2005ApJ...635..853B


Query : 2005ApJ...635..853B

2005ApJ...635..853B - Astrophys. J., 635, 853-863 (2005/December-3)

The relationship between stellar and black hole mass in submillimeter galaxies.

BORYS C., SMAIL I., CHAPMAN S.C., BLAIN A.W., ALEXANDER D.M. and IVISON R.J.

Abstract (from CDS):

We analyze deep X-ray, optical, and mid-infrared Spitzer observations of the CDF-N/GOODS-N region to study a sample of 13 submillimeter-detected galaxies with spectroscopic redshifts (median z=2.2). These galaxies are among the most active and massive at this epoch. We find evidence for a power-law correlation between the estimated stellar and X-ray luminosity, implying that masses of the black holes may be related to the stellar masses of their host galaxies. We derive the rest-frame UV-near-infrared spectral energy distributions for these galaxies, believed to be young spheroids, and fit them with model templates. Using the rest-frame near-infrared luminosities, which are relatively insensitive to uncertainties in stellar ages and reddening in these young dusty galaxies, and theoretical mass-to-light ratios, we can estimate their stellar masses. Although the submillimeter emission implies that these galaxies are undergoing an epoch of intense star formation, the Spitzer data reveal a massive stellar population already in place. We find that our submillimeter galaxies have a median stellar mass of ∼1011 M☉, which is roughly 10 times more massive than typical UV-selected star-forming systems at similar redshifts. These stellar masses are then compared to previously published black hole mass estimates derived from the X-ray luminosities under the assumption of Eddington-limit accretion. We find that the black hole masses for our high-redshift sample are approximately 1-2 orders of magnitude smaller than galaxies of comparable stellar mass in the local universe. Although our estimates of black hole masses will increase if the accretion is sub-Eddington, and our stellar masses will decrease if we assume a much younger stellar population or a different initial mass function, we find that only through a combination of effects is it possible to shift the high-redshift galaxies such that they lie on the local relation. This suggests that the black holes need to grow substantially between z=2.2 and the present day, with much of the black hole growth occurring after the current obscured, far-infrared luminous phase of activity, which is likely associated with the formation of the spheroid. This interpretation supports a scenario in which submillimeter galaxies pass through a subsequent accretion-dominated phase, where they would appear as optically bright quasars.

Abstract Copyright: ∼

Journal keyword(s): Galaxies: Evolution - Galaxies: Formation - Galaxies: High-Redshift - Galaxies: Starburst

Simbad objects: 17

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Number of rows : 17
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 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
2 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
3 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
4 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
5 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
6 NAME SMM J123622+621618 rG 12 36 22.68 +62 16 29.8 25.75 25.3095   24.8 24.6612 ~ 57 0
7 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
8 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
9 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
10 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
11 NAME Chandra Deep Field-North reg 12 36.8 +62 13           ~ 686 0
12 NAME GOODS-N Field reg 12 36 55.0 +62 14 15           ~ 1364 1
13 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
14 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
15 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
16 QSO B1235+6219 QSO 12 37 16.0012375248 +62 03 23.351091948 19.9 20.55 20.19 19.9 19.5 ~ 64 0
17 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

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