期刊
MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY
卷 478, 期 3, 页码 4142-4161出版社
OXFORD UNIV PRESS
DOI: 10.1093/mnras/sty1217
关键词
hydrodynamics; radiative transfer; methods: numerical; stars: formation; ISM: kinematics and dynamics; galaxies: star formation
资金
- NSF [AST-1413501]
- National Science Foundation [NSF PHY-1125915]
The physics of star formation at its extreme, in the nuclei of the densest and the most massive star clusters in the universe - potential massive black hole nurseries - has for decades eluded scrutiny. Spectroscopy of these systems has been scarce, whereas theoretical arguments suggest that radiation pressure on dust grains somehow inhibits star formation. Here, we harness an accelerated Monte Carlo radiation transport scheme to report a radiation hydrodynamical simulation of super star cluster formation in turbulent clouds. We find that radiation pressure reduces the global star formation efficiency by 30-35 per cent, and the star formation rate by 15-50 per cent, both relative to a radiation-free control run. Overall, radiation pressure does not terminate the gas supply for star formation and the final stellar mass of the most massive cluster is similar to 1.3 x 10(6) M-circle dot. The limited impact as compared to idealized theoretical models is attributed to a radiation-matter anticorrelation in the supersonically turbulent, gravitationally collapsing medium. In isolated regions outside massive clusters, where the gas distribution is less disturbed, radiation pressure is more effective in limiting star formation. The resulting stellar density at the cluster core is not greater than or equal to 10(8) M-circle dot pc(-3), with stellar velocity dispersion greater than or similar to 70 km s(-1). We conclude that the super star cluster nucleus is propitious to the formation of very massive stars via dynamical core collapse and stellar merging. We speculate that the very massive star may avoid the claimed catastrophic mass loss by continuing to accrete dense gas condensing from a gravitationally confined ionized phase.
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