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The formation of massive stars: accretion, disks and the development of hypercompact HII regions

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arxiv astro-ph/0603856 v3 pith:MFUQAUAS submitted 2006-03-31 astro-ph

classification astro-ph
keywords accretionregionflowionizationmassivestarregionsstars
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The hypothesis that massive stars form by accretion can be investigated by simple analytical calculations that describe the effect that the formation of a massive star has on its own accretion flow. Within a simple accretion model that includes angular momentum, that of gas flow on ballistic trajectories around a star, the increasing ionization of a massive star growing by accretion produces a three-stage evolutionary sequence. The ionization first forms a small quasi-spherical HII region gravitationally trapped within the accretion flow. At this stage the flow of ionized gas is entirely inward. As the ionization increases, the HII region transitions to a bipolar morphology in which the inflow is replaced by outflow within a narrow range of angle with about the bipolar axis. At higher rates of ionization, the opening angle of the outflow region progressively increases. Eventually, in the third stage, the accretion is confined to a thin region about an equatorial disk. Throughout this early evolution, the HII region is of hypercompact to ultracompact size depending on the mass of the enclosed star or stars. These small HII regions whose dynamics are dominated by stellar gravitation and accretion are different than compact and larger HII regions whose dynamics are dominated by the thermal pressure of the ionized gas.

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Cited by 2 Pith papers

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  1. The Zero-Age Massive Stellar Population of W49A from VLA Observations

    astro-ph.GA 2026-08 conditional novelty 6.0 of 10

    The high-mass stellar population of W49A, traced by 101 H II regions, shows a steep mass function slope (Gamma > 2.5) compared to the standard Salpeter slope of 1.35, implying a deficit of the most massive stars.

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    Simplified virial analyses of W43-MM1 cores overestimate non-thermal support because linewidths include organized motions of 1–3 km/s and surface terms are omitted, producing unexpectedly high stability fractions.

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