2003MNRAS.340.1095D


Query : 2003MNRAS.340.1095D

2003MNRAS.340.1095D - Mon. Not. R. Astron. Soc., 340, 1095-1135 (2003/April-3)

Quasars, their host galaxies and their central black holes.

DUNLOP J.S., McLURE R.J., KUKULA M.J., BAUM S.A., O'DEA C.P. and HUGHES D.H.

Abstract (from CDS):

We present the final results from our deep Hubble Space Telescope (HST) imaging study of the host galaxies of radio-quiet quasars (RQQs), radio-loud quasars (RLQs) and radio galaxies (RGs). We describe and analyse new Wide Field & Planetary Camera 2 (WFPC2) R -band observations for 14 objects, which when combined with the first tranche of HST imaging reported in McLure et al., provide a complete and consistent set of deep, red, line-free images for statistically matched samples of 13 RQQs, 10 RLQs and 10 RGs in the redshift band 0.1 < z < 0.25. We also report the results of new deep VLA imaging that has yielded a 5-GHz detection of all but one of the 33 active galactic nuclei (AGN) in our sample.

Careful modelling of our images, aided by a high dynamic-range point spread function, has allowed us to determine accurately the morphology, luminosity, scalelength and axial ratio of every host galaxy in our sample. Armed with this information we have undertaken a detailed comparison of the properties of the hosts of these three types of powerful AGN, both internally and with the galaxy population in general.

We find that spheroidal hosts become more prevalent with increasing nuclear luminosity such that, for nuclear luminosities MV< -23.5, the hosts of both radio-loud and radio-quiet AGN are virtually all massive ellipticals. Moreover, we demonstrate that the basic properties of these hosts are indistinguishable from those of quiescent, evolved, low-redshift ellipticals of comparable mass. This result rules out the possibility that radio-loudness is determined by host-galaxy morphology, and also sets severe constraints on evolutionary schemes that attempt to link low-z ultraluminous infrared galaxies with RQQs.

Instead, we show that our results are as expected given the relationship between black hole and spheroid mass established for nearby galaxies, and apply this relation to estimate the mass of the black hole in each object. The results agree remarkably well with completely independent estimates based on nuclear emission-line widths; all the quasars in our sample have Mbh> 5x108 M☉, while the radio-loud objects are confined to Mbh> 109 M☉. This apparent mass-threshold difference, which provides a natural explanation for why RQQs outnumber RLQs by a factor of 10, appears to reflect the existence of a minimum and a maximum level of black hole radio output, which is a strong function of black hole mass (∝M2–2.5bh). Finally, we use our results to estimate the fraction of massive spheroids/black holes that produce quasar-level activity. This fraction is ≃0.1 per cent at the present day, rising to >10 per cent at z ≃ 2-3.


Abstract Copyright: 2003 RAS

Journal keyword(s): black hole physics - galaxies: active - galaxies: photometry - quasars: general - infrared: galaxies

Simbad objects: 35

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Number of rows : 35
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 LEDA 3237 Sy1 00 54 52.1183662680 +25 25 38.983241532     15.42     ~ 421 0
2 [OKM2018] SWIFT J0056.9+1472 Sy1 00 57 09.9306975096 +14 46 10.142054004   16.56 16.29     ~ 167 0
3 ICRF J013957.3+013146 Sy1 01 39 57.30577668 +01 31 46.1387932   17.12 17.07     ~ 178 1
4 Mrk 1014 Sy1 01 59 50.2534701768 +00 23 40.864244784   16.08 15.87     ~ 606 0
5 7C 020415.59+291722.00 Sy1 02 07 02.2064405304 +29 30 46.051043400   16 16     ~ 161 1
6 PKS 0230-027 rG 02 32 43.6 -02 33 45     19.2     ~ 13 0
7 LEDA 138537 Sy1 02 47 40.8457737264 +19 40 57.824917500   16.77 16.66     ~ 48 0
8 PB 6972 QSO 03 00 29.7768363648 +02 40 50.861837028   16.1 16.1     ~ 33 0
9 3C 79.0 Sy2 03 10 00.0936589848 +17 05 58.599361932   19.54 18.75     ~ 268 3
10 3C 93.1 BLL 03 48 46.9073426592 +33 53 15.461439576   20.723   19.110   ~ 133 1
11 QSO B0736+01 Bla 07 39 18.03389906 +01 37 04.6177501   16.90 16.47 16.19   ~ 738 1
12 3C 219 Sy1 09 21 08.6258123424 +45 38 57.358202856   19.56 18.69     ~ 424 2
13 Ton 1057 Sy1 09 25 54.7145627448 +19 54 05.064888348   16.02 15.89     ~ 187 0
14 PG 0953+414 Sy1 09 56 52.3931554992 +41 15 22.211247636 14.710 15.611 15.546 15.294 14.720 ~ 472 0
15 7C 095855.9+290131 Sy2 10 01 49.5227371368 +28 47 08.943487440   18.21 17.27     ~ 447 1
16 4C 13.41 Sy1 10 07 26.0965408440 +12 48 56.184940764   15.81 15.68     ~ 418 2
17 2MASS J10145491+0033374 Sy1 10 14 54.9035635608 +00 33 37.366161048   20.23 18.94 16.104   ~ 169 0
18 PKS 1020-10 BLL 10 22 32.8200967176 -10 37 44.309640648   16.25 16.11 16.0   ~ 144 1
19 PKS 1215-033 rG 12 17 55.2979512456 -03 37 23.249281512   19.336 18.9 19.177   ~ 23 1
20 LEDA 39531 BLL 12 18 27.7800402360 +01 02 37.335539616   17.40   17.012   ~ 38 1
21 QSO B1217+023 BLL 12 20 11.8846520568 +02 03 42.223956876   16.15 15.97 15.6   ~ 338 2
22 M 87 AGN 12 30 49.42338414 +12 23 28.0436859 10.16 9.59 8.63   7.49 ~ 7815 3
23 ICRF J133253.2+020045 Sy1 13 32 53.27053616 +02 00 45.6991690   19.08 18.49     ~ 219 1
24 PKS J1345-0156 rG 13 45 16.8665165568 -01 56 25.651411548   17.80       ~ 28 1
25 LB 906 QSO 15 52 02.4005214816 +20 14 01.588323012   16.9 17.12     ~ 49 0
26 LEDA 3096499 Sy1 16 37 46.4977481160 +11 49 49.203034212   16.98 16.50     ~ 112 1
27 QSO B2004-447 Bla 20 07 55.1842447944 -44 34 44.274118260   19.3 19.3 18   ~ 185 1
28 ICRF J213745.1-143255 Sy1 21 37 45.1959922824 -14 32 55.695508728 15.41 15.63 15.53 15.0   ~ 390 1
29 QSO B2141+1730 Bla 21 43 35.54456275 +17 43 48.7875890   15.91 15.73 15.17   ~ 418 1
30 3C 436 Sy2 21 44 11.7308886192 +28 10 18.750481356   18.5       ~ 196 1
31 2MASS J22174773-0332383 Sy1 22 17 47.7281177664 -03 32 38.436635436   17.25 17.20 17.37   ~ 57 0
32 2MASX J22502534+1419519 Sy1 22 50 25.3475290512 +14 19 52.095751140   17.28 16.97 17.243   ~ 210 1
33 2MASX J23472568+1844502 Sy2 23 47 25.7033911152 +18 44 50.636115024     15.9     ~ 26 0
34 4C -01.61 BLL 23 51 56.1224889360 -01 09 13.315371768   16.83 16.59     ~ 380 1
35 2MASX J23580966-0800049 Sy1 23 58 09.6921883176 -08 00 04.719093984   18.5 17.5     ~ 51 1

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