1999AJ....117..677B


Query : 1999AJ....117..677B

1999AJ....117..677B - Astron. J., 117, 677-706 (1999/February-0)

The nature and evolution of classical double radio sources from complete samples.

BLUNDELL K.M., RAWLINGS S. and WILLOTT C.J.

Abstract (from CDS):

We present a study of the trends in luminosity, linear size, spectral index, and redshift of classical double radio sources, from three complete samples selected at successively fainter low radio-frequency flux limits. We have been able to decouple the effects of the tight correlation between redshift and luminosity (inherent in any single flux-limited sample) which have hitherto hindered interpretation of the relationships between these four source properties. The major trends found are that (i) spectral indices increase with linear size, (ii) rest-frame spectral indices have a stronger dependence on luminosity than on redshift except at high (GHz) frequencies, and (iii) the linear sizes are smaller at higher redshifts. We reproduce the observed dependences in a model for radio sources (born throughout cosmic time according to a radio-source birth function) whose lobes are fed with a synchrotron-emitting population from compact hotspots, and which suffer inverse Compton, synchrotron, and adiabatic expansion losses. The magnetic energy density within each hotspot is proportional to the jet power, and synchrotron losses suffered in the hotspot mean that the energy spectrum of the emitting particles fed to the lobes is governed by the jet power. The axial ratios of radio sources in our model increase as the sources age, and axial ratios are higher in sources with higher jet power. In simulating the basic observed dependences, we find that there is no need to invoke any systematic change in the environments of these objects with redshift if the consequences of imposing a survey flux limit on our simulated data sets are properly included in the model. It is also necessary to include appropriate energy loss mechanisms (such as the effects of the cosmic microwave background and feeding the lobes from a compact hotspot), which cause decreasing luminosity through the life of a source. Although our study has broken the luminosity-redshift degeneracy, we present evidence that for such studies there is an unavoidable ``youth-redshift degeneracy'', even though radio sources are short-lived relative to the age of the universe; it is imperative to take this into account in studies that seemingly reveal correlations of source properties with redshift such as the ``alignment effect.''

Abstract Copyright:

Journal keyword(s): Galaxies: Active - Galaxies: Evolution - Galaxies: Jets - Galaxies: Quasars: General - Radio Continuum

Simbad objects: 31

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Number of rows : 31
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 NVSS J021326+330757 Rad 02 13 26.7 +33 07 56           ~ 12 1
2 4C 41.17 rG 06 50 52.098 +41 30 30.53           ~ 337 1
3 QSO B0710+439 QSO 07 13 38.16413557 +43 49 17.2072102   20.7       ~ 244 0
4 5C 7.230 QSO 08 24 33.00930681 +24 38 43.1160776   19.93 19.41     ~ 29 1
5 NVSS J082529+385212 Rad 08 25 29.99 +38 52 12.0           ~ 5 1
6 3C 200 rG 08 27 25.38019 +29 18 44.9601   20       ~ 175 1
7 B2 0835+37 Rad 08 38 25.03 +37 10 37.3   19.5       ~ 20 0
8 7C 0927+3516 BLL 09 30 55.27911112 +35 03 37.6081515   20.98 20.35 18.40   ~ 71 1
9 M 82 AGN 09 55 52.430 +69 40 46.93 9.61 9.30 8.41     ~ 5858 6
10 4C 74.16 G 10 14 14.5 +74 37 34           ~ 38 1
11 4C 36.17 Rad 10 38 51.3 +36 01 15           ~ 17 1
12 7C 1049+3827 Sy2 10 52 11.7875 +38 11 43.913   20.9 20.9     ~ 36 1
13 NVSS J105911+392504 rG 10 59 11.4 +39 25 07           ~ 22 1
14 Mrk 421 BLL 11 04 27.3140835504 +38 12 31.798495872   13.50 12.90 8.31   ~ 2671 1
15 4C 37.29A rG 11 09 28.8583 +37 44 31.092     23.7     ~ 51 1
16 4C 37.31 rG 11 32 35.9 +36 54 12   23       ~ 40 1
17 NVSS J113505+370840 rG 11 35 05.9 +37 08 41           ~ 18 1
18 87GB 120133.1+392914 BiC 12 04 06.8559 +39 12 17.655   19.5       ~ 32 1
19 3C 268.3 Sy1 12 06 24.70656 +64 13 36.8760   21.847 20.790 19.910   ~ 188 1
20 7C 120500.2+340922 Sy2 12 07 32.930 +33 52 40.13   16.4       ~ 92 1
21 NVSS J121009+382114 rG 12 10 09.35904 +38 21 14.6484   21.3       ~ 17 1
22 6C 122535+365318 QSO 12 27 58.72552577 +36 35 11.8265176   21.5 21.5     ~ 134 0
23 7C 1245+3421 G 12 47 48.056 +34 05 12.41   19.5       ~ 22 1
24 ICRF J163433.8+624535 Sy2 16 34 33.80623119 +62 45 35.8960467   21.06 20.61     ~ 215 1
25 ICRF J163828.2+623444 Sy2 16 38 28.22535940 +62 34 44.3168151   20.7 20.7     ~ 163 2
26 NAME Her B Sy1 16 42 58.80997043 +39 48 36.9939552   16.81 16.59 16.84   ~ 1724 2
27 4C 13.66 G 18 01 39.0 +13 51 24           ~ 51 1
28 ClG 1821+64 ClG 18 21 56.7276 +64 20 55.841           ~ 504 1
29 7C 1821+6419 Sy1 18 21 57.2130271440 +64 20 36.221312076   14.23 14.24     ~ 601 1
30 NAME Cyg A Sy2 19 59 28.35656837 +40 44 02.0972325   16.22 15.10     ~ 2367 2
31 3C 454.3 Bla 22 53 57.7480438728 +16 08 53.561508864   16.57 16.10 15.22   ~ 2847 2

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