The anomalous chemical abundances and the structure of the Edgewood-Kuiper belt observed in the solar system constrain the initial mass and radius of the star cluster in which the sun was born to $M\simeq500$ to 3000 \msun and $R\simeq 1$ to 3 pc. When the cluster dissolved the siblings of the sun dispersed through the galaxy, but they remained on a similar orbit around the Galactic center. Today these stars hide among the field stars, but 10 to 60 of them are still present within a distance of $\sim 100$ pc. These siblings of the sun can be identified by accurate measurements of their chemical abundances, positions and their velocities. Finding even a few will strongly constrain the parameters of the parental star cluster and the location in the Galaxy where we were born.
Deep Dive into The lost siblings of the Sun.
The anomalous chemical abundances and the structure of the Edgewood-Kuiper belt observed in the solar system constrain the initial mass and radius of the star cluster in which the sun was born to $M\simeq500$ to 3000 \msun and $R\simeq 1$ to 3 pc. When the cluster dissolved the siblings of the sun dispersed through the galaxy, but they remained on a similar orbit around the Galactic center. Today these stars hide among the field stars, but 10 to 60 of them are still present within a distance of $\sim 100$ pc. These siblings of the sun can be identified by accurate measurements of their chemical abundances, positions and their velocities. Finding even a few will strongly constrain the parameters of the parental star cluster and the location in the Galaxy where we were born.
arXiv:0903.0237v1 [astro-ph.GA] 2 Mar 2009
DRAFT VERSION NOVEMBER 1, 2018
Preprint typeset using LATEX style emulateapj v. 04/03/99
THE LOST SIBLINGS OF THE SUN
SIMON F. PORTEGIES ZWART
Astronomical Institute ‘Anton Pannekoek’, University of Amsterdam, Kruislaan 403, Amsterdam, the Netherlands
Institute for Computer Science, University of Amsterdam, Kruislaan 403, Amsterdam, the Netherlands
Sterrewacht Leiden University of Leiden, Niels Bohrweg 2, 2333 CA Leiden, the Netherlands
Draft version November 1, 2018
ABSTRACT
The anomalous chemical abundances and the structure of the Edgewood-Kuiper belt observed in the solar
system constrain the initial mass and radius of the star cluster in which the sun was born to M ≃500 to 3000 M⊙
and R ≃1 to 3 pc. When the cluster dissolved the siblings of the sun dispersed through the galaxy, but they
remained on a similar orbit around the Galactic center. Today these stars hide among the field stars, but 10 to 60
of them are still present within a distance of ∼100 pc. These siblings of the sun can be identified by accurate
measurements of their chemical abundances, positions and their velocities. Finding even a few will strongly
constrain the parameters of the parental star cluster and the location in the Galaxy where we were born.
1. INTRODUCTION
It is commonly accepted that stars like the sun are born in
clusters (Lada et al., 1993). The cluster in which the sun was
born is long gone and the sun’s siblings are by now spread
over the Galaxy. The structure of the hot Edgeworth-Kuiper
belt objects provide evidence of this, as this population can
be reproduced by a relatively nearby encounter with another
star (Morbidelli & Levison, 2004). Such an encounter is ex-
pected to have occurred in the early history of the Solar system
(Malhotra, 2008). The existence of a well organized planetary
system, however, indicates that the parental cluster cannot have
been very dense as otherwise a nearby passing star would also
have perturbed the orbits of the planets.
Additional evidence for the sun’s dynamic history comes
from the discovery of radioactive isotopes and their decay prod-
ucts in the proto-solar nebula (Hester et al., 2004), which is ex-
plained by a supernova explosion within 1.6 pc of the infant sun
(Looney et al., 2006). The combination of arguments enables
us to estimate the mass and size of the star cluster in which the
sun was born. We follow the orbital evolution of these stars
through the Galaxy for the lifetime of the sun and conclude that
at least 1% (10 to 60) of the sun’s siblings should still be present
within 100 pc, and more than 10% should be within about a
kpc along the orbit of the solar system in the Galactic poten-
tial. With the Gaia satellite (Perryman et al., 2001) and ground-
based searches the radial velocity and distance to the majority
of the lost siblings will be determined, and the proper motion
will be measured. These constrain the orbit of the proto-solar
cluster and enable us to accurately determine the evolution of
the Galactic potential and the birth place of the sun.
2. THE PARENTAL STAR CLUSTER
The sun and its eight planets were born about 4.57 billion
years ago (Bonanno et al., 2002), probably in a star cluster, and
it is in due time that our location in the Galaxy became so deso-
late. Evidence for this dynamic past comes from meteorite fos-
sil records, where the presence of short-lived radioactive iso-
topes in primitive meteorites indicate that the 1.8 Myr young
sun was polluted by a supernova explosion of a star about 15 to
25 times more massive than the sun within a distance of 0.02 to
1.6 parsec (Looney et al., 2006). Such a massive star lives for
6 to 12 Myr before it sheds the majority of its mass in a super-
nova explosion. This massive star must have formed some 4.2
to 10.2 Myr earlier than the sun. Such range in the distribution
of stellar ages is also observed in the Orion Nebula where mas-
sive stars also tend to be a few to ∼10 Myr younger than the
low-mass stars (Palla & Stahler, 1999).
The presence of a massive star close to the infant sun
puts interesting constraints on its birth environment. Today,
such a massive star is not even present within a distance of
100 parsec.
By adopting a standard initial mass function
(Kroupa & Weidner, 2003) about 1 in 400 stars is sufficiently
massive to experience a supernova.
Stars of m = 15 to
25 M⊙are less common and would require a star cluster of
M >∼500 M⊙(Weidner & Kroupa, 2004).
Massive stars in a cluster tend to sink to the center in a frac-
tion ∝1/m of the two-body relaxation time scale (trlx). If
trlx >∼300 Myr even the most massive stars are unlikely to have
reached the cluster center by the time they explode. Massive
stars in clusters with smaller trlx tend to populate the central
region by the time they explode in supernovae, polluting the
nearby young stars and proto planetary disks in the process
(Wielen et al., 1996).
Low mass stars, like the sun, are not
strongly affect
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