2009ApJ...698.1380M


Query : 2009ApJ...698.1380M

2009ApJ...698.1380M - Astrophys. J., 698, 1380-1397 (2009/June-3)

Balancing the energy budget between star formation and active galactic nuclei in high-redshift infrared luminous galaxies.

MURPHY E.J., CHARY R.-R., ALEXANDER D.M., DICKINSON M., MAGNELLI B., MORRISON G., POPE A. and TEPLITZ H.I.

Abstract (from CDS):

We present deep Spitzer mid-infrared spectroscopy, along with 16, 24, 70, and 850 µm photometry, for 22 galaxies located in the Great Observatories Origins Deep Survey-North (GOODS-N) field. The sample spans a redshift range of 0.6 ≲ z ≲ 2.6, 24 µm flux densities between ∼0.2 and 1.2 mJy, and consists of submillimeter galaxies (SMGs), X-ray or optically selected active galactic nuclei (AGNs), and optically faint (zAB> 25 mag) sources. We find that infrared (IR; 8-1000 µm) luminosities derived by fitting local spectral energy distributions (SEDs) with 24 µm photometry alone are well matched to those when additional mid-infrared spectroscopic and longer wavelength photometric data are used for galaxies having z ≲ 1.4 and 24 µm-derived IR luminosities typically ≲3x1012 L☉. However, for galaxies in the redshift range between 1.4 ≲ z ≲ 2.6, typically having 24-µm-derived IR luminosities ≳3x1012 L☉, IR luminosities are overestimated by an average factor of ∼5 when SED fitting with 24 µm photometry alone. This result arises partly due to the fact that high-redshift galaxies exhibit aromatic feature equivalent widths that are large compared to local galaxies of similar luminosities. Using improved estimates for the IR luminosities of these sources, we investigate whether their infrared emission is found to be in excess relative to that expected based on extinction-corrected UV star formation rates (SFRs), possibly suggesting the presence of an obscured AGN. Through a spectral decomposition of mid-infrared spectroscopic data, we are able to isolate the fraction of IR luminosity arising from an AGN as opposed to star formation activity. This fraction is only able to account for ∼30% of the total IR luminosity among the entire sample and ∼35% of the "excess" IR emission among these sources, on average, suggesting that AGNs are not the dominant cause of the inferred "mid-infrared excesses" in these systems. Of the sources identified as having mid-infrared excesses, half are accounted for by using proper bolometric corrections while half show the presence of obscured AGNs. This implies sky and space densities for Compton-thick AGNs of ∼1600/deg2 and ∼1.3x10–4/Mpc3, respectively. We also note that IR luminosities derived from SED fitting the mid-infrared and 70 µm broadband photometry agree within ∼50% to those values estimated using the additional mid-infrared spectroscopic and submillimeter data. An inspection of the far-infrared (FIR)-radio correlation shows no evidence for evolution over this redshift range. However, we find that the SMGs have IR/radio ratios which are a factor of ∼3 lower, on average, than what is measured for star-forming galaxies in the local universe.

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Journal keyword(s): galaxies: evolution - infrared: galaxies - radio continuum: galaxies

Nomenclature: Tables 1-6: [MCA2009] NN (Nos 1-22).

Simbad objects: 25

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Number of rows : 25
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 NAME SMM J123555.14+620901.7 rG 12 35 55.14 +62 09 01.7 24.4 24.2 24.1 23.8 23.5 ~ 36 0
2 NAME SMM J123600.2+621047 QSO 12 36 00.15 +62 10 47.2 24.21 25.5874 25.35   24.6340 ~ 53 0
3 SDSS J123603.25+621111.1 rG 12 36 03.26 +62 11 10.9 23.10 22.3841 21.664 20.72 20.3027 ~ 46 0
4 NAME SMM J123616.15+621513.7 rG 12 36 16.11 +62 15 13.7 27.8 25.8257 25.78 25.3 26.6108 ~ 67 0
5 NAME SMM J123618+621554 rG 12 36 18.32 +62 15 50.5 25.84   25.58 25.07 25.0 ~ 68 0
6 NAME SMM J123618+621009 rG 12 36 19.12 +62 10 04.3 26.78         ~ 25 0
7 [WCB2004] GOODS 850-15a mm 12 36 21.101 +62 17 09.60           ~ 35 0
8 NAME SMM J123621.3+621708 rG 12 36 21.25 +62 17 08.3   25.1     25.0 ~ 54 0
9 SDSS J123622.50+621544.4 rG 12 36 22.50 +62 15 44.5 22.30 22.0680   20.74 20.4127 ~ 41 0
10 NAME SMM J123622+621618 rG 12 36 22.68 +62 16 29.8 25.75 25.3095   24.8 24.6612 ~ 57 0
11 SDSS J123633.24+620834.6 rG 12 36 33.246 +62 08 34.60 22.72 22.6031 22.487 21.92 21.5009 ~ 37 0
12 NAME SMM J123635+621239 rG 12 36 34.528 +62 12 41.39 25.26 23.8632 24.53 23.18 22.7131 ~ 126 0
13 GOODS J123637.03+620852.4 rG 12 36 37.04 +62 08 52.4 27.4 27.3 26.7     ~ 18 0
14 NAME SMM J123653+621119 rG 12 36 53.27 +62 11 16.7 25.34 23.6391 24.17 22.08 21.7685 ~ 33 0
15 NAME GOODS-N Field reg 12 36 55.0 +62 14 15           ~ 1364 1
16 CXO J123655.8+620807 rG 12 36 55.96 +62 08 08.2 25.50 25.2014   22.6 21.5716 ~ 35 0
17 GOODS J123656.47+621937.6 QSO 12 36 56.48 +62 19 37.7           ~ 16 0
18 NAME SMM J123701+621148 rG 12 37 01.58 +62 11 46.4 28.69 25.8 25.7 25.30 25.30 ~ 55 1
19 CXOHDFN J123704.2+621446 Sy2 12 37 04.34 +62 14 46.1 24.55 24.4432 24.97 24.5 24.4307 ~ 46 0
20 NAME SMM J123711.32+621331.3 rG 12 37 11.35 +62 13 31.0 25.3 24.9032   23.8 24.7226 ~ 59 1
21 SDSS J123716.59+621643.9 rG 12 37 16.63 +62 16 43.4 24.30 23.4089 23.44 21.98 22.2000 ~ 38 0
22 GOODS J123718.27+622259.0 G 12 37 18.27062 +62 22 58.9890           ~ 5 0
23 CXO J123726.5+622026 rG 12 37 26.5080 +62 20 26.840 26.7 27.4128   25.1 24.9925 ~ 23 0
24 SDSS J123734.60+621723.2 rG 12 37 34.53 +62 17 23.2 24.90 23.8683 23.77 22.1 20.9187 ~ 30 0
25 Z 294-4 Sy1 12 56 14.2341182928 +56 52 25.238373852   14.68 13.84     ~ 2096 3

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