2002A&A...391.1081V


Query : 2002A&A...391.1081V

2002A&A...391.1081V - Astronomy and Astrophysics, volume 391, 1081-1095 (2002/9-1)

The physical structure of Magellanic Cloud HII regions. II. Elemental abundances.

VERMEIJ R. and VAN DER HULST J.M.

Abstract (from CDS):

Based on a new data set of optical and infrared spectra described in Vermeij et al. (2002A&A...390..649V), we analyse the gas-phase elemental abundances of a sample of HII regions in the Large and Small Magellanic Cloud. The combined optical and infrared data set gives us access to all the ionization stages of astrophysically important elements such as sulfur and oxygen. We self-consistently determine the electron temperatures and densities for the O+, S++ and O++ ionization zones, and use these parameters in the derivation of the ionic fractions. We discuss the uncertainties on these ionic fractions. The different relations between the electron temperatures as proposed by Garnett (1992AJ....103.1330G) and Thuan et al. (1995ApJ...445..108T) are confronted with our results. We find our electron temperatures to be consistent with these relations, although the relation between Te[SIII] and Te[OIII] might be slightly steeper than predicted. We investigate the reliability of the Ionization Correction Factors (ICFs) used in the derivation of the full elemental abundances of sulfur and neon. We conclude that the prescription for the ICF used to derive the sulfur abundance as given by Stasinska (1978A&A....66..257S) for α=3 is accurate for O+/O>0.20. No conclusions could be drawn for neon. Avoiding the use of ICFs as much as possible, we then proceed to derive the full elemental abundances. We calculate a grid of general photoionization models to compare our results with the ``bright-line'' abundance diagnostics for oxygen (R23) and sulfur (S23(4)). The reliability of the newly proposed S234 parameter (Oey & Shields, 2000ApJ...539..687O) which includes emission lines from S+, S++ and S+3 is checked. We find a very good agreement between the S234 models and our analysis results. Finally, we compare the heavy element-to-oxygen ratios of our sample objects to those of giant HII regions in a large sample of low-metallicity blue dwarf galaxies (Izotov & Thuan, 1999ApJ...511..639I) and with the results from Kobulnicky & Skillman (1996ApJ...471..211K, 1997ApJ...489..636K) for the irregular galaxies NGC 1569 and NGC 4214.

Abstract Copyright:

Journal keyword(s): ISM: structure, abundances - ISM: lines and bands - HII regions - Magellanic Clouds

CDS comments: In table 1 N159-5 = [HT82] 5. N159-9 is a probable misprint for N159-5.

Simbad objects: 21

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Number of rows : 21
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2023
#notes
1 SNR B0057-72.2 SNR 00 59 27.40 -72 10 10.7   12.37 12.57     ~ 234 0
2 HD 7113 Em* 01 09 12.94464 -73 11 38.8968     11.7     ~ 120 0
3 LHA 115-N 88A HII 01 24 07.823 -73 09 03.77   13.25 12.18     ~ 72 1
4 NAME Magellanic Clouds GrG 03 00 -71.0           ~ 6634 1
5 NGC 1569 IG 04 30 49.186 +64 50 52.52 11.72 11.86 11.03     ~ 1213 3
6 BRHT 1a Cl* 04 51 51.3 -69 23 26           ~ 42 0
7 NGC 1722 HII 04 51 53.36 -69 23 25.9           ~ 69 0
8 NGC 1714 EmO 04 52 08.4 -66 55 23   11.51 11.61     ~ 82 2
9 LHA 120-N 83B HII 04 54 25.2 -69 11 00           ~ 47 1
10 IRAS 04571-6627 mul 04 57 15.5 -66 23 14           ~ 52 1
11 HD 32340 Em* 04 57 16.253 -66 23 20.94   13.11 12.45 14.00   O3-O6V 77 0
12 NGC 2060 SNR 05 37 51.4466169456 -69 10 23.947092084   9.69 9.59     ~ 347 2
13 [VPT2002] 30 Dor 1 HII 05 38 33.5 -69 06 27           ~ 7 0
14 [GSL2002] 114 HII 05 38 35.4 -69 05 41           ~ 8 0
15 [VPT2002] 30 Dor 3 HII 05 38 46.0 -69 05 08           ~ 8 0
16 [VPT2002] 30 Dor 4 HII 05 38 54.2 -69 05 15           ~ 7 0
17 NGC 2080 HII 05 39 42.6 -69 38 50           ~ 98 1
18 [JHS86] N160A-9 HII 05 39 43.3 -69 38 51           ~ 23 0
19 [GSL2002] 122 HII 05 39 46.1 -69 38 37           ~ 23 0
20 NAME N159 Blob in LMC HII 05 40 04.2 -69 44 43           ~ 38 0
21 NGC 4228 SBG 12 15 39.174 +36 19 36.80 10.63 10.30 9.93 9.74   ~ 932 1

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2023.04.01-00:14:25

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