2024A&A...692A.161B


Query : 2024A&A...692A.161B

2024A&A...692A.161B - Astronomy and Astrophysics, volume 692A161 (2024/12-1)

Genuine Retrieval of the AGN Host Stellar Population (GRAHSP).

BUCHNER J., STARCK H., SALVATO M., NETZER H., IGO Z., LALOUX B., GEORGAKAKIS A., GAUGER I., OLECHOWSKA A., LOPEZ N., SHANKAR S.D., LI J., NANDRA K. and MERLONI A.

Abstract (from CDS):

Context. The assembly and co-evolution of super-massive black holes (SMBHs) and their host galaxy stellar population is one of the key open questions in modern galaxy evolution. Observationally constraining this question is challenging. Important parameters of galaxies, such as the stellar mass (M⋆) and star formation rate (SFR), are inferred by modeling the spectral energy distribution (SED), with templates constructed on the basis of various assumptions on stellar evolution. In the case of galaxies triggering SMBH activity, the active galactic nucleus (AGN) contaminates the light of the host galaxy at all wavelengths, hampering inferences of host galaxy parameters. Underestimating the AGN contribution due to incomplete AGN templates results in a systematic overestimation of the stellar mass, biasing our understanding of AGN and galaxy co-evolution. This challenge has gained further attention with the advent of sensitive wide-area surveys with millions of newly detected luminous AGN, including those by eROSITA, Euclid, and LSST.
Aims. We aim to robustly estimate the accuracy, bias, scatter, and uncertainty of AGN host galaxy parameters, including stellar masses, and improve these measurements relative to previously used techniques.
Methods. This work makes two important contributions. Firstly, we present a new SED fitting code, GRAHSP, with an AGN model composed of a flexible power-law continuum with empirically determined broad and narrow lines and a FeII forest component, a flexible infrared torus that can reproduce the diverse dust temperature distributions, and appropriate attenuation on the galaxy and AGN light components. We verify that this model reproduces published X-ray to infrared SEDs of AGN to better than 20% accuracy. A fully Bayesian fit includes uncertainties in the model and the data, making the inference highly robust. The model is constrained with a fast nested sampling inference procedure supporting the many free model parameters. Secondly, we created a benchmark photometric data set where optically selected pure quasars are paired with non-AGN pure galaxies at the same redshift. Their photometry flux is summed into a hybrid (Chimera) object but with known galaxy and AGN properties. Based on this data-driven benchmark, true and retrieved stellar masses, SFR, and AGN luminosities can be compared, allowing for the evaluation and quantification of biases and uncertainties inherent in any given SED fitting methodology.
Results. The Chimera benchmark, which we release with this paper, shows that previous codes systematically overestimate M⋆ and SFR by 0.5 dex with a wide scatter of 0.7 dex at AGN luminosities above 1044 erg s–1. In 20% of cases, the estimated error bars lie completely outside a 1 dex-wide band centreed around the true value, which we consider an outlier. In contrast, GRAHSP shows no measurable bias on M⋆ and SFR, with an outlier fraction of only about 5%. GRAHSP also estimates more realistic uncertainties.
Conclusions. Unbiased characterization of galaxies hosting AGN enables characterization of the environmental conditions conducive to black hole growth, whether star formation is suppressed at high black hole activity, and identifying the mechanisms that prevent overluminous AGN relative to the host galaxy mass. It can also shed light on the long-standing questions of whether AGN obscuration is primarily an orientation effect or related to phases in galaxy evolution.

Abstract Copyright: © The Authors 2024

Journal keyword(s): methods: data analysis - techniques: photometric - galaxies: general - galaxies: nuclei - quasars: general - galaxies: Seyfert

Simbad objects: 42

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Number of rows : 42
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 LEDA 1790 Sy1 00 29 13.7012449608 +13 16 03.947778264   15.70 15.41     ~ 474 0
2 ESO 350-38 Sy2 00 36 52.489 -33 33 17.23   14.31 14.41 13.49   ~ 450 0
3 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 12317 1
4 Mrk 1502 Sy1 00 53 34.9331107632 +12 41 35.929269132   14.41 14.03     ~ 1242 1
5 LEDA 3237 Sy1 00 54 52.1183662680 +25 25 38.983241532     15.42     ~ 421 0
6 ESO 113-45 Sy1 01 23 45.7631533440 -58 48 20.808928944   14.08 13.83 13.34   ~ 965 0
7 NGC 863 Sy2 02 14 33.5604714720 -00 46 00.181845336   14.48 13.81 17.9   ~ 770 0
8 NAME Chandra Deep Field-South reg 03 32 28.0 -27 48 30           ~ 2282 1
9 MCG+01-12-009 Bla 04 33 11.0956735296 +05 21 15.619461552   15.72 15.05 10.08   ~ 2099 2
10 Z 395-23 Sy1 05 16 11.4092471904 -00 08 59.157166920   14.30 13.92     ~ 953 1
11 Ton 951 Sy1 08 47 42.4485615096 +34 45 04.482515304   14.83 14.50     ~ 487 0
12 Mrk 110 Sy1 09 25 12.8479065576 +52 17 10.386311208   16.82 16.41     ~ 681 1
13 NGC 3227 Sy1 10 23 30.5765149296 +19 51 54.282206700   12.61 11.79     ~ 1807 2
14 NAME Lockman Hole reg 10 45 00.0 +58 00 00           ~ 910 0
15 NGC 3516 Sy1 11 06 47.4632200800 +72 34 07.298374656   13.12 12.40     ~ 1638 0
16 2MASS J11135466+1244390 Sy1 11 13 54.6593262552 +12 44 39.060865860   21.59 20.74 19.00   ~ 40 0
17 IRAS 11119+3257 Sy1 11 14 38.8902542640 +32 41 33.483258276   19.22 17.96     ~ 165 0
18 NGC 4051 Sy1 12 03 09.6101337312 +44 31 52.682601288   11.08 12.92 9.94   ~ 2270 1
19 NGC 4151 Sy1 12 10 32.5759813872 +39 24 21.063527532   12.18 11.48     ~ 3938 2
20 PB 3894 Sy1 12 14 17.6738687784 +14 03 13.182723144   14.46 14.19     ~ 873 0
21 3C 273 BLL 12 29 06.6998257176 +02 03 08.597629980   13.05 14.830 14.11   ~ 6022 1
22 Z 294-4 Sy1 12 56 14.2341182928 +56 52 25.238373852   14.68 13.84     ~ 2096 3
23 LEDA 3800210 Sy2 13 00 05.3479083912 +16 32 14.758987848   17.1 17.10     ~ 64 0
24 LEDA 45656 Sy1 13 09 47.0031619008 +08 19 48.212362524   16.04 15.89     ~ 412 0
25 PKS 1345+12 Sy2 13 47 33.36161873 +12 17 24.2398927   19.28 18.44 15.718   ~ 652 2
26 Z 336-28 Sy1 13 53 03.4348964112 +69 18 29.410910460   15.15 14.46     ~ 812 1
27 LEDA 51016 Sy1 14 17 00.8224797456 +44 56 06.336360024   16.93 16.63     ~ 275 0
28 NGC 5548 Sy1 14 17 59.5400291832 +25 08 12.603122268   14.35 13.73     ~ 2895 0
29 Z 296-15 Sy1 14 36 22.0820611632 +58 47 39.394934844   14.19 13.79     ~ 592 0
30 NGC 5728 Sy2 14 42 23.8918506576 -17 15 11.240783784   14.34 13.40     ~ 679 1
31 Mrk 290 Sy1 15 35 52.4031021552 +57 54 09.515660508   15.55 15.27     ~ 575 0
32 Z 195-3 Sy1 15 59 09.6231720696 +35 01 47.561352852   15.69 15.06     ~ 346 0
33 Mrk 876 Sy1 16 13 57.1795021224 +65 43 09.952685328   16.03 15.49     ~ 620 0
34 LEDA 2817004 Sy2 16 18 09.4114 +01 39 20.951           ~ 44 1
35 8C 1704+608 Bla 17 04 41.3742408840 +60 44 30.520617000   15.65 15.40 15.30   ~ 782 1
36 7C 1821+6419 Sy1 18 21 57.2130271440 +64 20 36.221312076   14.23 14.24     ~ 632 1
37 2C 1590 BLL 18 45 37.622 +09 53 44.74           ~ 82 1
38 Mrk 509 Sy1 20 44 09.7504483224 -10 43 24.727155528   13.35 13.12 10.7   ~ 1370 0
39 Z 495-18 Sy1 22 42 39.3363009144 +29 43 31.302092640   14.86 14.16     ~ 748 1
40 NGC 7469 Sy1 23 03 15.6 +08 52 26 12.60 13.00 12.34     ~ 2253 3
41 MCG-02-58-022 Sy1 23 04 43.4776098480 -08 41 08.629476864   16.20 15.91 9.4   ~ 481 1
42 4C -01.61 BLL 23 51 56.1224889360 -01 09 13.315371768   16.83 16.59     ~ 380 1

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