2005ApJ...632..736A


Query : 2005ApJ...632..736A

2005ApJ...632..736A - Astrophys. J., 632, 736-750 (2005/October-3)

The X-ray spectral properties of SCUBA galaxies.

ALEXANDER D.M., BAUER F.E., CHAPMAN S.C., SMAIL I., BLAIN A.W., BRANDT W.N. and IVISON R.J.

Abstract (from CDS):

Deep SCUBA surveys have uncovered a large population of massive submillimeter-emitting galaxies (SMGs; f850µm≳4 mJy) at z≳1. Although it is generally believed that these galaxies host intense star formation activity, there is growing evidence that a substantial fraction also harbor an active galactic nucleus (AGN; i.e., an accreting super-massive black hole [SMBH]). We present here possibly the strongest evidence for this viewpoint to date: the combination of ultradeep X-ray observations (the 2 Ms Chandra Deep Field-North) and deep Keck spectroscopic data of SMGs with radio counterparts. We find that the majority (~75%) of these radio-selected spectroscopically identified SMGs host AGN activity; the other ~25% have X-ray properties consistent with star formation (X-ray-derived star formation rates of ~1300-2700 M☉/yr. The AGNs have properties generally consistent with those of nearby luminous AGNs (Γ~1.8±0.5, NH~1020-1024/cm2, and LX~1043-1044.5 ergs/s), and the majority (~80%) are heavily obscured (NH≳1023/cm2). We construct composite rest-frame 2-20 keV spectra for three different obscuration classes [NH<1023/cm2, NH=(1-5)x1023/cm2, and NH>5x1023/cm2], which reveal features not seen in the individual X-ray spectra. An ~1 keV equivalent width Fe Kα emission line is seen in the composite X-ray spectrum of the most heavily obscured AGNs, suggesting Compton-thick or near Compton-thick absorption. Even taking into account the effects of absorption, we find that the average X-ray to far-IR luminosity ratio of the AGN-classified SMGs (LX/LFIR=0.004) is approximately 1 order of magnitude below that found for typical quasars. This result suggests that intense star formation activity (of order ~1000 M☉/yr) dominates the bolometric output of these SMGs. However, we also explore the possibility that the X-ray to far-IR luminosity ratio of the AGN components is intrinsically less than that found for typical quasars and postulate that some SMGs may be AGN dominated. We investigate the implications of our results for the growth of massive black holes, discuss the prospects for deeper X-ray observations, and explore the scientific potential offered by the next generation of X-ray observatories.

Abstract Copyright: ∼

Journal keyword(s): Galaxies: Active - Galaxies: Starburst - Infrared: Galaxies - X-Rays: Galaxies

Nomenclature: Table 1: [ABC2005] JHHMMSS.ss+DDMMSS.s N=20.

Simbad objects: 30

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Number of rows : 30
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 M 77 Sy2 02 42 40.7091669408 -00 00 47.859690204 9.70 9.61 8.87 10.1 9.9 ~ 4897 2
2 IRAS 09104+4109 Sy2 09 13 45.4951283928 +40 56 28.215343572   19.69 19.21     ~ 260 1
3 NGC 2992 Sy2 09 45 42.045 -14 19 34.90 13.54 13.14 12.18 12.6 12.2 ~ 951 3
4 [VV96] J102434.5+470911 Sy1 10 24 34.5 +47 09 11     20.5     ~ 489 0
5 NGC 3256 Sy2 10 27 51.284 -43 54 13.55   11.83 11.33 10.62 11.9 ~ 920 2
6 NAME SMM J123549.44+621536.8 rG 12 35 49.43 +62 15 36.8 24.6 23.9 23.6 23.3 23.1 ~ 63 0
7 NAME SMM J123553.3+621338 rG 12 35 53.27 +62 13 37.6   24.8     23.89 ~ 22 1
8 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
9 NAME SMM J123600.2+621047 QSO 12 36 00.15 +62 10 47.2 24.21 25.5874 25.35   24.6340 ~ 53 0
10 NAME SMM J123606.72+621550.7 QSO 12 36 06.703 +62 15 50.97 23.8 23.3   23.21 23.2659 ~ 31 0
11 NAME SMM J123606.9+621021 rG 12 36 06.87 +62 10 21.5 26.74 27.3812 25.57 24.4 24.5585 ~ 55 0
12 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
13 NAME SMM J123618+621554 rG 12 36 18.32 +62 15 50.5 25.84   25.58 25.07 25.0 ~ 68 0
14 [WCB2004] GOODS 850-15a mm 12 36 21.101 +62 17 09.60           ~ 35 0
15 NAME SMM J123621.3+621708 rG 12 36 21.25 +62 17 08.3   25.1     25.0 ~ 54 0
16 NAME SMM J123622+621618 rG 12 36 22.68 +62 16 29.8 25.75 25.3095   24.8 24.6612 ~ 57 0
17 NAME SMM J123629.13+621045.8 Sy2 12 36 29.172 +62 10 46.53 25.66 25.4122 25.81 23.50 22.7656 ~ 61 0
18 NAME SMM J123632.61+620800.1 Sy2 12 36 32.57 +62 07 59.8 23.71 24.1097 24.65 24.0 23.7465 ~ 42 0
19 NAME MM J123633+6214.1 G 12 36 33.2 +62 14 07           ~ 74 0
20 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
21 NAME SMM J123635.6+621424 Sy1 12 36 35.588 +62 14 24.32 24.41 24.0665 24.46 23.8 23.2789 ~ 88 0
22 NAME SMM J123636.75+621156.1 AGN 12 36 36.762 +62 11 56.40 24.78 24.1589 23.412 21.81 21.9886 ~ 51 0
23 NAME Chandra Deep Field-North reg 12 36.8 +62 13           ~ 686 0
24 NAME Hubble Deep Field reg 12 36 49.5 +62 12 58           ~ 1967 1
25 NAME SMM J123707.2+621408 rG 12 37 07.19 +62 14 08.0 28.12 26.8993 26.6 25.6 25.3860 ~ 114 0
26 NAME SMM J123712.0+621325 rG 12 37 12.000 +62 13 25.83 25.92 26.0414 26.2 25.6 25.1091 ~ 70 2
27 NAME SMM J123712.1+621212 rG 12 37 12.06 +62 12 11.9 27.8 27.4458 27.3 26.1 25.9429 ~ 42 0
28 QSO B1235+6219 QSO 12 37 16.0012375248 +62 03 23.351091948 19.9 20.55 20.19 19.9 19.5 ~ 64 0
29 NAME SMM J123721.87+621035.3 Sy2 12 37 21.837 +62 10 36.05 24.2 23.8312 23.80 22.8 21.8676 ~ 43 0
30 NGC 6240 Sy2 16 52 58.9 +02 24 03   14.31 13.37     ~ 1734 2

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