Table 1
Herschel fluxes, as measured within the five annuli we have considered (see Fig. 9, left-hand panel).
Ap | 100 | 160 | 250 | 350 | 500 | a | b | T D | M D | M HI |
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MH2 | g2d | g2d∗ |
Jy | Jy | Jy | Jy | Jy | kpc | kpc | K | lg(M⊙) | lg(M⊙) | lg(M⊙) | lg(M⊙) | |||
|
||||||||||||||
1 | 220 | 254 | 124 | 50 | 18 | 2.2 | 2.2 |
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7.19 | 7.21 | 6.82 | 66 | 68 |
2 | 732 | 1493 | 1001 | 464 | 181 | 16.4 | 3.6 |
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8.48 | 8.54 | 7.93 | 75 | 83 |
3 | 1307 | 2943 | 2200 | 1110 | 459 | 23.2 | 5.2 |
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9.03 | 9.13 | 8.40 | 92 | 111 |
4 | 813 | 2302 | 2031 | 1143 | 518 | 33.6 | 7.5 |
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9.31 | 9.42 | – | a109 | a140 |
5 | – | 354 | 435 | 278 | 138 | 42.4 | 9.5 |
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8.99 | 9.08 | – | b131 | b158 |
tot | 3055 | 7348 | 5791 | 3047 | 1313 | 42.4 | 9.5 |
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9.65 | 9.74 | 8.42 | 111 | 137 |
Notes. Dust temperature (TD) and masses (MD), and their uncertainties, are derived from SED fitting (see text for details). We also report the mass of hydrogen in the atomic phase, as derived from H i maps of Braun et al. (2009) (both corrected and non-corrected for self-opacity), and the mass of gas in the molecular phase derived by CO data (Nieten et al. 2006). Last two columns give the total gas-to-dust ratios within the given annulus. Results for the largest annulus and for the whole galaxy are limited by the size of the CO map (see text for more details): the value indicated with a assumes a mass of 5% of total, within that annulus, and the value of the gas-to-dust in the outermost annulus (b) was computed assuming a negligible contribution from the molecular fraction, and it is hence to be interpreted as a lower limit. Values in the columns labelled with ∗ are calculated using the self-opacity corrected maps. “a” and “b” are the major and minor axis length, respectively, of the ellipses, given in kpc (first aperture is circular).
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