2010
DOI: 10.1051/0004-6361/200913371
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Looking for high-mass young stellar objects: H$_{\sf 2}$O and OH masers in ammonia cores

Abstract: Context. The earliest stages of high-mass star formation have yet to be characterised well, because high-angular resolution observations are required to infer the properties of the molecular gas hosting the newly formed stars. Aims. We search for high-mass molecular cores in a large sample of 15 high-mass star-forming regions that are observed at highangular resolution, extending a pilot survey based on a smaller number of objects. Methods. The sample was chosen from surveys of H 2 O and OH masers to favour th… Show more

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Cited by 17 publications
(31 citation statements)
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“…The corrected mass is M / sin 2 i. The estimated range of values of M is consistent with the mass of a main-sequence star of spectral type B1 (10.7 M ): i.e., the spectral type estimated for CM2, which is the centimeter continuum source associated with core A, from the 1.3 cm continuum emission assuming that it is optically thin (Codella et al 2010) and following the tables of Davies et al (2011) and Mottram et al (2011). As already mentioned in Sect.…”
Section: Velocity Gradients In Core Asupporting
confidence: 70%
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“…The corrected mass is M / sin 2 i. The estimated range of values of M is consistent with the mass of a main-sequence star of spectral type B1 (10.7 M ): i.e., the spectral type estimated for CM2, which is the centimeter continuum source associated with core A, from the 1.3 cm continuum emission assuming that it is optically thin (Codella et al 2010) and following the tables of Davies et al (2011) and Mottram et al (2011). As already mentioned in Sect.…”
Section: Velocity Gradients In Core Asupporting
confidence: 70%
“…This value is greater than the stellar luminosity of 6.3 × 10 3 L estimated for the centimeter continuum source CM2 that is associated with core A. This stellar luminosity estimate has been obtained from the 1.3 cm emission, assuming that it is optically thin (Codella et al 2010) and following the tables of Davies et al (2011) and Mottram et al (2011), which tabulate the ZAMS stellar parameters (temperature, luminosity, and radius) and the spectral type as a function of mass and Lyman photon flux. These authors used the calculations of Martins et al (2005) However, the SED was computed by integrating the emission over a region of ∼2 , which also includes the emission of the UC Hii region CM1.…”
Section: Spectral Energy Distributionmentioning
confidence: 67%
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