2008A&A...477...95C


Query : 2008A&A...477...95C

2008A&A...477...95C - Astronomy and Astrophysics, volume 47795-104 (2008/1-1)

Modeling the spectral energy distribution of ULIRGs. I. The radio spectra.

CLEMENS M.S., VEGA O., BRESSAN A., GRANATO G.L., SILVA L. and PANUZZO P.

Abstract (from CDS):

We aim to constrain new starburst/AGN models of IRAS bright galaxies via their spectral energy distribution from the near-infrared to the radio. To this end, we determine the radio spectra for a sample of 31 luminous and ultraluminous IRAS galaxies (LIRGs/ULIRGs). We present here new high frequency VLA observations at 22.5GHz and 8.4GHz and also derive fluxes at other radio frequencies from archival data. Together with radio data from the literature, we construct the radio spectrum for each source. In the selection of data we have made every effort to ensure that these fluxes neither include contributions from nearby objects, nor underestimate the flux due to high interferometer resolution. From our sample of well-determined radio spectra we find that very few have a straight power-law slope. Although some sources show a flattening of the radio spectral slope at high frequencies, the average spectrum shows a steepening of the radio spectrum from 1.4 to 22.5GHz. This is unexpected, because in sources with high rates of star formation, we expect that flat spectrum, free-free emission will make a significant contribution to the radio flux at higher radio frequencies. Despite this trend, the radio spectral indices between 8.4 and 22.5GHz are flatter for sources with higher values of the far-infrared (FIR)-radio flux density ratio, q, when this is calculated at 8.4GHz. Therefore, sources that are deficient in radio emission relative to FIR emission (presumably younger sources) have a larger thermal component to their radio emission. However, we find no correlation between the radio spectral index between 1.4 and 4.8GHz and q at 8.4GHz. Because the low frequency spectral index is affected by free-free absorption, and this is a function of source size for a given mass of ionised gas, this is evidence that the ionised gas in ULIRGs shows a range of densities. The youngest LIRGs and ULIRGs are characterised by flatter average radio spectral indices from 1.4 to 22.5GHz, and by a larger contribution to their high frequency, radio spectra from free-free emission. However, the youngest sources are not those that have the greatest free-free absorption at low radio frequencies. The sources in which the effects of free-free absorption are strongest are instead the most compact sources. Although these have the warmest FIR colours, they are not necessarily the youngest sources.

Abstract Copyright: ∼

Journal keyword(s): dust, extinction - galaxies: active - infrared: galaxies - radio continuum: galaxies

Simbad objects: 36

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Number of rows : 36
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 NGC 17 Sy2 00 11 06.612 -12 06 28.33   14.14 13.52     ~ 369 1
2 IC 1623 IG 01 07 47.24 -17 30 25.0   15       ~ 338 2
3 Z 436-30 LIN 01 20 02.654 +14 21 41.73   14.9       ~ 176 1
4 3C 48 QSO 01 37 41.2996631208 +33 09 35.080388820   16.62 16.20     ~ 2924 2
5 IRAS 01364-1042 LIN 01 38 52.86288 -10 27 11.5848   16.77   15.74   ~ 132 0
6 ZW III 35 Sy2 01 44 30.516 +17 06 09.18   15.24 14.81     ~ 261 1
7 IRAS 03359+1523 G 03 38 47.1918750504 +15 32 53.853117504   16.3       ~ 112 0
8 NGC 1569 rG 04 30 49.186 +64 50 52.52 11.72 11.86 11.03     ~ 1297 3
9 NGC 1614 Sy1 04 34 00.027 -08 34 44.57   14.66 13.99     ~ 697 1
10 IRAS 05189-2524 Sy2 05 21 01.3994605776 -25 21 45.321827832   15.47 14.75     ~ 545 0
11 NGC 2623 LIN 08 38 24.016 +25 45 16.29 14.10 13.99 13.36     ~ 533 2
12 IRAS 08572+3915 LIN 09 00 25.38288 +39 03 54.2988     16.66     ~ 450 1
13 NVSS J102000+081335 rG 10 20 00.1849825704 +08 13 33.648546108   17.5       ~ 167 1
14 IRAS 10565+2448 LIN 10 59 18.12811 +24 32 34.7357   15.7       ~ 302 0
15 APG 148 IG 11 03 53.89153 +40 50 59.8850   14.29       ~ 190 1
16 IC 694 AG? 11 28 27.312 +58 34 42.29   18.2       ~ 258 2
17 NGC 3690C G 11 28 30.70 +58 33 48.4           ~ 351 0
18 NGC 3690 IG 11 28 31.0 +58 33 41   13.19 12.86     ~ 1015 4
19 NGC 3690B GiP 11 28 31.02 +58 33 40.7   11.8       ~ 635 4
20 NGC 3690NE AGN 11 28 33.07 +58 33 54.2   11.8       ~ 635 4
21 IRAS 12112+0305 PaG 12 13 45.98880 +02 48 39.9600           ~ 373 0
22 [CGM90] IRAS 12112+0305 NE rG 12 13 46.10735 +02 48 41.4959           ~ 369 0
23 Z 294-4 Sy1 12 56 14.2341182928 +56 52 25.238373852   14.68 13.84     ~ 2096 3
24 3C 286 Sy1 13 31 08.2883506368 +30 30 32.960091564   17.51 17.25     ~ 4558 2
25 NGC 5256 PaG 13 38 17.81 +48 16 41.2   14.1 13.42     ~ 449 1
26 LEDA 52270 Sy1 14 37 38.2867288488 -15 00 24.087592692   16.58 16.40     ~ 300 2
27 Z 221-50 SyG 15 18 06.1187 +42 44 45.086   15.0 15     ~ 239 1
28 2MASX J15265942+3558372 LIN 15 26 59.44451 +35 58 37.0521   15.61       ~ 295 1
29 IC 1127 SyG 15 34 57.22396 +23 30 11.6084   14.76 13.88     ~ 3090 4
30 NGC 6240 Sy2 16 52 58.9 +02 24 03   14.31 13.37     ~ 1734 2
31 NGC 6285 AGN 16 58 24.016 +58 57 21.23   15.3       ~ 117 0
32 APG 293 G 16 58 27.8 +58 56 48           ~ 115 0
33 NGC 6286 AGN 16 58 31.3566512040 +58 56 10.114753560   14.2       ~ 202 1
34 NGC 7469 Sy1 23 03 15.6 +08 52 26 12.60 13.00 12.34     ~ 2253 3
35 IC 5298 Sy2 23 16 00.6756811155 +25 33 24.081139422   15.0       ~ 205 0
36 Z 455-59 AGN 23 51 26.731 +20 35 10.22   14.9       ~ 237 0

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