2004ApJ...616..783R


Query : 2004ApJ...616..783R

2004ApJ...616..783R - Astrophys. J., 616, 783-803 (2004/December-1)

Very large array H92α and H53α radio recombination line observations of M82.

RODRIGUEZ-RICO C.A., VIALLEFOND F., ZHAO J.-H., GOSS W.M. and ANANTHARAMAIAH K.R.

Abstract (from CDS):

We present high angular resolution (0".6) observations made with the Very Large Array of the radio continuum at 8.3 and 43 GHz, as well as H92α and H53α radio recombination lines from the nearby (∼3 Mpc) starburst galaxy M82. In the continuum we identify 58 sources at 8.3 GHz, of which 19 have no counterparts in catalogs published at other frequencies. At 43 GHz we identify 18 sources, unresolved at 0".6 resolution, of which five were unknown previously. The spatial distribution of the H92α line is inhomogeneous; we identify 27 features; about half of them are associated with continuum emission sources. Their sizes are typically in the range 2-10 pc. Although observed with poorer signal-to-noise ratio, the H53α line is detected. The line and continuum emission are modeled using a collection of H II regions at different distances from the nucleus. The observations can be interpreted assuming a single-density component, but equally well with two components if constraints originating from previous high-resolution continuum observations are used. The high-density component has a density of ∼4x104/cm3. However, the bulk of the ionization is in regions with densities that are typically a factor of 10 lower. The gas kinematics, using the H92α line, confirms the presence of steep velocity gradient (26 km/s/arcsec) in the nuclear region, as previously reported, in particular from observations of the [Ne II] line at 12 µm. This gradient has about the same amplitude on both sides of the nucleus. Since this steep gradient is observed not only on the major axis but also at large distances along a band at P.A.∼150°, the interpretation in terms of x2orbits elongated along the minor axis of the bar, which would be observed at an angle close to the inclination of the main disk, seems inadequate. The observed kinematics cannot be modeled using a simple model that consists of a set of circular orbits observed at different tilt angles. Ad hoc radial motions must be introduced to reproduce the pattern of the velocity field. Different families of orbits are indicated since we detect a signature in the kinematics at the transition between the two plateaus observed in the NIR light distribution. These H92α data also reveal the base of the outflow where the injection toward the halo on the northern side occurs. The outflow has a major effect on the observed kinematics, present even in the disk at distances close to the nucleus. The kinematic pattern suggests a connection between the gas flowing in the plane of M82 toward the center; this behavior most likely is due to the presence of a bar and the outflow out of the plane.

Abstract Copyright:

Journal keyword(s): Galaxies: Individual: Messier Number: M82 - Galaxies: ISM - Galaxies: Starburst - ISM: H II Regions - Radio Lines: Galaxies

Nomenclature: Table 2: [RVZ2004] SS.ss+SS.s N=62.

CDS comments: Table 2: source ID and coordinates (col. 1 and 2) are not galactic coordinates but 'SS.ss+SS.s' relative to RA = 09h51m, Dec = +69deg54' (1950). Fig. 6, Table 3, Table 4: regions WN not in SIMBAD.

Simbad objects: 70

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Number of rows : 70
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 NGC 253 SyG 00 47 33.134 -25 17 19.68   8.03   6.94 8.1 ~ 3343 2
2 3C 48 QSO 01 37 41.2996631208 +33 09 35.080388820   16.62 16.20     ~ 2820 2
3 NGC 2146 SBG 06 18 37.710 +78 21 25.27 11.67 11.38 10.59     ~ 722 2
4 [RVZ2004] 37.54+53.2 Rad 09 55 46.34 +69 40 39.3           ~ 2 0
5 [FBM2010] 38.76+53.5 HII 09 55 47.530 +69 40 39.94           ~ 3 0
6 [FBM2010] 39.10+57.3 SNR 09 55 47.880 +69 40 43.72           ~ 23 0
7 [FBM2010] 39.28+54.1 HII 09 55 48.040 +69 40 40.59           ~ 9 0
8 [FBM2010] 39.40+56.2 SNR 09 55 48.160 +69 40 43.00           ~ 16 0
9 [FBM2010] 39.64+53.3 SNR 09 55 48.400 +69 40 39.82           ~ 14 0
10 [FMB2008] 39.67+55.5 HII 09 55 48.43 +69 40 41.9           ~ 9 0
11 [FMB2008] 39.77+56.9 SNR 09 55 48.55 +69 40 43.3           ~ 10 0
12 [RVZ2004] 39.92+55.9 SR? 09 55 48.69 +69 40 41.9           ~ 1 0
13 [RVZ2004] 40.10+55.0 Rad 09 55 48.87 +69 40 41.0           ~ 1 0
14 [FBM2010] 40.32+55.2 SNR 09 55 49.060 +69 40 41.53           ~ 11 0
15 [RVZ2004] 40.49+57.4 HXB 09 55 49.26 +69 40 43.4           ~ 2 0
16 [FBM2010] 40.61+56.3 SNR 09 55 49.370 +69 40 42.44           ~ 16 0
17 [FBM2010] 40.68+55.1 SNR 09 55 49.420 +69 40 41.43           ~ 19 0
18 [GIB2011] 3 HII 09 55 49.69 +69 40 45.2           ~ 8 0
19 [MMW2002] 40.96+57.9 Rad 09 55 49.720 +69 40 43.84           ~ 3 0
20 [GIB2011] 5 HII 09 55 49.92 +69 40 42.5           ~ 6 0
21 [HTC94] 29 SNR 09 55 50.041 +69 40 44.57           ~ 19 0
22 [FBM2010] 41.30+59.6 SNR 09 55 50.050 +69 40 45.92           ~ 23 0
23 [RVZ2004] 41.62+59.9 Rad 09 55 50.38 +69 40 45.9           ~ 2 0
24 CXOM82 J095550.9+694044 HXB 09 55 50.690 +69 40 43.76           ~ 96 0
25 [MMW2002] 42.08+58.4 Rad 09 55 50.832 +69 40 44.34           ~ 3 0
26 [FMB2008] 42.20+59.1 HII 09 55 50.94 +69 40 45.3           ~ 28 1
27 [MMW2002] 42.48+58.4 Rad 09 55 51.230 +69 40 44.29           ~ 4 0
28 [MMW2002] 42.56+58.0 Rad 09 55 51.304 +69 40 43.98           ~ 3 0
29 [FBM2010] 42.67+55.6 SNR 09 55 51.390 +69 40 41.80           ~ 16 0
30 [FMB2008] 42.69+58.2 HII 09 55 51.44 +69 40 44.3           ~ 4 0
31 [RVZ2004] 43.00+59.0 SR? 09 55 51.74 +69 40 44.9           ~ 1 0
32 [RVZ2004] 43.21+61.3 Rad 09 55 51.95 +69 40 47.2           ~ 2 0
33 [FBM2010] 43.31+59.2 SNR 09 55 52.030 +69 40 45.42           ~ 32 0
34 [RVZ2004] 43.39+62.6 SNR 09 55 52.14 +69 40 48.7           ~ 3 0
35 [MPW94] 43.55+60.0 Rad 09 55 52.2 +69 40 46           ~ 3 0
36 [RVZ2004] 43.50+61.2 Rad 09 55 52.24 +69 40 47.1           ~ 1 0
37 [RVZ2004] 43.65+57.7 Rad 09 55 52.38 +69 40 43.6           ~ 1 0
38 M 82 AGN 09 55 52.430 +69 40 46.93 9.61 9.30 8.41     ~ 5866 6
39 NAME 44.0+59.5 SNR 09 55 52.730 +69 40 45.78           ~ 45 1
40 [RVZ2004] 44.08+63.1 Rad 09 55 52.82 +69 40 49.0           ~ 1 0
41 [RVZ2004] 44.11+64.3 SR? 09 55 52.85 +69 40 50.2           ~ 1 0
42 [RVZ2004] 44.17+64.4 Rad 09 55 52.91 +69 40 50.3           ~ 1 0
43 [FBM2010] 44.28+59.3 SNR 09 55 52.990 +69 40 45.49           ~ 18 0
44 [FBM2010] 44.34+57.8 SNR 09 55 53.050 +69 40 43.94           ~ 5 0
45 [RVZ2004] 44.43+62.5 Rad 09 55 53.16 +69 40 48.4           ~ 1 0
46 [FBM2010] 44.51+58.2 SNR 09 55 53.230 +69 40 44.36           ~ 19 0
47 [RVZ2004] 44.50+65.3 Rad 09 55 53.24 +69 40 51.2           ~ 1 0
48 [RVZ2004] 44.84+61.8 Rad 09 55 53.57 +69 40 47.6           ~ 1 0
49 [FBM2010] 44.89+61.2 SNR 09 55 53.610 +69 40 47.36           ~ 12 0
50 [MMW2002] 44.93+63.9 HII 09 55 53.64 +69 40 50.0           ~ 4 0
51 [FBM2010] 45.17+61.2 SNR 09 55 53.880 +69 40 47.43 20.412 20.009 19.315   18.763 ~ 28 0
52 [FBM2010] 45.39+60.3 Rad 09 55 54.070 +69 40 46.50           ~ 3 0
53 [FBM2010] 45.42+64.7 SNR 09 55 54.130 +69 40 53.58           ~ 19 0
54 [RVZ2004] 45.63+66.9 Rad 09 55 54.36 +69 40 52.7           ~ 1 0
55 [HTC94] 44 SR? 09 55 54.376 +69 40 48.97           ~ 2 0
56 [FBM2010] 45.75+65.3 SNR 09 55 54.460 +69 40 51.43           ~ 19 0
57 [FBM2010] 45.89+63.9 SNR 09 55 54.5322387360 +69 40 49.332992124           ~ 16 0
58 [RVZ2004] 45.93+74.3 Rad 09 55 54.66 +69 41 00.1           ~ 1 0
59 [RVZ2004] 46.17+67.6 HII 09 55 54.89 +69 40 53.8           ~ 7 0
60 [RVZ2004] 46.33+66.2 Rad 09 55 55.05 +69 40 52.0           ~ 1 0
61 [FBM2010] 46.52+63.9 SNR 09 55 55.220 +69 40 50.01           ~ 20 0
62 [FBM2010] 46.56+73.8 SNR 09 55 55.2461826408 +69 41 00.756320928           ~ 9 0
63 [FBM2010] 46.70+67.1 SNR 09 55 55.410 +69 40 53.17           ~ 20 0
64 [RVZ2004] 46.74+69.7 GlC 09 55 55.51 +69 40 55.8 24.275 23.213 21.502   19.693 ~ 2 0
65 [RVZ2004] 47.11+66.3 Rad 09 55 55.82 +69 40 52.1           ~ 1 0
66 [MMW2002] 47.37+68.0 SNR 09 55 56.07 +69 40 54.0           ~ 7 0
67 6C 104451+715930 QSO 10 48 27.61992778 +71 43 35.9384142     19.0 17.49   ~ 241 1
68 3C 286 Sy1 13 31 08.2883506368 +30 30 32.960091564   17.51 17.25     ~ 4349 2
69 M 83 SBG 13 37 00.91920 -29 51 56.7400 8.85 8.11 7.52 7.21   ~ 2579 2
70 IC 4553 SyG 15 34 57.22396 +23 30 11.6084   14.76 13.88     ~ 2962 4

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