2011MNRAS.410.1687D


Query : 2011MNRAS.410.1687D

2011MNRAS.410.1687D - Mon. Not. R. Astron. Soc., 410, 1687-1702 (2011/January-3)

The properties of the interstellar medium within a star-forming galaxy at z= 2.3.

DANIELSON A.L.R., SWINBANK A.M., SMAIL I., COX P., EDGE A.C., WEISS A., HARRIS A.I., BAKER A.J., DE BREUCK C., GEACH J.E., IVISON R.J., KRIPS M., LUNDGREN A., LONGMORE S., NERI R. and OCANA FLAQUER B.

Abstract (from CDS):

We present an analysis of the molecular and atomic gas emission in the rest-frame far-infrared and submillimetre from the lensed z= 2.3 submillimetre galaxy SMM J2135-0102. We obtain very high signal-to-noise ratio detections of 11 transitions from three species and limits on a further 20 transitions from nine species. We use the 12CO, [C I] and HCN line strengths to investigate the gas mass, kinematic structure and interstellar medium (ISM) chemistry and find strong evidence for a two-phase medium within this high-redshift starburst galaxy, comprising a hot, dense, luminous component and an underlying extended cool, low-excitation massive component. Employing a suite of photodissociation region models, we show that on average the molecular gas is exposed to an ultraviolet (UV) radiation field that is ∼ 1000 times more intense than the Milky Way, with star-forming regions having a characteristic density of n ∼ 104/cm3. Thus, the average ISM density and far-UV radiation field intensity are similar to those found in local ultraluminous infrared galaxies (ULIRGs) and to those found in the central regions of typical starburst galaxies, even though the star formation rate is far higher in this system. The 12CO spectral line energy distribution and line profiles give strong evidence that the system comprises multiple kinematic components with different conditions, including temperature, and line ratios suggestive of high cosmic-ray flux within clouds, likely as a result of high star formation density. We find tentative evidence of a factor of ∼ 4 temperature range within the system. We expect that such internal structures are common in high-redshift ULIRGs but are missed due to the poor signal-to-noise ratio of typical observations. We show that, when integrated over the galaxy, the gas and star formation surface densities appear to follow the Kennicutt–Schmidt relation, although by comparing our data to high-resolution submillimetre imaging, our data suggest that this relation breaks down on scales of <100 pc. By virtue of the lens amplification, these observations uncover a wealth of information on the star formation and ISM at z ∼ 2.3 at a level of detail that has only recently become possible at z < 0.1 and show the potential physical properties that will be studied in unlensed galaxies when the Atacama Large Millimeter Array is in full operation.

Abstract Copyright: 2010 The Authors. Journal compilation2010 RAS

Journal keyword(s): galaxies: active - galaxies: evolution - galaxies: high-redshift - galaxies: starburst - submillimetre: galaxies

Simbad objects: 14

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Number of rows : 14
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 253 SyG 00 47 33.134 -25 17 19.68   8.03   6.94 8.1 ~ 3335 2
2 NAME SMM J02399-0136 G 02 39 51.87 -01 35 58.8       21.20   ~ 191 2
3 M 82 AGN 09 55 52.430 +69 40 46.93 9.61 9.30 8.41     ~ 5858 6
4 NAME Sextans dSph G 10 13 02.9 -01 36 53   12 10.4     ~ 853 0
5 NAME SMM J123711+622212 AGN 12 37 11.92 +62 22 12.1   27.1786 25.185   24.4196 ~ 206 0
6 Mrk 231 Sy1 12 56 14.2341182928 +56 52 25.238373852   14.68 13.84     ~ 1987 3
7 QSO J1415+1129 QSO 14 15 46.25 +11 29 43.4   17.63 17.23     ~ 650 0
8 IC 4553 SyG 15 34 57.22396 +23 30 11.6084   14.76 13.88     ~ 2961 4
9 NAME SMM J16359+6613 G 16 35 55.62 +66 12 59.5           ~ 60 1
10 NGC 6240 Sy2 16 52 58.9 +02 24 03   14.31 13.37     ~ 1637 2
11 EM* MWC 349 ** 20 32 45.499080 +40 39 36.74124   15.88 13.15 12.13   Bep 801 0
12 2SLAQ J213402.24+002416.2 QSO 21 34 02.2392164616 +00 24 16.255758816   21.45 21.04     ~ 4 0
13 NAME Eyelash LeG 21 35 11.60 -01 02 52.0           ~ 228 0
14 ClG J2135-0102 ClG 21 35 12.00 -01 03 00.1           ~ 61 0

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