2012ApJ...760...99P


Query : 2012ApJ...760...99P

2012ApJ...760...99P - Astrophys. J., 760, 99 (2012/December-1)

The triple evolution dynamical instability: stellar collisions in the field and the formation of exotic binaries.

PERETS H.B. and KRATTER K.M.

Abstract (from CDS):

Physical collisions and close approaches between stars play an important role in the formation of exotic stellar systems. Standard theories suggest that collisions are rare, occurring only via random encounters between stars in dense clusters. We present a different formation pathway, the triple evolution dynamical instability (TEDI), in which mass loss in an evolving triple star system causes orbital instability. The subsequent chaotic orbital evolution of the stars triggers close encounters, collisions, exchanges between the stellar components, and the dynamical formation of eccentric compact binaries (including Sirius-like binaries). We demonstrate that the rate of stellar collisions due to the TEDI is approximately 10–4/yr per Milky Way Galaxy, which is nearly 30 times higher than the total collision rate due to random encounters in the Galactic globular clusters. Moreover, we find that the dominant type of stellar collision is qualitatively different; most collisions involve asymptotic giant branch stars, rather than main sequence or slightly evolved stars, which dominate collisions in globular clusters. The TEDI mechanism should lead us to revise our understanding of collisions and the formation of compact, eccentric binaries in the field.

Abstract Copyright: ∼

Journal keyword(s): binaries: close - binaries: general - instabilities - stars: AGB and post-AGB - stars: evolution - stars: kinematics and dynamics - stars: mass-loss - white dwarfs

Simbad objects: 3

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Number of rows : 3
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 * alf CMa SB* 06 45 08.91728 -16 42 58.0171 -1.51 -1.46 -1.46 -1.46 -1.43 A0mA1Va 1610 0
2 PSR J1903+0327 Psr 19 03 05.7937 +03 27 19.222           ~ 187 1
3 M 15 GlC 21 29 58.33 +12 10 01.2           ~ 3274 0

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