2012
DOI: 10.1051/eas/1257003
|View full text |Cite
|
Sign up to set email alerts
|

Formation of Low-Mass Stars and Brown Dwarfs

Abstract: Abstract. These lectures attempt to expose the most important ideas, which have been proposed to explain the formation of stars with particular emphasis on the formation of brown dwarfs and low-mass stars. We first describe the important physical processes which trigger the collapse of a self-gravitating piece of fluid and regulate the star formation rate in molecular clouds. Then we review the various theories which have been proposed along the years to explain the origin of the stellar initial mass function … Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1

Citation Types

0
3
0

Year Published

2013
2013
2022
2022

Publication Types

Select...
2
1
1

Relationship

0
4

Authors

Journals

citations
Cited by 4 publications
(3 citation statements)
references
References 140 publications
(218 reference statements)
0
3
0
Order By: Relevance
“…recently summarised, for example, by Bastian et al (2010), Kroupa et al (2011), andJeffries (2012). In the substellar regime, the characterization of the mass spectrum of a cluster gains another importance, since it could help distinguish among different formation scenarios for brown dwarfs (e.g., Hennebelle 2012). This is the goal of a large programme (P.I.…”
Section: Introductionmentioning
confidence: 99%
“…recently summarised, for example, by Bastian et al (2010), Kroupa et al (2011), andJeffries (2012). In the substellar regime, the characterization of the mass spectrum of a cluster gains another importance, since it could help distinguish among different formation scenarios for brown dwarfs (e.g., Hennebelle 2012). This is the goal of a large programme (P.I.…”
Section: Introductionmentioning
confidence: 99%
“…We have addressed the question of whether the fields threading the gas are swept along by it by estimating the timescale for ambipolar diffusion of the field out of the gas, following Eq. (2.18) of Hennebelle (2012), which shows that the diffusion time varies as n · n i (L/B) 2 where n and n i are the number densities of atoms and of ions, respectively, L is a characteristic length scale and B is the field strength. For our extended and thin flows (L ∼ 1000 AU, n ∼ 0.3×10 3 cm −3 and for characteristic numbers of the ionization fractions in the cold gas and with B set to a few microGauss (Padoan 2018), diffusion timescales are at least one order of magnitude greater than 10 6 years.…”
Section: The Turbulent Casementioning
confidence: 96%
“…Brown dwarfs are substellar objects whose masses are intermediate between the latest M-type stars and the most massive planets (Hayashi & Nakano 1963;Shu 1977;Becklin & Zuckerman 1988;Rebolo et al 1995;Oppenheimer et al 1995;Saumon et al 2006). Similar to stars, brown dwarfs form from interstellar molecular gas cloud core collapse (Uehara & Inutsuka 2000; Bate et al 2002;Krumholz et al 2005;Whitworth & Stamatellos 2006;Chabrier et al 2007; Corresponding author: Joe Zalesky jazalesk@asu.edu Whitworth et al 2007;Hennebelle 2012), but do not achieve masses high enough to sustain core H-fusion over their lifetime (Burrows et al 2001). As the effective temperatures of brown dwarfs are much cooler than those of stars (< 2500K), molecules and condensates form in their photospheres and dominate the spectral energy distribution.…”
Section: Introductionmentioning
confidence: 99%