2000AJ....119.2634B


Query : 2000AJ....119.2634B

2000AJ....119.2634B - Astron. J., 119, 2634-2644 (2000/June-0)

Emission-line properties of 3CR radio galaxies. III. Origins and implications of the velocity fields.

BAUM S.A. and McCARTHY P.J.

Abstract (from CDS):

We present the results of an analysis of the large-scale velocity fields of the ionized gas associated with powerful radio galaxies. Long-slit spectra of 52 objects provide a sample of resolved velocities that span a wide range of redshifts and radio and emission-line luminosities. Line widths reaching 1000 km.s–1 and resolved velocity fields with amplitudes of up 1500 km.s–1 are found on scales from 10 to 100 kpc in the environments of radio galaxies at redshifts greater than 0.5. The global velocities and FWHM are of comparable amplitudes in the FR II sources, while the FR I sources have FWHM values that are larger than their resolved velocity fields. We find evidence for systematically larger line widths and velocity field amplitudes at z>0.6. Several of the largest amplitude systems contain two galaxies with small projected separations. All of the greater than 1000 km.s–1 systems occur in objects at z>0.6 and all have comparable radio and [O II] sizes. There is a weak correlation of off-nuclear line widths and velocity field with the ratio of the radio and emission-line sizes, but it is of low statistical significance and there is a very large dispersion. The change in properties at redshifts above z∼0.6 could reflect a difference in environments of the host galaxies, with the hosts inhabiting higher density regions with increasing redshift (e.g., Hill & Lilly). The mass of ionized gas and the apparent enclosed dynamical mass are correlated and both increase steeply with redshift and/or radio power. The origin of the velocities remains uncertain. The data do not require jet-gas interactions to explain the kinematics and superficially are slightly more consistent with gravitational origins for the bulk of the kinematics. If the line width reflects the underlying gravitational potential, the observed FWHM traces the velocity dispersion of the host galaxy or its surrounding group or cluster. The highest velocities seen then point to interesting environments for intermediate- and high-redshift radio galaxies. Turbulent interactions with the expanding radio source as the origin of the kinematics are certainly not ruled out. In the jet interaction scenario, the maximum velocities seen in the nebula can be used to constrain the density of the preshock gas to be roughly ne>0.6 cm–3.

Abstract Copyright: ∼

Journal keyword(s): Galaxies: Kinematics and Dynamics - Radio Emission Lines

CDS comments: Table 1 : PKS 0745 = 0745-191, 1345 = 1345+125, 0634 = 0634-206. MRC 0457 = 0457-235, 0406 = 0406-244, 2104 = 2104-242.

Simbad objects: 61

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Number of rows : 61
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 2C 94 Sy2 01 08 52.8701830824 +13 20 14.262799812   15.19       ~ 494 2
2 8C 0106+729 Sy1 01 09 44.2610635193 +73 11 57.121454897   19.5       ~ 155 1
3 3C 34.0 rG 01 10 18.665 +31 47 20.48   21       ~ 177 2
4 3C 63 BLL 02 20 54.3166497648 -01 56 50.431204212           ~ 149 1
5 NGC 1218 Sy1 03 08 26.22380005 +04 06 39.3007808   12.84       ~ 413 0
6 3C 79.0 Sy2 03 10 00.0936589848 +17 05 58.599361932   19.54 18.75     ~ 268 3
7 Z 390-93 QSO 03 27 54.19499480 +02 33 41.9824262   13.95       ~ 230 1
8 2C 349 Sy2 03 58 54.4370049840 +10 26 02.791855968   16.68 15.41     ~ 356 2
9 TXS 0406-244 QSO 04 08 51.463920 -24 18 16.40880     22.40     ~ 82 1
10 PMN J0459-2330 rG 04 59 17.258 -23 30 57.41           ~ 14 1
11 LEDA 19313 Sy2 06 36 32.2509554376 -20 34 53.181243300   18.27 17.58     ~ 139 2
12 3C 169.1 rG 06 51 15.356 +45 09 26.21   20.5       ~ 63 1
13 3C 171.0 Sy2 06 55 14.7385158451 +54 08 57.427918985   19.94 19.08     ~ 264 1
14 3C 172 rG 07 02 08.30458800 +25 13 53.5192680   20.5       ~ 121 1
15 3C 180 Sy2 07 27 04.70 -02 04 37.0   19       ~ 82 1
16 PKS 0745-19 rG 07 47 31.3247085936 -19 17 40.013334276   19.60       ~ 422 1
17 ClG 0745-1910 ClG 07 47 32.4 -19 18 23           ~ 378 0
18 2XMM J080535.0+240951 Sy2 08 05 35.0054956728 +24 09 50.330022516   15.46       ~ 336 1
19 3C 196.1 Sy2 08 15 27.825 -03 08 27.67   18.490 16.940 16.797   ~ 124 1
20 ATO J146.9381+07.4223 Sy1 09 47 45.1433922288 +07 25 20.595729756   17.37 16.95     ~ 389 1
21 3C 244.1 QSO 10 33 33.9860997312 +58 14 35.611906344   19.0 19.0     ~ 191 1
22 3C 256 rG 11 20 43.022 +23 27 55.21   21.5       ~ 123 1
23 3C 257 rG 11 23 09.062 +05 30 20.58           ~ 92 1
24 NGC 3862 Sy2 11 45 05.00904503 +19 36 22.7409909   14.98 13.97     ~ 646 1
25 3C 265.0 Sy1 11 45 28.95577 +31 33 47.2434   20.0       ~ 250 1
26 3C 266 rG 11 45 43.384 +49 46 07.90   22       ~ 150 1
27 3C 267 rG 11 49 56.526 +12 47 18.95   22.5       ~ 158 2
28 M 84 Sy2 12 25 03.74333 +12 53 13.1393 12.67 12.09 10.49     ~ 1841 2
29 M 87 AGN 12 30 49.42338414 +12 23 28.0436859 10.16 9.59 8.63   7.49 ~ 7815 3
30 3C 275 rG 12 42 19.610 -04 46 20.45   21       ~ 116 1
31 3C 277.2 Sy1 12 53 32.425 +15 42 25.29   21.5       ~ 152 1
32 7C 125441.29+473632.00 SyG 12 56 57.485 +47 20 20.23   22.0       ~ 285 1
33 2MASX J13110466+2728070 Sy2 13 11 04.6615315248 +27 28 07.229535420   18.93 18.00     ~ 200 1
34 6C 131905+425044 Sy2 13 21 17.813 +42 35 15.38   16.86 16.23     ~ 282 1
35 PKS 1345+12 Sy2 13 47 33.36161873 +12 17 24.2398927   19.28 18.44 15.718   ~ 652 2
36 3C 294 rG 14 06 44.317 +34 11 30.19           ~ 234 1
37 3C 299 rG 14 21 05.6960 +41 44 49.260   20.496 19.330 18.560   ~ 187 1
38 3C 300 Sy2 14 22 59.85648 +19 35 36.7152   19.66 18.73     ~ 206 2
39 4C -04.53 rG 14 55 01.39497840 -04 20 59.8277760   19       ~ 68 1
40 3C 324.0 Sy1 15 49 49.170 +21 25 39.50   21.5       ~ 312 1
41 3C 326.1 rG 15 56 09.984 +20 04 20.81     20.0     ~ 116 1
42 NAME 3C 330G2 Sy2 16 09 34.92456720 +65 56 37.8351240   20.33       ~ 280 1
43 3C 341 rG 16 28 04.049 +27 41 43.07   19       ~ 146 1
44 3C 337 QSO 16 28 53.870 +44 19 03.52   20.0       ~ 148 1
45 3C 340 rG 16 29 37.862 +23 20 14.41   22       ~ 126 1
46 3C 352 rG 17 10 44.1001 +46 01 29.834   22.8       ~ 150 1
47 4C -00.67 Sy2 17 20 28.1680537512 -00 58 46.582453920   15.36       ~ 345 1
48 3C 356 QSO 17 24 20.232 +50 57 14.47   21.5 21.5     ~ 225 1
49 3C 368.0 rG 18 05 06.358 +11 01 32.55   21.5       ~ 253 1
50 3C 381.0 Sy2 18 33 46.2946146576 +47 27 02.566037088   18.64 17.24     ~ 209 1
51 3C 403.0 Sy2 19 52 15.7996999344 +02 30 24.238200816   15.42 16.5     ~ 353 1
52 MCG+07-41-003 Bla 19 59 28.35656837 +40 44 02.0972325   16.22 15.10     ~ 2537 2
53 PMN J2106-2404 rG 21 06 58.463 -24 05 06.11   23.0       ~ 79 2
54 3C 433.0 Sy2 21 23 44.5778423928 +25 04 27.670672416   17.660 16.350     ~ 338 1
55 3C 435 rG 21 29 06.105 +07 32 58.49   21       ~ 68 2
56 3C 437 rG 21 47 25.107 +15 20 37.51   23       ~ 128 2
57 3C 441 rG 22 06 04.917 +29 29 20.01   21.0       ~ 198 3
58 NGC 7236 LIN 22 14 44.9886363216 +13 50 47.450963760   14.3 14.3     ~ 286 1
59 3C 454.1 rG 22 50 32.934 +71 29 19.26   22       ~ 79 1
60 3C 458 rG 23 12 54.455 +05 16 23.63   20       ~ 94 1
61 3C 460 Sy2 23 21 28.50264 +23 46 47.6400   20.315   18.468   ~ 90 1

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