2013MNRAS.432..530R


Query : 2013MNRAS.432..530R

2013MNRAS.432..530R - Mon. Not. R. Astron. Soc., 432, 530-553 (2013/June-2)

Radiative efficiency, variability and bondi accretion on to massive black holes: the transition from radio AGN to quasars in brightest cluster galaxies.

RUSSELL H.R., McNAMARA B.R., EDGE A.C., HOGAN M.T., MAIN R.A. and VANTYGHEM A.N.

Abstract (from CDS):

We examine unresolved nuclear X-ray sources in 57 brightest cluster galaxies to study the relationship between nuclear X-ray emission and accretion on to supermassive black holes. The majority of the clusters in our sample have prominent X-ray cavities embedded in the surrounding hot atmospheres, which we use to estimate mean jet power and average accretion rate on to the supermassive black holes over the past several hundred Myr. We find that roughly half of the sample have detectable nuclear X-ray emission. The nuclear X-ray luminosity is correlated with average accretion rate determined using X-ray cavities, which is consistent with the hypothesis that nuclear X-ray emission traces ongoing accretion. The results imply that jets in systems that have experienced recent active galactic nucleus (AGN) outbursts, in the last ∼ 107yr, are `on' at least half of the time. Nuclear X-ray sources become more luminous with respect to the mechanical jet power as the mean accretion rate rises. We show that nuclear radiation exceeds the jet power when the mean accretion rate rises above a few percent of the Eddington rate, or a power output of ∼10^45 erg s^-1, where the AGN apparently transitions to a quasar. The nuclear X-ray emission from three objects (A2052, Hydra A, M84) varies by factors of 2-10 on time-scales of 6 months to 10 years. If variability at this level is a common phenomenon, it can account for much of the scatter in the relationship between mean accretion rate and nuclear X-ray luminosity. We find no significant change in the spectral energy distribution as a function of luminosity in the variable objects. The nuclear X-ray luminosity is consistent with emission from either a jet, an advection-dominated accretion flow, or a combination of the two, although other origins are possible. We also consider the longstanding problem of whether jets are powered by the accretion of cold circumnuclear gas or nearly spherical inflows of hot keV gas. For a subset of 13 nearby systems in our sample, we re-examine the relationship between the jet power and the Bondi accretion rate. The results indicate weaker evidence for a trend between Bondi accretion and jet power, due to uncertainties in the cavity volumes and gas densities at the Bondi radius. We suggest that cold gas fuelling could be a likely source of accretion power in these objects; however, we cannot rule out Bondi accretion, which could play a significant role in low-power jets.

Abstract Copyright: © 2013 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society (2013)

Journal keyword(s): accretion, accretion discs - galaxies: active - galaxies: jets - X-rays: galaxies: clusters

Simbad objects: 62

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Number of rows : 62
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 NGC 193 rG 00 39 18.5878961880 +03 19 52.605787764   14.3       ~ 149 1
2 ACO 85 ClG 00 41 36.21 -09 19 30.4           ~ 974 0
3 ACO 133 ClG 01 02 41.5 -21 52 53           ~ 391 1
4 ZwCl 0104+0048 ClG 01 06 50.5 +01 04 10           ~ 67 0
5 NGC 507 rG 01 23 39.950 +33 15 22.22   13.0       ~ 459 1
6 ACO 262 ClG 01 52 50.4 +36 08 46           ~ 727 1
7 ACO 426 ClG 03 19 47.6 +41 30 54           ~ 2508 1
8 NGC 1316 rG 03 22 41.789 -37 12 29.52 9.81 9.15 8.53 7.66   ~ 1491 1
9 ZwCl 0335+0956 ClG 03 38 35.3 +09 57 54           ~ 402 1
10 BAX 058.2454+19.6830 ClG 03 52 58.9 +19 40 58           ~ 39 0
11 ACO 478 ClG 04 13 24.8 +10 27 52           ~ 522 0
12 NGC 1600 rG 04 31 39.858 -05 05 09.97   8.9   10.81   ~ 409 1
13 ZwCl 0735+7421 ClG 07 41 40.3 +74 14 58     17.70     ~ 273 0
14 3C 186 QSO 07 44 17.4720658920 +37 53 17.250697320   17.5 18.14 17.2   ~ 339 1
15 PKS 0745-19 rG 07 47 31.3247085936 -19 17 40.013334276   19.60       ~ 422 1
16 ClG 0745-1910 ClG 07 47 32.4 -19 18 23           ~ 378 0
17 ACO 611 ClG 08 00 58.7 +36 02 49           ~ 275 0
18 4C 55.16 Bla 08 34 54.90398776 +55 34 21.0703409   20.75 19.45 17.180   ~ 297 2
19 ZwCl 0857+2107 ClG 09 00 36.90 +20 53 40.3           ~ 103 0
20 IRAS 09104+4109 Sy2 09 13 45.4951283928 +40 56 28.215343572   19.69 19.21     ~ 260 1
21 MCG-02-24-007 LIN 09 18 05.66848602 -12 05 43.8060823   14.38 14.8     ~ 1077 1
22 ClG J0947+7623 ClG 09 46 59.916 +76 23 43.99           ~ 165 0
23 NVSS J094712+762312 Rad 09 47 12.37 +76 23 09.3           ~ 151 1
24 ZwCl 0949+5207 ClG 09 52 49.1 +51 53 05           ~ 141 0
25 ZwCl 1021+0426 ClG 10 23 39.0 +04 11 14   15.6 17.95     ~ 297 0
26 NGC 4261 LIN 12 19 23.2160630 +05 49 29.700024   13.92 12.87     ~ 1290 0
27 M 84 Sy2 12 25 03.74333 +12 53 13.1393 12.67 12.09 10.49     ~ 1841 2
28 M 49 Sy2 12 29 46.8 +08 00 01   13.21 12.17     ~ 2174 2
29 M 87 AGN 12 30 49.42338414 +12 23 28.0436859 10.16 9.59 8.63   7.49 ~ 7815 3
30 M 89 Sy2 12 35 39.80733343 +12 33 22.8308657 11.29 10.73 9.75     ~ 1037 2
31 NGC 4636 LIN 12 42 49.8333280080 +02 41 15.951929028   12.62 11.84     ~ 1156 1
32 ACO 3526 ClG 12 48 49.2 -41 18 17           ~ 1154 2
33 HCG 62 CGG 12 53 05.6 -09 12 21           ~ 313 0
34 NGC 4782 rG 12 54 35.698 -12 34 06.92   13 12.75 13.11   ~ 158 2
35 NGC 5044 BiC 13 15 23.9607836592 -16 23 07.547751744   11.9   10.74   ~ 531 0
36 ACO 1795 ClG 13 48 47.4 +26 34 55           ~ 1330 0
37 ACO 1835 ClG 14 01 02.07 +02 52 43.2           ~ 727 1
38 IC 4374 Bla 14 07 29.76229070 -27 01 04.2916695   13.61   11.79 12.55 ~ 142 3
39 3C 295 Sy1 14 11 20.6 +52 12 09   22.34 20.80 18.54   ~ 1021 4
40 ACO S 780 ClG 14 59 29.1 -18 10 45           ~ 93 0
41 NGC 5813 LIN 15 01 11.2302420864 +01 42 07.141569696 12.00 11.45 10.46 10.06   ~ 673 2
42 NGC 5846 rG 15 06 29.253 +01 36 20.29   11.9   9.74   ~ 891 2
43 ACO 2029 ClG 15 10 54.2 +05 44 23           ~ 1020 0
44 ACO 2052 ClG 15 16 41.64 +07 01 45.5           ~ 756 1
45 Z 49-90 Sy2 15 16 44.4893939136 +07 01 17.825410740   15.19 14.17     ~ 463 4
46 ACT-CL J1521.8+0742 ClG 15 21 48.8 +07 43 41     15.13     ~ 326 0
47 MCXC J1524.2-3154 ClG 15 24 12.9 -31 54 25           ~ 34 0
48 MCXC J1558.3-1410 ClG 15 58 22.0 -14 09 59           ~ 44 0
49 ACO 2199 ClG 16 28 34.5 +39 32 26           ~ 1206 1
50 MCG+01-43-006 SyG 16 51 07.9886687784 +04 59 35.547131472     18.25     ~ 502 1
51 NGC 6269 rG 16 57 58.1011343880 +27 51 15.883449192   14.4 13.73     ~ 109 1
52 NGC 6338 Bla 17 15 22.9842192344 +57 24 40.346559927   14.2   8   ~ 205 2
53 ClG 1821+64 ClG 18 21 56.7276 +64 20 55.841           ~ 511 1
54 7C 1821+6419 Sy1 18 21 57.2130271440 +64 20 36.221312076   14.23 14.24     ~ 632 1
55 3C 388.0 SyG 18 44 02.3840387736 +45 33 29.628672300   16.91 15.56     ~ 338 1
56 3C 401 SyG 19 40 25.116 +60 41 34.97   19.1       ~ 206 1
57 MCG+07-41-003 Bla 19 59 28.35656837 +40 44 02.0972325   16.22 15.10     ~ 2537 2
58 ACO 2390 ClG 21 53 37.4 +17 41 46           ~ 732 2
59 ACO S 1101 ClG 23 13 58.5 -42 43 39           ~ 272 1
60 ACO 2597 ClG 23 25 19.70 -12 07 27.7           ~ 572 0
61 ACO 2667 ClG 23 51 39.37 -26 05 02.7           ~ 190 0
62 ACO 4059 ClG 23 57 02.2 -34 45 58           ~ 400 1

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