2010ApJ...717..766L


Query : 2010ApJ...717..766L

2010ApJ...717..766L - Astrophys. J., 717, 766-775 (2010/July-2)

Mid-infrared spectroscopy of high-redshift 3CRR sources.

LEIPSKI C., HAAS M., WILLNER S.P., ASHBY M.L.N., WILKES B.J., FAZIO G.G., ANTONUCCI R., BARTHEL P., CHINI R., SIEBENMORGEN R., OGLE P. and HEYMANN F.

Abstract (from CDS):

Using the Spitzer Space Telescope, we have obtained rest-frame 9-16 µm spectra of 11 quasars and 9 radio galaxies from the 3CRR catalog at redshifts 1.0 < z < 1.4. This complete flux-limited 178 MHz selected sample is unbiased with respect to orientation and therefore suited to studying orientation-dependent effects in the most powerful active galactic nuclei (AGNs). The mean radio-galaxy spectrum shows a clear silicate absorption feature (τ9.7µm= 1.1) whereas the mean quasar spectrum shows silicates in emission. The mean radio-galaxy spectrum matches a dust-absorbed mean quasar spectrum in both shape and overall flux level. The data for individual objects conform to these results. The trend of the silicate depth to increase with decreasing core fraction of the radio source further supports that for this sample orientation is the main driver for the difference between radio galaxies and quasars, as predicted by AGN unification. However, comparing our high-z sample with lower redshift 3CRR objects reveals that the absorption of the high-z radio galaxy MIR continuum is lower than expected from a scaled-up version of lower luminosity sources, and we discuss some effects that may explain these trends.

Abstract Copyright: ∼

Journal keyword(s): galaxies: active - galaxies: high-redshift - infrared: galaxies

Simbad objects: 21

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Number of rows : 21
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 3C 13 rG 00 34 14.555 +39 24 16.67   22.5       ~ 144 1
2 3C 65 rG 02 23 43.190 +40 00 52.46   23.0       ~ 185 1
3 7C 022927.30+341049.00 QSO 02 32 28.8769824336 +34 23 46.713498468   20.70 19     ~ 197 1
4 3C 181.0 Sy2 07 28 10.2171164616 +14 37 36.565176324   19.35 18.92     ~ 168 2
5 3C 186 QSO 07 44 17.4720658920 +37 53 17.250697320   17.5 18.14 17.2   ~ 339 1
6 3C 190 QSO 08 01 33.5525166480 +14 14 42.813906612   21.07 20.26 18.972   ~ 249 2
7 3C 204 QSO 08 37 45.0013678200 +65 13 35.305376376   18.76 18.21     ~ 184 1
8 3C 208 QSO 08 53 08.6093021736 +13 52 54.845406984   17.76 17.42     ~ 257 1
9 3C 212 QSO 08 58 41.44702653 +14 09 44.7622845   19.96 19.06     ~ 257 1
10 4C 12.37 QSO 10 42 44.6052783816 +12 03 31.263917976   18.03 17.77     ~ 448 2
11 3C 252.0 rG 11 11 31.960 +35 40 44.64   22       ~ 127 1
12 3C 266 rG 11 45 43.384 +49 46 07.90   22       ~ 150 1
13 3C 267 rG 11 49 56.526 +12 47 18.95   22.5       ~ 158 2
14 ICRF J120913.6+433920 Sy1 12 09 13.6108333200 +43 39 20.916497268   18.81 18.24     ~ 248 1
15 7C 132816.2+252436 QSO 13 30 37.6960744824 +25 09 10.983105972   18.31 17.67     ~ 373 1
16 3C 324.0 Sy1 15 49 49.170 +21 25 39.50   21.5       ~ 312 1
17 7C 154914.09+625020.00 QSO 15 49 59.206 +62 41 18.31   21.92 20.70     ~ 147 2
18 3C 356 QSO 17 24 20.232 +50 57 14.47   21.5 21.5     ~ 225 1
19 4C 16.49 QSO 17 34 42.6025956120 +16 00 32.342065776     18.4     ~ 78 2
20 3C 368.0 rG 18 05 06.358 +11 01 32.55   21.5       ~ 253 1
21 3C 469.1 rG 23 55 22.89 +79 55 21.0   22.5       ~ 85 2

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