2002ApJ...566..857T


Query : 2002ApJ...566..857T

2002ApJ...566..857T - Astrophys. J., 566, 857-879 (2002/February-3)

A far ultraviolet spectroscopic explorer survey of interstellar molecular hydrogen in the Small and Large Magellanic Clouds.

TUMLINSON J., SHULL J.M., RACHFORD B.L., BROWNING M.K., SNOW T.P., FULLERTON A.W., JENKINS E.B., SAVAGE B.D., CROWTHER P.A., MOOS H.W., SEMBACH K.R., SONNEBORN G. and YORK D.G.

Abstract (from CDS):

We describe a moderate-resolution Far Ultraviolet Spectroscopic Explorer (FUSE) survey of H2 along 70 sight lines to the Small and Large Magellanic Clouds, using hot stars as background sources. FUSE spectra of 67% of observed Magellanic Cloud sources (52% of LMC and 92% of SMC) exhibit absorption lines from the H2 Lyman and Werner bands between 912 and 1120 Å. Our survey is sensitive to N(H2)≥1014 cm–2; the highest column densities are logN(H2)=19.9 in the LMC and 20.6 in the SMC. We find reduced H2 abundances in the Magellanic Clouds relative to the Milky Way, with average molecular fractions fH2=0.010+0.005–0.002 for the SMC and fH2=0.012+0.006–0.003 for the LMC, compared with fH2=0.095 for the Galactic disk over a similar range of reddening. The dominant uncertainty in this measurement results from the systematic differences between 21 cm radio emission and Lyα in pencil beam sight lines as measures of N(H I). These results imply that the diffuse H2 masses of the LMC and SMC are 8x106 and 2x106 M, respectively, 2% and 0.5% of the H I masses derived from 21 cm emission measurements. The LMC and SMC abundance patterns can be reproduced in ensembles of model clouds with a reduced H2 formation rate coefficient, R∼3x10–18 cm3.s–1, and incident radiation fields ranging from 10-100 times the Galactic mean value. We find that these high-radiation, low formation rate models can also explain the enhanced N(4)/N(2) and N(5)/N(3) rotational excitation ratios in the Clouds. We use H2 column densities in low rotational states (J=0 and 1) to derive kinetic and/or rotational temperatures of diffuse interstellar gas, and we find that the distribution of rotational temperatures is similar to Galactic gas, with <T01≥82±21 K for clouds with N(H2)≥1016.5 cm–2. There is only a weak correlation between detected H2 and far-infrared fluxes as determined by IRAS, perhaps as a result of differences in the survey techniques. We find that the surface density of H2 probed by our pencil beam sight lines is far lower than that predicted from the surface brightness of dust in IRAS maps. We discuss the implications of this work for theories of star formation in low-metallicity environments.

Abstract Copyright:

Journal keyword(s): ISM: Clouds - ISM: Molecules - Galaxies: Magellanic Clouds - Ultraviolet: ISM

Simbad objects: 71

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Number of rows : 71
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 LIN 78 HXB 00 46 32.6338987968 -73 06 05.564426436 12.53 13.59 13.827   13.999 O3/4V 45 1
2 SK 10 s*b 00 46 42.1591125672 -73 24 55.494317340 11.903 12.984 13.176   13.35 O6.5I(f) 45 0
3 BBB SMC 266 s*b 00 47 50.0484011088 -73 08 21.054056928   12.35 12.55 12.36   O6I(f) 69 0
4 AzV 47 * 00 48 51.4911440520 -73 25 58.537753356 12.263 13.314 13.496   14.00 O8III 35 0
5 BBB SMC 1 * 00 50 17.2067283312 -72 53 30.259838832 12.093 13.144 13.326 13.39 13.47 OC7.5III((f)) 43 0
6 LIN 156 s*b 00 50 32.4050818488 -72 52 36.441355908 11.553 12.604 12.756   12.89 O5.5I(f) 50 0
7 AzV 83 s*b 00 50 52.0015192368 -72 42 14.940550980 12.233 13.244 13.366   13.67 O7Iaf+ 47 0
8 AzV 95 * 00 51 21.6002057448 -72 44 14.875230300 12.67 13.64 13.83   13.95 O7III((f)) 40 0
9 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 11149 1
10 AzV 207 * 00 58 33.1896798552 -71 55 46.721984016 12.99 14.13 14.35   14.58 O7Vz((f)) 36 0
11 Cl* NGC 346 ELS 7 * 00 58 57.3961905528 -72 10 33.660822720 12.68 13.82 14.13   14.28 O4V((f+)) 52 0
12 Cl* NGC 346 W 4 EB* 00 59 00.0525662904 -72 10 37.962442344 11.82 12.93 13.13   13.77 O5-6V((f)) 37 0
13 Cl* NGC 346 W 3 * 00 59 00.7591806336 -72 10 28.171806492 11.46 12.61 12.80   13.63 O2III(f) 62 0
14 SK 80 s*b 00 59 31.9751731656 -72 10 46.106730444   12.12 12.31     O7Iaf+ 108 0
15 RMC 17 s*b 00 59 45.7300850520 -72 44 56.416111080   12.02 12.2     B1Ia 63 0
16 AzV 238 ** 00 59 55.5078343032 -72 13 37.781342400   13.55 13.77     O9III 33 0
17 RMC 18 s*b 01 00 06.8830919184 -72 13 57.371461032   11.7 11.5     B1Ia 66 0
18 SK 94 s*b 01 01 07.7622056304 -71 59 58.783358472   12.21 12.36 12.20   B1.5-2Iab 32 0
19 AzV 321 * 01 02 57.0821742960 -72 08 09.112126884 12.49 13.66 13.82   14.10 O9.5Ib 27 0
20 RMC 28 s*b 01 03 10.5480205584 -72 02 14.335031256 11.833 12.924 13.086   13.60 O9.7I 41 0
21 RMC 31 WR* 01 03 25.2272050176 -72 06 43.857668340   12.11 12.30     WN3:h+O5.5V+O5.5If+O7.5V 114 0
22 SK 116 s*b 01 04 55.7398901040 -72 46 48.146591280 11.413 12.494 12.646     O9Iabw 35 0
23 AzV 378 * 01 05 09.4353086232 -72 05 34.656190260 12.60 13.64 13.90   14.18 O9.5III 23 0
24 AzV 388 * 01 05 39.5306276568 -72 29 26.938329540 12.79 13.86 14.12   14.37 O5V 42 0
25 SK 159 s*b 01 15 58.8782034384 -73 21 24.351532740 10.80 11.77 11.90     B0Ia 73 0
26 LIN 547 WR* 01 31 04.1367366432 -73 25 03.784411524   12.75 12.90     WO4+O4V 96 0
27 HD 268605 s*b 04 50 18.9258130824 -67 39 38.036838240 10.244 11.2 11.377   11.322 O9.5/B0Ia 86 0
28 HD 268685 s*b 04 54 31.8862673064 -67 15 24.584925456 10.616 11.376 11.541   11.599 B1.5Ia 43 0
29 HD 32109 WR* 04 55 31.3415815464 -67 30 02.683346940 12.893 13.46 13.81 13.95 13.512 WN4b 74 0
30 SK -65 21 s*b 05 01 22.2741446472 -65 41 47.884690176 11.119 12.08 12.70   12.373 O9.7Iab 40 0
31 HD 270952 WR* 05 01 23.0763876936 -65 52 33.206008764 10.944 11.871 12.07   12.187 O6Iaf+ 54 0
32 HD 33133 WR* 05 03 08.9126630616 -66 40 57.492259824   12.46 12.63 12.85   WN7h 93 0
33 HD 268960 V* 05 03 12.6982527768 -69 01 37.040851884 11.218 12.01 12.166   12.443 O(f)+B1I? 19 0
34 SK -70 60 * 05 04 40.7778022320 -70 15 34.497999576 12.609 13.646 13.914   13.967 O4V 24 0
35 SK -70 69 * 05 05 18.6717716496 -70 25 49.874974104 12.586 13.616 13.854   14.074 O3V(f) 39 0
36 SK -68 41 * 05 05 27.1146438696 -68 10 02.642123460 10.855 11.868 12.01   12.086 B0.5Ia 51 0
37 HD 269050 s*b 05 07 20.4218668824 -68 32 08.569322196 10.593 11.581 11.54 11.46 11.55 B0Ia(e?) 70 0
38 SK -67 69 * 05 14 20.0729621208 -67 08 03.171550632 11.950 13.012 13.040   13.330 O3III 25 0
39 HD 269357 * 05 18 59.4790204920 -69 12 54.801550908   11.89 12.10     O6Ib(f) 55 0
40 SK -67 76 * 05 20 05.7171800112 -67 21 10.618641612 11.575 12.542 12.42   12.845 B0Ia 20 0
41 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 17434 0
42 SK -69 124 * 05 25 18.2515805760 -69 03 11.489785740 11.583 12.664 12.826   12.791 OB 24 0
43 SK -67 101 * 05 25 56.2422042240 -67 30 28.813234608   12.46 12.63     O8II((f)) 33 1
44 HD 36402 WR* 05 26 03.9637892880 -67 29 57.087864096   11.25 11.621 11.65   (WC) 138 0
45 HD 36521 WR* 05 26 30.2591541144 -68 50 27.500574192   12.156 12.317 12.529   WC4+O6III/V+O 84 0
46 BI 170 * 05 26 47.6917783584 -69 06 12.016345140 11.823 12.914 13.116   12.975 O9.5Ib 25 0
47 SK -67 111 s*b 05 26 48.0782169672 -67 29 29.782796892   12.33 12.42     O6Iaf(n)pv 46 0
48 BI 173 * 05 27 09.9440507208 -69 07 56.452079568 11.85 12.86 13.00     O8III 26 0
49 SK -70 91 ** 05 27 33.5728977024 -70 36 47.950130916 11.369 12.55 12.78   12.937 O2III(f*)+OB 27 0
50 SK -66 100 * 05 27 45.4472444328 -66 55 15.293259480 12.227 12.976 13.204   13.501 O6II(f) 44 0
51 HD 269582 WR* 05 27 52.6621673400 -68 59 08.488879836 12.206 10.818 11.093 12.70 11.234 WN10h 108 0
52 HD 37026 WR* 05 30 12.1637529576 -67 26 08.329055928 12.853 13.16 13.53 13.56 13.856 WC 76 0
53 HD 269676 ** 05 31 15.634248 -71 04 09.90516 11.134 11.417 11.547 12.061 12.191 O6+O9: 82 0
54 HD 269687 WR* 05 31 25.5247745448 -69 05 38.556251700 10.86 11.78 11.87 12.05   WN11h 110 0
55 HD 269698 s*b 05 31 44.2080798984 -67 38 01.374839556 9.520 12.00 12.22 12.47 11.167 O4Ia 111 0
56 SK -67 169 * 05 31 51.5898307488 -67 02 22.242829128   12.06 12.18     B1Ia 29 0
57 SK -67 167 s*b 05 31 51.9123196824 -67 39 41.372080308 11.243 12.364 12.586   11.819 O4If+n 40 0
58 SK -67 191 * 05 33 34.0158776232 -67 30 19.741489992 12.153 13.214 13.436   14.838 O8V 28 0
59 BI 208 * 05 33 57.3355514112 -67 24 20.179711404 12.742 13.716 13.921   14.141 O7V 18 0
60 HD 37680 WR* 05 34 19.2493989720 -69 45 10.295445528 12.807 12.98 13.25 13.21 13.490 WC 74 1
61 HD 269810 Em* 05 35 13.8977747136 -67 33 27.542449260   12.08 12.22 12.53   O3III(f*) 106 0
62 BI 229 Pu* 05 35 32.1627904200 -66 02 37.668974208 12.290 12.705 12.894 13.206 12.881 O7III 20 0
63 SK -66 169 s*b 05 36 54.6614083464 -66 38 22.427577744   12.43 12.56     O9.7Ia+ 33 0
64 SK -66 172 * 05 37 05.3893162560 -66 21 34.989059484   13.01 13.1     OB 41 0
65 HD 269896 s*b 05 37 49.1356176384 -68 55 01.639049016 11.338 9.493 11.449 11.49   ON9.7Ia+ 86 0
66 Brey 77 WR* 05 38 42.1044150840 -69 05 55.335965424     12.86   12.79 O2If* 79 0
67 RMC 136 Cl* 05 38 42.396 -69 06 03.36   5.81 5.40     ~ 2019 2
68 HD 38282 WR* 05 38 53.3783458680 -69 02 00.895545204   10.98 11.11 11.26   WN5/6h+WN6/7h 170 1
69 HD 269927 ** 05 38 58.856976 -69 29 22.47504     10.68 11.23   B0I+O7If 27 0
70 BI 272 * 05 44 23.1088099248 -67 14 29.211340416 12.163 13.127 13.201   13.524 O7III 23 0
71 HD 270145 s*b 05 48 49.6513961040 -70 03 57.837376476 10.903 12.110 12.166     O6.5Iaf 48 1

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