) and not included in the SED fitting. Details are given in Section \ref{['sedfitting']}.
  • Figure 4: Comparison between our rest-frame median stacked SED (open gray circles) and other literature spectra or SEDs of LRDs. All fluxes are normalized to the rest-frame 1 $\mu$m flux density. We show the stacked SEDs from Kokorev+2024; Akins+2025 and Casey+2024 (Casey+2024; both AGN and galaxy fits as red and blue dot-dashed lines, respectively). Other single LRD SEDs include: CAPER-z9 ($z$=9.288; Taylor+2025); A2744-45924 ($z$=4.4655; Labbe+2024); RUBIES-BLAGN-1 ($z$=3.1034; Wang+2025); the BiRD ($z$=2.33; Loiacono+2025); the Rosetta Stone (or GN 280754; $z$=2.26; Juodzbalis+2024a) and The Cliff ($z$=3.55; deGraaff+2025).
  • Figure 5: Sketch of the proposed hot AGN-dust scenario, both for stellar-dominated (left) and AGN-dominated (right) optical and/or UV continuum.
  • ...and 1 more figures