2023MNRAS.520..129T


Query : 2023MNRAS.520..129T

2023MNRAS.520..129T - Mon. Not. R. Astron. Soc., 520, 129-146 (2023/March-3)

Inclination dependence of warm coronal flux in high-accretion-rate AGNs.

TANG Z.-Y., FENG J.-J. and FAN J.-H.

Abstract (from CDS):

Most active galactic nucleus (AGN) spectra show a soft X-ray excess above the 2-10 keV power law extrapolation. A warm corona has been widely used to explain the excess, but its observed radiation flux in the actually physical environment has yet to be further studied. For the first time, we calculate the relativistic warm coronal flux under the finite disc-corona thickness in high-accretion-rate systems. The numerical results show that the warm coronal flux generally rises first and then drops with increasing inclination. The flux rise is more significant for a compact and low-temperature warm corona and can reach 1-2 dexes. Meanwhile, the flux drop is significant if and only if the warm corona is heavily obscured due to the finite thickness. Our model can successfully explain the soft excess variance and the X-ray weak fraction in a high-accretion-rate AGN sample. In conclusion, our study indicates that when fitting the soft X-ray spectra of AGNs, the relativistic inclination dependence of warm coronal flux is essential, especially for the high-accretion-rate systems with thick warm coronae.

Abstract Copyright: © 2023 The Author(s) Published by Oxford University Press on behalf of Royal Astronomical Society

Journal keyword(s): accretion, accretion discs - black hole physics - galaxies: active

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 Ton S 180 Sy1 00 57 20.2040816832 -22 22 56.575212564   14.60 14.34 15.23   ~ 320 0
2 [VV2006] J030000.0-080357 QSO 03 00 00.0066457824 -08 03 56.995335000   17.11 16.94     ~ 29 0
3 QSO J0809+4619 QSO 08 09 08.1365285760 +46 19 25.574163852   16.83 16.72     ~ 60 0
4 QSO J0820+2334 QSO 08 20 24.2210785368 +23 34 50.452002372   17.87 17.74     ~ 37 0
5 SDSS J094012.29+461850.3 QSO 09 40 12.2957131752 +46 18 50.308929324           ~ 11 0
6 2MASSI J1048179+312905 Sy1 10 48 17.9830525056 +31 29 05.780748624   18.31 17.92     ~ 23 0
7 2MASS J11031293+4141549 Sy1 11 03 12.9342552360 +41 41 54.957214860   17.04 16.76     ~ 47 1
8 [VV2006] J112756.7+115427 QSO 11 27 56.7661245072 +11 54 27.129296628   17.51 17.35     ~ 35 0
9 2MASS J11275739+6441183 Sy1 11 27 57.4164317808 +64 41 18.398869764   17.83 17.66     ~ 31 0
10 2MASS J12063307+4125361 Sy1 12 06 33.0773977320 +41 25 36.035651964   18.03 17.74     ~ 29 0
11 2MASS J12073462+1506438 QSO 12 07 34.6307734152 +15 06 43.697908548   18.31 17.98     ~ 28 0
12 RMB 221 Sy1 12 18 50.5204079496 +10 15 54.283624488   17.76 17.63     ~ 48 0
13 QSO J1245+3356 QSO 12 45 11.2585883616 +33 56 10.098792816   17.06 16.88     ~ 62 0
14 LB 2522 Sy1 13 01 12.9250750776 +59 02 06.693816732   16.04 15.89     ~ 298 0
15 PB 4007 Sy1 13 36 02.0092074528 +17 25 13.092799188   16.50 16.33     ~ 93 1

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