4.7 Article

Structure and evolution of the envelopes of deeply embedded massive young stars

Journal

ASTROPHYSICAL JOURNAL
Volume 537, Issue 1, Pages 283-303

Publisher

IOP PUBLISHING LTD
DOI: 10.1086/309011

Keywords

circumstellar matter; dust, extinction; ISM : jets and outflows; ISM : molecules; stars : formation; submillimeter

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The physical structure of the envelopes around a sample of 14 massive young stars is investigated using maps and spectra in submillimeter continuum and lines of (CO)-O-17, CS, (CS)-S-34, and H2CO. Nine of the sources are highly embedded luminous (10(3)-10(5) L.) young stellar objects that are bright near-infrared sources but weak in radio continuum; the other objects are similar but not bright in the near-infrared and contain hot-core-type objects and/or ultracompact H II regions. The data are used to constrain the temperature and density structure of the circumstellar envelopes on 10(2)-10(5) AU scales, to investigate the relation between the different objects, and to search for evolutionary effects. The total column densities and the temperature profiles are obtained by fitting self-consistent dust models to submillimeter photometry. The calculated temperatures range from 300 to 1000 K at similar to 10(2) AU and from 10 to 30 K at similar to 10(5) AU from the star. Visual extinctions are a few hundred to a few thousand magnitudes, assuming a grain opacity at 1300 mu m of approximate to 1 cm(-2) g(-1) of dust, as derived earlier for one of our sources. The mid-infrared data are consistent with a 30% decrease of the opacity at higher temperatures, caused by the evaporation of the ice mantles. The CS, (CS)-S-34, and H2CO data as well as the submillimeter dust emission maps indicate density gradients n proportional to r(-a). Assuming a constant CS abundance throughout the envelope, values of alpha = 1.0-1.5 are found, which is significantly flatter than the alpha = 2.0 +/- 0.3 generally found for low-mass objects. This flattening may indicate that in massive young stellar objects, nonthermal pressure is more important for the support against gravitational collapse, while thermal pressure dominates for low-mass sources. We find alpha = 2 for two hot-core-type sources but regard this as an upper limit since, in these objects, the CS abundance may be enhanced in the warm gas close to the star. The assumption of spherical symmetry is tested by modeling infrared absorption line data of (CO)-C-13, CS emission-line profiles and near-infrared continuum. There is a distinct, but small deviation from spherical symmetry: the data are consistent with a decrease of the optical depth by a factor of approximate to 3 in the central less than or similar to 10. The homogeneity of the envelopes is verified by the good agreement of the total masses in the power-law models with the virial masses. Modeling of (CO)-O-17 emission shows that approximate to 40%-90% of the CO is frozen out onto the dust. The CO abundances show a clear correlation with temperature, as expected if the abundance is controlled by freeze-out and thermal desorption. The CS abundance is 3 x 10(-9) on average, ranging from (4-8) x 10(-10) in the cold source GL 7009S to (1-2) x 10(-8) in the two hot-core-type sources. Dense outflowing gas is seen in the CS and H2CO line wings; the predominance of blueshifted emission suggests the presence of dense, optically thick material within 10 of the center. Interferometric continuum observations at 1300-3500 mu m show compact emission, probably from a 0.3 diameter, optically thick dust component, such as a dense shell or a disk. The emission is a factor of 10-100 stronger than expected for the envelopes seen in the single-dish data, so that this component may be opaque enough to explain the asymmetric CS and H2CO line profiles. The evolution of the sources is traced by the overall temperature (measured by the far-infrared color), which increases systematically with the decreasing ratio of envelope mass to stellar mass. The observed anticorrelation of near-infrared and radio continuum emission suggests that the erosion of the envelope proceeds from the inside out. Conventional tracers of the evolution of low-mass objects do not change much over this narrow age range.

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