2009MNRAS.394..443M


Query : 2009MNRAS.394..443M

2009MNRAS.394..443M - Mon. Not. R. Astron. Soc., 394, 443-453 (2009/March-3)

The XMM-Newton view of AGN with intermediate-mass black holes.

MINIUTTI G., PONTI G., GREENE J.E., HO L.C., FABIAN A.C. and IWASAWA K.

Abstract (from CDS):

We have observed with XMM-Newton four radiatively efficient active type 1 galaxies with black hole masses <106M, selected optically from the Sloan Digital Sky Survey and previously detected in the ROSAT All Sky Survey. Their X-ray spectra closely resemble those of more luminous Seyferts and quasars, powered by accretion on to much more massive black holes and none of the objects is intrinsically absorbed by cold matter totally covering the source. We show here that their soft X-ray spectrum exhibits a soft excess with the same characteristics as that observed ubiquitously in radio-quiet Seyfert 1 galaxies and type 1 quasars, both in terms of temperatures and strength. This is highly surprising because the small black hole mass of these objects should lead to a thermal disc contribution in the soft X-rays and not in the ultraviolet (as for more massive objects) with thus a much more prominent soft X-ray excess. Moreover, even when the soft X-ray excess is modelled with a pure thermal disc, its luminosity turns out to be much lower than that expected from accretion theory for the given temperature. While alternative scenarios for the nature of the soft excess (namely smeared ionized absorption and disc reflection) cannot be distinguished on a pure statistical basis, we point out that the absorption model produces a strong correlation between absorbing column density and ionization state, which may be difficult to interpret and is most likely spurious. Moreover, as pointed out before by others, absorption must occur in a fairly relativistic wind which is problematic, especially because of the enormous implied mass outflow rate. As for reflection, it does only invoke standard ingredients of any accretion model for radiatively efficient sources such as a hard X-rays source and a relatively cold (though partially ionized) accretion disc, and therefore seems the natural choice to explain the soft excess in most (if not all) cases. The reflection model is also consistent with the additional presence of a thermal disc component with the theoretically expected temperature (although, again, with smaller-than-expected total luminosity). We also studied in some detail the X-ray variability properties of the four objects. The observed active galaxies are among the most variable in X-rays and their excess variance is among the largest. This is in line with their relatively small black hole mass and with expectations from simple power spectra models.

Abstract Copyright: © 2009 The Authors. Journal compilation © 2009 RAS

Journal keyword(s): galaxies: active - X-rays: galaxies

Simbad objects: 34

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Number of rows : 34
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 Mrk 335 Sy1 00 06 19.5372339024 +20 12 10.617404076   14.19 13.85     ~ 1252 0
2 Mrk 1502 Sy1 00 53 34.9331107632 +12 41 35.929269132   14.41 14.03     ~ 1166 1
3 Ton S 180 Sy1 00 57 20.2040816832 -22 22 56.575212564   14.60 14.34 15.23   ~ 300 0
4 2XMM J010712.0+140844 Sy1 01 07 12.0268679880 +14 08 44.981850408   19.30 18.83     ~ 49 0
5 ESO 113-45 Sy1 01 23 45.7631533440 -58 48 20.808928944   14.08 13.83 13.34   ~ 880 0
6 NGC 863 Sy1 02 14 33.5604714720 -00 46 00.181845336   14.48 13.81 17.9   ~ 689 0
7 Mrk 1095 Sy1 05 16 11.4092471904 -00 08 59.157166920   14.30 13.92     ~ 890 1
8 LEDA 88588 Sy1 07 08 41.4886614696 -49 33 06.308921700   16.02 15.7 12.7   ~ 517 0
9 Mrk 110 Sy1 09 25 12.8479065576 +52 17 10.386311208   16.82 16.41     ~ 604 0
10 HE 1029-1401 Sy1 10 31 54.3173785536 -14 16 51.378102372   14.08 13.86     ~ 132 0
11 NGC 3783 Sy1 11 39 01.7096819040 -37 44 19.009642992   12.46 13.43 11.33 12.1 ~ 1647 0
12 2MASX J11400874+0307114 Sy1 11 40 08.7172457952 +03 07 11.399104884   19.03 18.48     ~ 54 1
13 NAME G 1200-2038 Sy1 12 02 56.93256 -20 56 02.9580           ~ 161 0
14 NGC 4051 Sy1 12 03 09.6101337312 +44 31 52.682601288   11.08 12.92 9.94   ~ 2164 1
15 NGC 4151 Sy1 12 10 32.5759813872 +39 24 21.063527532   12.18 11.48     ~ 3687 2
16 PB 3894 Sy1 12 14 17.6738687784 +14 03 13.182723144   14.46 14.19     ~ 821 0
17 NGC 4253 Sy1 12 18 26.5163572920 +29 48 46.531535472   14.34 13.57     ~ 1039 1
18 NGC 4395 Sy2 12 25 48.8633109888 +33 32 48.700168152 10.84 10.54 10.11 9.98   ~ 1177 1
19 NGC 4593 Sy1 12 39 39.4435107024 -05 20 39.034988448   13.95 13.15     ~ 1089 0
20 LEDA 42648 Sy1 12 42 10.6050409800 +33 17 02.662913436   16.45 15.65     ~ 116 0
21 LEDA 88835 Sy1 13 25 19.3805530608 -38 24 52.611680340   16.64 13.80 15.33 14.78 ~ 418 0
22 NGC 5139 GlC 13 26 47.28 -47 28 46.1           ~ 3424 0
23 IC 4271 Sy2 13 29 21.4493074392 +37 24 50.460172056   15.6       ~ 125 1
24 ESO 445-50 Sy1 13 49 19.2601801224 -30 18 34.213815504   13.81 13.66 12.18 12.35 ~ 803 0
25 2XMM J135724.5+652506 Sy1 13 57 24.5204418120 +65 25 05.952508176   18.91 18.58     ~ 46 0
26 NGC 5548 Sy1 14 17 59.5400291832 +25 08 12.603122268   14.35 13.73     ~ 2708 0
27 Z 47-107 Sy1 14 34 50.6282462496 +03 38 42.520770600   15.84 15.28     ~ 55 0
28 Mrk 478 Sy1 14 42 07.4714418744 +35 26 22.938625500   14.91 14.58     ~ 533 0
29 Mrk 841 Sy1 15 04 01.1935384104 +10 26 15.780409692   14.50 14.27     ~ 649 0
30 2XMM J160531.8+174825 Sy1 16 05 31.8490706465 +17 48 26.223103808           ~ 33 0
31 Mrk 509 Sy1 20 44 09.7504483224 -10 43 24.727155528   13.35 13.12 10.7   ~ 1275 0
32 UGC 12163 Sy1 22 42 39.3363009144 +29 43 31.302092640   14.86 14.16     ~ 697 1
33 LEDA 3096712 Sy1 22 57 39.0250746096 -36 56 06.528333048   16.59 16.0 15.64   ~ 75 0
34 NGC 7469 Sy1 23 03 15.6 +08 52 26 12.60 13.00 12.34     ~ 2094 3

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