2025A&A...700A.168G


Query : 2025A&A...700A.168G

2025A&A...700A.168G - Astronomy and Astrophysics, volume 700A168 (2025/8-1)

Milliarcsecond astrometric oscillations in active galactic nuclei as a precursor of multi-messenger gravitational wave events.

GURVITS L.I., POLNAREV A.G., FREY S., TITOV O., OSETROVA A.A., FAN X. and MELNIKOV A.

Abstract (from CDS):

Context. The existence of supermassive black hole binaries (SMBHBs) is predicted by various cosmological and evolutionary scenarios for active galactic nuclei. These objects are considered as contributors into the gravitational wave (GW) background, as well as emitters of discrete GW bursts. Yet, SMBHBs remain a rather elusive class of extragalactic objects.
Aims. Previously we have identified the quasar J2102+6015 as a potential SMBHB system on the basis of absolute astrometric very long baseline interferometry (VLBI) monitoring. Here we present another case, the source J0204+1514, exhibiting a similar oscillating astrometric pattern. Our aim is to analyse the evolution of SMBHBs as generators of GW and provide a physical 'multi-messenger' link between astrometric manifestation in the radio domain and GW emission.
Methods. We analysed the available archive VLBI astrometry data that resulted in the detection of astrometric oscillations in the source J0204+1514. We assume these oscillations to be manifestations of orbital motion in a binary system. We estimated the parameters of the suspected SMBHB in this source and applied basic theoretical models to project its evolution towards coalescence. We also developed a simplified 'toy' model of SMBHBs consistent with the discovered astrometric oscillations and made quantitative predictions of GW emission of such sources using the case of J0204+1514 as an example potentially applicable to other SMBHBs.
Results. We provide observational evidence of astrometric oscillations in the source J0204+1514. As an ad hoc result, we also provide a re-assessed estimate of the redshift of J2102+6015, z = 1.42. A toy model of the object containing a SMBHB with parameters consistent with the observed astrometric oscillations of the source J0204+1514 as an example enables us to consider GW emission as the cause of the system's orbital evolution.
Conclusions. We conclude that astrometric VLBI monitoring has an appreciable potential for future detections of SMBHBs that could become multi-messenger targets for both electromagnetic (in radio domain) and GW astronomy. To outline the contours of a future physical model connecting SMBHB evolution with detectable GW manifestations, we present a toy model and, as an example, apply this toy model to the astrometrically oscillating source J0204+1514 described in this work. We also provide a justification for aiming future space-borne VLBI missions at direct imaging of SMBHBs as a synergistic contribution into future multi-messenger studies involving prospective GW facilities.

Abstract Copyright: © The Authors 2025

Journal keyword(s): gravitational waves - techniques: interferometric - astrometry - quasars: supermassive black holes - quasars: individual: J2102+6015 - quasars: individual: J2236+2828

Simbad objects: 27

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Number of rows : 27
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 SDSS J005113.92+002047.0 rG 00 51 13.9347375336 +00 20 47.171347080           ~ 10 0
2 4C 15.05 Bla 02 04 50.41389294 +15 14 11.0436097   21.9 21.00 21.00   ~ 426 1
3 3C 66A BLL 02 22 39.6114771888 +43 02 07.799534304   15.71 15.21 14.5   ~ 942 2
4 Z 538-57 Sy1 02 23 11.41124925 +42 59 31.3853324   15.71 14.81     ~ 582 2
5 ICRF J040549.2+380332 SyG 04 05 49.26287155 +38 03 32.2348497   18.5 18.5     ~ 187 3
6 ASASSN -20qc SN? 04 13 02.379 -53 04 21.80           ~ 16 0
7 NGC 1566 Sy1 04 20 00.3968473248 -54 56 16.624708764 10.29 10.19 9.73 9.21 10.1 ~ 1051 2
8 3C 186 QSO 07 44 17.4720658920 +37 53 17.250697320   17.5 18.14 17.2   ~ 339 1
9 LEDA 3095775 Sy1 07 52 17.8468408368 +19 35 42.281437848   16.35 16.09     ~ 73 1
10 Z 59-39 Sy2 08 04 46.4040459432 +10 46 36.016606848   14.9       ~ 85 0
11 ICRF J080512.8-011113 QSO 08 05 12.88848306 -01 11 13.7952408       17.87   ~ 71 0
12 PG 0851+202 BLL 08 54 48.8749846272 +20 06 30.639583620   15.649 15.146 15.446   ~ 2513 1
13 QSO B0903-573 BLL 09 04 53.1791655231 -57 35 05.782508724           ~ 131 1
14 [VV98] J104406.4+295901 Bla 10 44 06.3421 +29 59 00.990   19.25 19.03 18.64   ~ 50 1
15 6C 104451+715930 Bla 10 48 27.61992778 +71 43 35.9384142     19.0 17.49   ~ 270 1
16 FIRST J111005.0+365336 Sy1 11 10 05.0364218064 +36 53 36.320648064   21.09 20.88     ~ 34 1
17 HSCS J121503.42-014858.7 QSO 12 15 03.42 -01 48 58.7           ~ 4 0
18 HSCS J121503.55-014859.3 QSO 12 15 03.55 -01 48 59.3           ~ 3 0
19 M 87 AGN 12 30 49.42338414 +12 23 28.0436859 10.16 9.59 8.63   7.49 ~ 7815 3
20 MCG-03-34-064 Sy2 13 22 24.4583154360 -16 43 42.481822404   14   13.16   ~ 345 2
21 NVSS J144515+492604 rG 14 45 15.447 +49 26 05.84           ~ 15 0
22 NAME Sgr A* X 17 45 40.03599 -29 00 28.1699           ~ 4970 3
23 QSO J2102+6015 Bla 21 02 40.21905211 +60 15 09.8365719           ~ 31 1
24 4C -02.81 BLL 21 34 10.30958988 -01 53 17.2389056   18.6 19.00 18.87   ~ 431 1
25 NGC 7277 EmG 22 26 10.950 -31 08 42.96   14.14   14.1 13.8 ~ 35 0
26 QSO B2232+282 BLL 22 36 22.47084387 +28 28 57.4132050   19.1 19.0 17.60   ~ 306 2
27 [FMD2015] J230010.19-000531.8 rG 23 00 10.18 -00 05 31.7           ~ 7 0

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