2026A&A...706A.100R


Query : 2026A&A...706A.100R

2026A&A...706A.100R - Astronomy and Astrophysics, volume 706A100 (2026/2-1)

Silicate emission in a type-2 quasar: JWST/MIRI constraints on torus geometry and radiative feedback.

RAMOS ALMEIDA C., ASENSIO RAMOS A., WESTERDORP PLAZA C., GARCIA-BERNETE I., LOPEZ-RODRIGUEZ E., HONIG S., AUDIBERT A., GARCIA-BURILLO S., PEREIRA-SANTAELLA M., DONNAN F., ALONSO-HERRERO A., GONZALEZ-MARTIN O., LEVENSON N., RIGOPOULOU D., TADHUNTER C. and SPERANZA G.

Abstract (from CDS):

Type-2 quasars (QSO2s) are active galactic nuclei (AGN) seen through a significant amount of dust and gas that obscures the central supermassive black hole and the broad line region. Despite this, recent mid-infrared spectra of the central 0.5-1.1 kpc of five QSO2s at z ∼ 0.1, obtained with the MRS module of JWST/MIRI, revealed 9.7, 18, and 23 μm silicate features in emission in two of them. This indicates that the high angular resolution of JWST/MIRI now allows us to peer into their nuclear region, exposing some of the directly illuminated dusty clouds that produce silicate emission. To test this, we fit the nuclear mid-infrared spectrum of the QSO2 with the strongest silicate features, J1010, with two different sets of torus models implemented in an updated version of the Bayesian tool BayesClumpy. These are the CLUMPY and the CAT3D-WIND models. The CAT3D-WIND model is preferred by the observations based on the marginal likelihood and fit residuals, although the two torus models successfully reproduce the spectrum by means of intermediate covering factors (C$ _{\mathrm{T}} = 0.45\pm^{0.26}_{0.18} $ and C$ _{\mathrm{T}} = 0.66\pm^{0.16}_{0.17} $ for the CLUMPY and CAT3D-WIND models) and low inclinations ($ \mathrm{i} = 50{\circ}\pm^{8{\circ}}_{9{\circ}} $ and $ \mathrm{i} = 13{\circ}\pm^{7{\circ}}_{6{\circ}} $). Indeed, four of the five QSO2s with JWST/MIRI observations, including J1010, are in the blowout or “forbidden” region of the Eddington ratio-column density diagram, indicating that they are actively clearing gas and dust from their nuclear regions, leading to reduced covering factors. This is in contrast with Seyfert 2 galaxies observed with JWST, which are in the “permitted” regions of the diagram and show 9.7 μm silicate features in absorption. This supports a scenario where the more luminous the AGN and the higher their Eddington ratio, the lower the torus covering factor, driven by radiation pressure on dusty gas.

Abstract Copyright: © The Authors 2026

Journal keyword(s): galaxies: active - galaxies: evolution - galaxies: ISM - galaxies: nuclei - quasars: general

Simbad objects: 15

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Number of rows : 15
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 Mrk 1502 Sy1 00 53 34.9331107632 +12 41 35.929269132   14.41 14.03     ~ 1242 1
2 IRAS 05563-3820 Sy1 05 58 02.0566707456 -38 20 04.452162288   16.05 14.98 11.6   ~ 249 1
3 MCG+05-23-016 Sy1 09 34 06.3274325304 +27 20 59.506582524   16       ~ 76 0
4 MCG-05-23-016 Sy2 09 47 40.1332188528 -30 56 55.960779696   14.10 13.69 12.44   ~ 611 0
5 2MASS J10104334+0612013 Sy2 10 10 43.3642763928 +06 12 01.383491808   18.45 17.87     ~ 42 1
6 LEDA 3469502 Sy2 11 00 12.3868783440 +08 46 16.287755052   17.84 17.38     ~ 42 1
7 Z 294-4 Sy1 12 56 14.2341182928 +56 52 25.238373852   14.68 13.84     ~ 2096 3
8 SDSS J135646.10+102609.0 Sy2 13 56 46.106 +10 26 09.09   18.90 18.11     ~ 95 0
9 NGC 5506 Bla 14 13 14.8761010056 -03 12 27.556909272   15.25 14.38     ~ 1173 1
10 NAME Teacup AGN Sy2 14 30 29.8820644560 +13 39 12.007458684   16.89 16.64     ~ 82 0
11 NGC 5728 Sy2 14 42 23.8918506576 -17 15 11.240783784   14.34 13.40     ~ 679 1
12 LEDA 1270205 Sy2 15 09 04.2181476552 +04 34 41.766157380   18.90 18.27     ~ 30 0
13 ESO 137-34 Sy2 16 35 14.114 -58 04 48.10   12.20   10.84 11.6 ~ 165 0
14 NGC 7172 Sy2 22 02 01.897 -31 52 11.60   12.72 13.61 11.15 25.10 ~ 572 2
15 NGC 7319 Sy2 22 36 03.602 +33 58 33.18   14.57 13.53 12.65   ~ 325 0

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