2008A&A...484..631V


Query : 2008A&A...484..631V

2008A&A...484..631V - Astronomy and Astrophysics, volume 484, 631-653 (2008/6-4)

Modelling the spectral energy distribution of ULIRGs. II. The energetic environment and the dense interstellar medium.

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

Abstract (from CDS):

By using the spectral energy distribution (SED) from the near-infrared to the radio of a statistically significant number of luminous infrared galaxies we determine important physical parameters for this population of objects. In particular we constrain the optical depth towards the luminosity source, the star formation rate, the star formation efficiency and the AGN fraction. We fit the near-infrared to radio spectral energy distributions of a sample of 30 luminous and ultra-luminous infrared galaxies with pure starburst models or models that include both starburst and AGN components. We find that although about half of our sample have best-fit models that include an AGN component, only 30% (9/30) have an AGN that accounts for more than 10% of the infrared luminosity from 8 to 1000µm, whereas all have an energetically dominant starburst. Our derived AGN fractions are generally in good agreement with measurements of the mid-infrared line ratios, Ne[V]/Ne[II] and O[IV]/Ne[II] by Spitzer IRS, but much lower than those derived from PAH equivalent widths or the mid-infrared spectral slope. Our models determine the mass of dense molecular gas within which active star formation takes place via the extinction required to reproduce the infrared part of the SED. Assuming that this mass is that traced by the HCN molecule, we reproduce the observed linear relation between HCN flux and infrared luminosity found previously. We also find that the star formation efficiency, as defined by the current star formation rate per unit molecular gas mass, falls as the starburst ages. If the evolution of ULIRGs includes a phase in which an AGN contributes an important fraction to the infrared luminosity, this phase should last an order of magnitude less time than the starburst phase. However, we find no convincing evidence that an energetically important AGN is associated with a particular phase of the starburst. Because the mass of dense molecular gas that we derive is consistent with observations of the HCN molecule, it should be possible to estimate the mass of dense, star-forming molecular gas in such objects when molecular line data are not available.

Abstract Copyright:

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

CDS comments: Paragraph 5.1 IRAS 15250+3909 is a probable misprint for IRAS 15250+3609.

Simbad objects: 40

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Number of rows : 40
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 34 Sy2 00 11 06.612 -12 06 28.33   14.14 13.52     ~ 350 0
2 IC 1623 IG 01 07 47.380 -17 30 24.51   15       ~ 310 2
3 Z 436-30 LIN 01 20 02.654 +14 21 41.73   14.9       ~ 153 0
4 IRAS 01364-1042 LIN 01 38 52.890 -10 27 11.35   16.77   15.74   ~ 117 0
5 ZW III 35 Sy2 01 44 30.516 +17 06 09.18   15.24 14.81     ~ 249 0
6 UGC 2369 PaG 02 54 00.9 +14 58 31   14.6       ~ 115 1
7 UGC 2369 S GiP 02 54 01.80 +14 58 14.0           ~ 101 1
8 IRAS 03359+1523 G 03 38 47.1918750504 +15 32 53.853117504   16.3       ~ 106 0
9 NGC 1614 Sy1 04 34 00.027 -08 34 44.57   14.66 13.99     ~ 667 0
10 LEDA 17155 Sy2 05 21 01.3994605776 -25 21 45.321827832   15.47 14.75     ~ 498 0
11 NGC 2623 LIN 08 38 24.016 +25 45 16.29 14.10 13.99 13.36     ~ 498 1
12 NAME IRAS F08572+3915 NW LIN 09 00 25.364 +39 03 54.23     16.66     ~ 420 1
13 UGC 4881 IG 09 15 55.5 +44 19 58   14.9       ~ 169 0
14 UGC 5101 Sy2 09 35 51.6045544584 +61 21 11.589382368   15.20 15.50     ~ 572 4
15 NVSS J102000+081335 rG 10 20 00.1849825704 +08 13 33.648546108   17.5       ~ 157 1
16 LEDA 33083 LIN 10 59 18.128 +24 32 34.74   15.7       ~ 274 1
17 APG 148 IG 11 03 54.0 +40 51 00   14.29       ~ 177 1
18 IC 2810 AGN 11 25 45.055 +14 40 35.98   15.4       ~ 126 0
19 IC 2810b AGN 11 25 49.5408391632 +14 40 06.610250208   15.4       ~ 40 0
20 IC 694 AG? 11 28 27.312 +58 34 42.29   18.2       ~ 252 2
21 UGC 6472 C G 11 28 30.70 +58 33 48.4           ~ 351 0
22 NGC 3690 IG 11 28 31.0 +58 33 41   13.19 12.86     ~ 978 4
23 GSW B1 PoG 11 28 31.0 +58 33 41           ~ 39 1
24 NAME NGC 3690 West GiP 11 28 31.02 +58 33 40.7   11.8       ~ 629 4
25 NAME NGC 3690 East AGN 11 28 33.07 +58 33 54.2   11.8       ~ 631 4
26 LEDA 39024 LIN 12 13 46.107 +02 48 41.50           ~ 354 1
27 Mrk 231 Sy1 12 56 14.2341182928 +56 52 25.238373852   14.68 13.84     ~ 1989 3
28 IC 883 SBG 13 20 35.4 +34 08 22   14.8       ~ 400 1
29 NGC 5256 PaG 13 38 17.81 +48 16 41.2   14.1 13.42     ~ 430 1
30 Mrk 273 Sy2 13 44 42.1781 +55 53 12.819   15.68 14.91     ~ 913 3
31 NGC 5544 GiP 14 17 02.5231177296 +36 34 17.716954440   13.2       ~ 81 0
32 LEDA 52270 Sy1 14 37 38.2867288488 -15 00 24.087592692   16.58 16.40     ~ 276 1
33 Z 221-50 SyG 15 18 06.1187 +42 44 45.086   15.0 15     ~ 219 1
34 2MASX J15265942+3558372 LIN 15 26 59.442 +35 58 37.01   15.61       ~ 272 1
35 IC 4553 SyG 15 34 57.22396 +23 30 11.6084   14.76 13.88     ~ 2961 4
36 APG 293 G 16 58 27.8 +58 56 48           ~ 113 0
37 NGC 6286 GiG 16 58 31.3566512040 +58 56 10.114753560   14.2       ~ 186 1
38 NGC 7469 Sy1 23 03 15.6 +08 52 26 12.60 13.00 12.34     ~ 2096 3
39 IC 5298 Sy2 23 16 00.6756811155 +25 33 24.081139422   15.0       ~ 193 0
40 Mrk 331 GiP 23 51 26.731 +20 35 10.22   14.9       ~ 227 0

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