2024A&A...689A.247L


Query : 2024A&A...689A.247L

2024A&A...689A.247L - Astronomy and Astrophysics, volume 689A247 (2024/9-1)

The XMM-Newton and NuSTAR view of IRASF11119+3257 I. Detection of multiple ultra fast outflow components and a very cold corona.

LANZUISI G., MATZEU G., BALDINI P., BERTOLA E., COMASTRI A., TOMBESI F., LUMINARI A., BRAITO V., REEVES J., CHARTAS G., BIANCHI S., BRUSA M., CRESCI G., NARDINI E., PICONCELLI E., ZAPPACOSTA L., SERAFINELLI R., GASPARI M., GILLI R., CAPPI M., DADINA M., PERNA M., VIGNALI C. and VEILLEUX S.

Abstract (from CDS):

Context. IRASF11119+3257 is an ultra-luminous infrared galaxy with a post-merger morphology, hosting a type-1 quasar at z = 0.189. It shows a prominent ultra-fast outflow (UFO) absorption feature (vout ∼ 0.25c) in its 2013 Suzaku spectrum. This is the first system in which the energy released by the UFO was compared to that of the known galaxy-scale molecular outflow to investigate the mechanism driving active galactic nuclei (AGN) feedback.
Aims. In 2021, we obtained the first XMM-Newton long look of the target, coordinated with a simultaneous NuSTAR observation, with the goal of constraining the broad band continuum and the nuclear wind physical properties and energetics with an unprecedented accuracy.
Methods. The new high-quality data allowed us to clearly detect at a confidence level P > 99.8% multiple absorption features associated with the known UFO at the 9.1 and 11.0 keV rest frames. Furthermore, an emission plus absorption feature at 1.1 - 1.3 keV reveals the presence of a blueshifted P-Cygni profile in the soft band.
Results. We associate the two hard band features with blends of FeXXV and FeXXVI Heα-Lyα and Heβ-Lyβ line pairs and infer a large column (NH ∼ 1024 cm–2) of highly ionized (log ξ ∼ 5) gas outflowing at vout = 0.27 ± 0.01c. The 1.3 keV absorption line can be associated with a blend of Fe and Ne transitions, produced by a lower column (NH ∼ 3 × 1021 cm–2) and ionization (log ξ ∼ 2.6) gas component outflowing at the same speed. Using a radiative-transfer disk wind model to fit the highly ionized UFO, we derive a mass outflow rate comparable with the mass accretion rate and the Eddington limit ($ {\dot{M}}_{\mathrm{out}}=4.25_{-0.73}^{+1.11}\, M_{\odot}/\mathrm{yr} $, ∼1.6 Ṁacc and ∼1.0 ṀEdd), and kinetic energy ($ \dot E_{\mathrm{kin}}=1.21_{-0.20}^{+0.32}L_{\mathrm{bol}} $ and ∼0.7LEdd) and momentum flux ($ {\dot P_{\mathrm{out}}}=6.37_{-1.09}^{+1.67} L_{\mathrm{bol}}/c $) among the highest reported in the literature. We measured an extremely low high-energy cutoff (Ecut ∼ 25 - 30 keV). This and several other cases in the literature suggest that a steep X-ray continuum may be related to the formation of powerful winds. We also analyzed the ionized [OIII] component of the large-scale outflow through optical spectroscopy and derived a large outflow velocity (vout ∼ 3000 km/s) and energetics comparable with the large-scale molecular outflows. Finally, we observe a trend of decreasing outflow velocity from forbidden optical emission lines of decreasing ionization levels, interpreted as the outflow decelerating at large distances from the ionizing source.
Conclusions. The lack of a significant momentum boost between the nuclear UFO and the different phases of the large-scale outflow, observed in IRASF11119 and in a growing number of similar sources, can be explained by (i) a momentum-driven expansion, (ii) an inefficient coupling of the UFO with the host interstellar medium, or (iii) by repeated energy-driven expansion episodes with a low duty cycle, that average out on long timescales to produce the observed large-scale outflow.

Abstract Copyright: © The Authors 2024

Journal keyword(s): galaxies: active - galaxies: nuclei - quasars: absorption lines - quasars: supermassive black holes - quasars: individual: IRAS F11119+3257

Simbad objects: 19

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Number of rows : 19
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 MCG-02-07-024 Sy1 02 30 05.5225590096 -08 59 53.207139372   14.74 14.29 13.981 13.585 ~ 332 0
3 LEDA 2816425 Sy1 04 44 28.7756530728 +12 21 11.721056364           ~ 75 0
4 QSO J0831+5245 QSO 08 31 41.7108197808 +52 45 17.616994560   19.2   14.5 13.9 ~ 574 1
5 NGC 2992 Sy2 09 45 42.045 -14 19 34.90 13.54 13.14 12.18 12.6 12.2 ~ 951 3
6 IRAS 11119+3257 Sy1 11 14 38.8902542640 +32 41 33.483258276   19.22 17.96     ~ 165 0
7 LEDA 34449 Sy1 11 17 06.3989076960 +44 13 33.324039480   16.32 16.12     ~ 265 1
8 2MASS J11594101-1959247 Sy1 11 59 41.0142906912 -19 59 24.583599996   16.2 16.2     ~ 37 0
9 PB 3894 Sy1 12 14 17.6738687784 +14 03 13.182723144   14.46 14.19     ~ 873 0
10 Z 294-4 Sy1 12 56 14.2341182928 +56 52 25.238373852   14.68 13.84     ~ 2096 3
11 LEDA 88835 Sy1 13 25 19.3805530608 -38 24 52.611680340   16.64 13.80 15.33 14.78 ~ 457 0
12 LBQS 1338-0038 QSO 13 41 13.9355679576 -00 53 15.028930032   17.98 17.68     ~ 59 0
13 QSO B1422+2309 BLL 14 24 38.0938 +22 56 00.587   16.77 15.84 14.79   ~ 464 1
14 QSO J1614+4704 QSO 16 14 34.6744012152 +47 04 20.074719288   16.81 16.51     ~ 56 0
15 6C 170204+454510 Sy1 17 03 30.3824218008 +45 40 47.166180564   16.0       ~ 170 2
16 QSO B1725-142 QSO 17 28 19.7893499760 -14 15 55.854918288   14.69 14.03 13.7   ~ 362 0
17 Mrk 509 Sy1 20 44 09.7504483224 -10 43 24.727155528   13.35 13.12 10.7   ~ 1370 0
18 QSO B2202-0209 QSO 22 05 09.90 -01 55 18.0   17.5 17.5     ~ 28 0
19 Z 495-18 Sy1 22 42 39.3363009144 +29 43 31.302092640   14.86 14.16     ~ 748 1

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