2013MNRAS.435.1493A


Query : 2013MNRAS.435.1493A

2013MNRAS.435.1493A - Mon. Not. R. Astron. Soc., 435, 1493-1510 (2013/October-3)

Using [CI] to probe the interstellar medium in z ∼ 2.5 sub-millimeter galaxies.

ALAGHBAND-ZADEH S., CHAPMAN S.C., SWINBANK A.M., SMAIL I., DANIELSON A.L.R., DECARLI R., IVISON R.J., MEIJERINK R., WEISS A. and VAN DER WERF P.P.

Abstract (from CDS):

We present new [Ci](1-0) and 12CO(4-3) Plateau de Bure Interferometer observations of five sub-millimeter galaxies (SMGs) and combine these with all available [Ci](1-0) literature detections in SMGs to probe the gas distribution within a sample of 14 systems. We explore the [Ci](1-0) properties of the SMG population, particularly investigating the ratio of the [Ci](1-0) luminosity to various 12CO transition and far-infrared luminosities. We find that the SMGs with new observations extend the spread of L[Ci](1-0)/LFIR to much higher values than found before, with our complete sample providing a good representation of the diverse z > 2 SMG population. We compare the line ratios to the outputs of photodissociation region (PDR) models to constrain the physical conditions in the interstellar medium (ISM) of the SMGs, finding an average density of <log(n/cm-3)> = 4.3±0.2 and an average radiation field (in terms of the local field value, G0) of <log(G0)> = 3.9±0.4. Overall, we find the SMGs are most comparable to local ultraluminous infrared galaxies (ULIRGs) in G0 and n; however, a significant tail of 5 of the 14 SMGs are likely best compared to less compact, local starburst galaxies, providing new evidence that many SMGs have extended star formation distributions and are therefore not simply scaled up versions of local ULIRGs. We derive the ISM properties of a sample of quasars also finding that they have higher densities and radiation fields on average than the SMGs, consistent with the more extreme local ULIRGs, and reinforcing their interpretation as transition objects. We explore the limitations of using simple PDR models to understand [Ci], which may be concomitant with the bulk H2 mass rather than PDR distributed. We therefore also assess [Ci] as a tracer of H2, finding that for our sample SMGs, the H2 masses derived from [Ci] are often consistent with those determined from low excitation 12CO. We conclude that [Ci] observations provide a useful tool to probe the bulk gas and gas processes occurring within merging SMGs, however more detailed, resolved observations are required to fully exploit [Ci] as a diagnostic.

Abstract Copyright: © 2013 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society (2013)

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

Nomenclature: Fig. 3, Table 1: [ACS2013] SXDF4a (Nos a-b).

CDS comments: p.1495, 1749-096 is a probable misprint for (QSO B)1749+096. ID 141 = H-ATLAS J142413.9+022304 in Simbad. SA 22.96 = NAME SMM J221804.42+002154.4 in Simbad.

Simbad objects: 35

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Number of rows : 35
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 4C 01.02 Bla 01 08 38.77110544 +01 35 00.3171844   18.54 18.39 19.05   ~ 589 1
2 QSO B0130-17 Bla 01 32 43.48746292 -16 54 48.5220804   18.75 18.44 15.44   ~ 247 1
3 1RXS J014126.8-092857 BLL 01 41 25.83216015 -09 28 43.6742470   16.94 16.55 17.21   ~ 302 1
4 [CCM2006] SXDF850.11 G 02 17 25.117 -04 59 37.44           ~ 13 0
5 AS2UDS J021738.68-050339.57 rG 02 17 38.675793 -05 03 39.56548   25.66119 21.4657 24.97221   ~ 19 0
6 [ACS2013] SXDF4a G 02 17 38.75 -05 03 38.3           ~ 1 0
7 [CCM2006] SXDF850.7 G 02 17 38.921 -05 05 23.72           ~ 11 0
8 [ACS2013] SXDF4b G 02 17 38.95 -05 03 43.3           ~ 1 0
9 QSO B0237-027 Bla 02 39 45.47227239 -02 34 40.9145702   19.5 21 19.04   ~ 145 1
10 NAME SMM J02399-0136 rG 02 39 51.87 -01 35 58.8       21.20   ~ 201 2
11 M 77 Sy2 02 42 40.7091669408 -00 00 47.859690204 9.70 9.61 8.87 10.1 9.9 ~ 4897 2
12 NAME Ori A MoC 05 38 -07.1           ~ 3187 0
13 NAME Ori B MoC 05 41 43.0 -01 54 44           ~ 1498 0
14 M 82 AGN 09 55 52.430 +69 40 46.93 9.61 9.30 8.41     ~ 6156 6
15 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
16 Z 294-4 Sy1 12 56 14.2341182928 +56 52 25.238373852   14.68 13.84     ~ 2096 3
17 BRI B1335-0417 G 13 38 03.4151935680 -04 32 34.981751112   19.4       ~ 112 0
18 NAME SMM J14011+0252 rG 14 01 04.95 +02 52 24.0           ~ 156 1
19 QSO J1415+1129 QSO 14 15 46.25 +11 29 43.4   17.63 17.23     ~ 678 0
20 NAME G15.v2.779 LeG 14 24 13.9 +02 23 04           ~ 59 0
21 IC 1127 SyG 15 34 57.22396 +23 30 11.6084   14.76 13.88     ~ 3090 4
22 NAME SMM J16359+6613 G 16 35 55.62 +66 12 59.5           ~ 62 1
23 NAME SMM J163650.43+405734.5 Sy1 16 36 50.5 +40 57 34   23.3 23.30   21.83 ~ 91 0
24 NAME SMM J16366+4105 AGN 16 36 58.2 +41 05 24   26.0     24.48 ~ 56 0
25 NGC 6240 Sy2 16 52 58.9 +02 24 03   14.31 13.37     ~ 1734 2
26 LDN 57 DNe 17 22 38.2 -23 49 34           ~ 336 1
27 NAME Galactic Center reg 17 45 39.60213 -29 00 22.0000           ~ 16269 0
28 4C 09.57 BLL 17 51 32.81857326 +09 39 00.7284066   17.46 16.78 15.57   ~ 1007 1
29 [LWB2009] MM184222+593828 LeG 18 42 22.32 +59 38 29.6           ~ 21 0
30 EM* MWC 349 ** 20 32 45.499080 +40 39 36.74124   15.88 13.15 12.13   Bep 837 0
31 NAME Eyelash LeG 21 35 11.60 -01 02 52.0           ~ 245 0
32 NAME SMM J221804.42+002154.4 G 22 18 04.42 +00 21 54.4   25.2     23.07 ~ 15 0
33 3C 446 BLL 22 25 47.25929101 -04 57 01.3907626   18.83 18.39 16.3   ~ 863 1
34 3C 454.0 QSO 22 51 34.7277468096 +18 48 40.087264428   18.52 18.4     ~ 232 2
35 3C 454.3 Bla 22 53 57.7480438728 +16 08 53.561508864   16.57 16.10 15.22   ~ 3004 2

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