Clumps and triggered star formation in ionized molecular clouds
Infrared shells and bubbles are ubiquitous in the Galaxy and can generally be associated with H ii regions formed around young, massive stars. In this paper, we use high-resolution 3D SPH simulations to explore the effect of a single O7 star emitting photons at 1049 s−1 and located at the centre of...
Saved in:
Published in: | Monthly notices of the Royal Astronomical Society Vol. 435; no. 2; pp. 917 - 927 |
---|---|
Main Authors: | , , , , |
Format: | Journal Article |
Language: | English |
Published: |
London
Oxford University Press
21-10-2013
|
Subjects: | |
Online Access: | Get full text |
Tags: |
Add Tag
No Tags, Be the first to tag this record!
|
Summary: | Infrared shells and bubbles are ubiquitous in the Galaxy and can generally be associated with H ii regions formed around young, massive stars. In this paper, we use high-resolution 3D SPH simulations to explore the effect of a single O7 star emitting photons at 1049 s−1 and located at the centre of a molecular cloud with mass 104 M and radius 6.4 pc; the internal structure of the cloud is characterized by its fractal dimension,
(with
), and the variance of its (lognormal) density distribution,
(with
). Our study focuses on the morphology of the swept-up cold gas and the distribution and statistics of the resulting star formation. If the fractal dimension is low, the border of the H ii region is dominated by extended shell-like structures, and these break up into a small number of massive high-density clumps which then spawn star clusters; star formation occurs relatively quickly, and delivers somewhat higher stellar masses. Conversely, if the fractal dimension is high, the border of the H ii region is dominated by a large number of pillars and cometary globules, which contain compact dense clumps and tend to spawn single stars or individual multiple systems; star formation occurs later, the stellar masses are somewhat lower, and the stars are more widely distributed. |
---|---|
ISSN: | 0035-8711 1365-2966 |
DOI: | 10.1093/mnras/stt1115 |