Figure 9. Sailboats in the
harbor of Nice, a seaside city at the epicenter of theoretical research
into the evolution of the Solar System.
into the evolution of the Solar System.
the grand tack
For a long time, the circular, evenly-spaced orbits of the
Solar System were interpreted as relics of a placid evolutionary history. Each
planet seemed to have assembled very near its present orbit and maintained long-term
dynamical harmony with its neighbors. In addition, the distribution of mass
among the eight planets seemed to support a scenario of orderly growth: the
smallest, Mercury, travels on the shortest orbit, where planetesimals were
least abundant in the primordial nebula; the largest, Jupiter, occupies the
nebula’s sweet spot, where solids were plentiful and growth was fastest; the
next planet outward, Saturn, is only one-third as massive as Jupiter; and the combined
mass of the two outer planets, Uranus and Neptune, is only one-third of
Saturn’s.
This simple scenario, as it turns out, has fatal flaws.
- Our system’s mass distribution exhibits two striking discontinuities. Considering its position in the planetary line-up, Mars should be a few times the mass of Earth, yet it is only one-ninth as massive (Figure 12); while Neptune, the outermost planet, should be less massive than Uranus, its inner neighbor, yet it is almost 20% heavier.
- The skewed configurations of several planetary orbits testify to violent histories. Although Venus and Neptune have orbital eccentricities smaller than 1%, and Earth is under 2%, three adjacent giant planets – Jupiter, Saturn, and Uranus – have eccentricities in the vicinity of 5%, while Mars has 9% and Mercury has more than 20%.
- Both Jupiter and Neptune share their orbits with large populations of so-called Trojan asteroids, which occupy the stable Lagrange points located 60 degrees ahead of and behind each planet. A relatively static model of system evolution cannot explain these accumulations of small bodies.
- The axis of rotation of Uranus is tilted more than 90 degrees to the plane of the Sun’s equator (Between Earth & Uranus, Part I), a configuration that is often explained as resulting from a collision between Uranus and an otherwise unknown rogue planet in the Solar System’s infancy (Slattery et al. 1992, Parisi et al. 2008).
Taken together, these discontinuities, eccentricities, and
irregularities offer incontrovertible proof of a complex evolutionary process.
The Nice model (Figure 9), which has become the most widely
endorsed scenario of Solar System evolution, took as its starting point the
moment when the Solar nebula had completely evaporated (Gomes et al. 2005, Tsiganis et al. 2005). At that time the four
(or five) massive outer planets were assumed to be collected in a much more
compact configuration than they are today, orbiting inside a semimajor axis of
15 AU.
However, the original Nice model could not explain how our
giants happened to arrive in such a snug relationship. Over the past few years
this gap in our understanding has been filled by a series of studies outlining
a remarkable sequence of events known as the Grand Tack (Morbidelli et al. 2007, Batygin & Brown 2010, Morbidelli et al.
2011, Pierens & Raymond 2011, Walsh et al. 2011). The “tack” in this
nickname has nothing to do with sharp pointy objects. Instead, it refers to a
sailing maneuver (Figure 10) in which a ship sails against the wind by
zigzagging back and forth (tacking) across her forward path, thereby changing
the direction from which the wind hits her sails at the turning point of each
zigzag (tack).
Figure 10. 2011 Extreme Sailing
Series, Nice, Côte d’Azur
In the Grand Tack model, the rapid accretion of solids in
the inner system during the first few million years after the Sun ignited was paralleled
by an even more rapid accumulation of rocky and icy particles beyond 3 AU. The
problem of narrow feeding zones, which made most inner-system embryos stall
somewhere between the masses of the Moon and Mars, did not pose a barrier to
growth in this outer region. Two large protoplanets assembled between 3 and 5
AU, with the inner object quickly reaching the phase of runaway growth, during
which it accreted a deep hydrogen atmosphere. This object was proto-Jupiter,
the first gas giant to emerge from the Sun’s protoplanetary cloud.
Having opened a gap in the dissipating nebula, proto-Jupiter
began to spiral toward the Sun, carried along with the flow of accreting gases in
a process known as Type II migration.
The proto-giant plowed through broad fields of planetesimals orbiting inward of
3 AU, pitching them into the Sun, scattering them on eccentric orbits, or
ejecting them from the system altogether.
Right behind proto-Jupiter came the second proto-giant, the
ancestor of Saturn, which initiated runaway accretion not long after its bigger
sibling and began to spiral inward even faster. When proto-Jupiter reached a
semimajor axis of 1.5 AU (equivalent to the current orbit of Mars) the two
objects entered into a mean motion resonance
(MMR), such that their orbital periods could be expressed as the
ratio of two small integers. Large suites of numerical simulations have
specified the likely resonance as 3:2, such that proto-Jupiter completed three
orbits for every two of proto-Saturn (Morbidelli
et al. 2007, Batygin & Brown 2010, Pierens & Raymond 2011). The
2:1 and 5:3 resonances have also been shown to result in similar outcomes, at
least in some iterations of the model (Batygin
& Brown 2010).
Figure 11. The
Grand Tack. Migration of the four giant planets through the Solar nebula
over a period of 600,000 years. Distance is marked in astronomical units (AU). The narrow belt of planetesimals at 1 AU (the present orbit of Earth) later coalesced into the four terrestrial planets.
The establishment of this orbital resonance was in effect a
“marriage” between the two proto-giants, such that their dynamical trajectories
thereafter became inextricably linked. Their inward migration now halted and abruptly
reversed. This striking reversal is the Grand Tack itself, which brought both
giants back into the outer system, maintaining their resonant configuration the
whole time (Figure 11). Jupiter’s tacking maneuver permitted a considerably
diminished belt of planetesimals and planetary embryos to reassemble around 1
AU, the current orbit of the Earth. Meanwhile, the outward passage of Saturn
brought the inner of the newly-formed gas dwarfs under its gravitational
influence, such that Saturn captured the young dwarf (either Uranus or Neptune)
in another MMR (Morbidelli et al. 2007, Batygin
& Brown 2010). This gas dwarf, in turn, captured the next dwarf out.
In one promising model developed by Morbidelli and
colleagues (2007), Neptune (identified as the outer gas dwarf) participated in
a 3:4 MMR with Uranus, Uranus participated in a 2:3 MMR with Saturn, and Saturn
participated in another 2:3 MMR with Jupiter. In this model, the ratio of the
four orbital periods, from Neptune to Jupiter, is 3:4:6:9.
Having attained their mature masses, Jupiter and Saturn
paused in their flight from the Sun. A likely explanation for their journey’s
end is the attenuation of the Solar nebula, to the point where it could no longer
sustain gas-driven migration: as if an ebbing flood had stranded these two
giants in its wake. Jupiter landed near its present semimajor axis of 5.2 AU,
Saturn achieved an orbit near 7 AU, while the brood of gas dwarfs – Neptune,
Uranus, and perhaps “Amphitrite” – were confined to a region between 9 and 15
AU. Beyond these cold orbits stretched the solid remnants of the protoplanetary
disk: a field of rocky and icy objects extending to a radius of about 30 AU or
so. This population would eventually contribute to the Kuiper Belt.
Intuitively, the titanic sequence of events involved in the
Grand Tack might seem to require many aeons to reach its climax. As a point of
reference, the Mesozoic Era on Earth lasted 180 million years, during which the
supercontinent Pangaea broke up and the dinosaurs evolved, flourished, and died
out. Yet the span of time required for the Grant Tack was actually shorter by a
few orders of magnitude. According to recent simulations, only 600,000 years
elapsed from the accretion of Jupiter’s atmosphere, through the migration of both
gas giants across the Solar nebula, to the establishment of the four-way
orbital resonance that provisionally stabilized the outer system (Walsh et al. 2011). Thereafter, according to
this model, the four giant planets ran like clockwork for hundreds of millions
of years in precisely matched revolutions around the Sun.
Although the duration of the Grand Tack can be estimated, uncertainty
surrounds both its absolute chronology (in terms of time since the Sun’s
ignition) and its relative chronology (in terms of its temporal relationship
with other key system events). For example, Vesta formed about 2 or 3 million
years after the Sun, but did its birth occur before, during, or after Jupiter’s
migration? The same questions can be asked of Mars, whose accretion was
complete about 10 million years after the condensation of the Solar nebula.
Two synchronisms seem clear: the Grand Tack finished when the
nebula dispersed, and the process of dispersal coincided with the formation of
the regular satellites of Jupiter and Saturn in “gas-starved” accretion disks
around their parent planets (Canup & Ward
2006). Given what we know about the lifetimes of gas disks, these
outcomes transpired no earlier than 3 million years and probably not much later
than 6 million years after the Sun’s first light.
Figure 12. Runts
of the Litter. Mercury & Mars are dramatically smaller
and less massive than their cloudy siblings, Venus & Earth.
and less massive than their cloudy siblings, Venus & Earth.
worlds in collision
The evaporation of the gas nebula ended the tumultuous first
act of our Solar System’s origin story. Jupiter’s brief incursion to a
perihelion of 1.5 AU had devastated the inner system. All that remained of the
earlier population of planetesimals and embryos was a narrow ring of rocky and
icy objects orbiting around 1.0 AU, near the present orbits of Venus and Earth.
Much of the second act of the drama focuses on events in this inner region,
although its finale involves the whole system.
The notion that the four terrestrial planets (Mercury
through Mars) originated in a narrow annulus between 0.7 and 1 AU (Hansen 2009), instead of in a much broader
field of planetesimals extending from ~0.5 AU to ~3.5 AU, is perfectly
congruent with the scenario of the Grand Tack (Brasser
2012, Morbidelli et al. 2012). Yet it was originally advanced by Brad
Hansen on the basis of numerical simulations whose sole purpose was to
reproduce the current architecture of the inner Solar System (Hansen 2009). In fact, Hansen conceded that, although
his model nicely explained the masses, orbits, and formation timescales of the
four inner planets, it could not account for the origin of their depleted birth
environment or for existence of the current Asteroid Belt.
Serendipitously, the Grand Tack fills both gaps. We have
already seen that it explains the annulus as a leftover from Jupiter’s
marauding days. The Asteroid Belt then becomes a by-blow of the accretion of
the terrestrial planets, a junkyard that collected all the debris ejected from
the inner system by gravitational scattering and collisions between planetary
embryos.
After Jupiter withdrew from the inner system, the remaining
mass of planetesimals accreted into a population of planetary embryos that
underwent violent impacts. This process assembled Mars within about 10 million
years after the birth of the Sun, and simultaneously ejected the young planet from
the main annulus onto a wider and somewhat eccentric orbit (Hansen 2009). Mercury was probably produced on
a similar timescale and ejected onto an even more eccentric orbit closer to the
Sun, although its formation has not yet been explored in detail. Both of these
planets are considerably smaller and less massive than Earth and Venus (Figure
12): Mars has only 0.11 of Earth’s mass (Mea), while Mercury has only 0.06 Mea.
Their stunted growth is readily explained by their early expulsion from the “birth
ring.” At 0.81 Mea, Venus required the equivalent of five Mercuries and five Marses
to attain her current bulk, while Earth needed approximately six of each.
All scenarios agree that Earth is the youngest of the
terrestrial planets, and thus the youngest planet in the whole system. According
to the most widely accepted models, its formation was not complete until it
suffered a glancing collision with a Mars-sized object late in its accretion
history. The resulting debris endowed the Earth with its final mass and
contributed to a circumplanetary ring from which the Moon rapidly assembled (Canup 2004). Although debate continues over
the timing of this Moon-forming event, a date between 30 and 50 million years
after the condensation of the Solar nebula has broad support (Canup 2004, Jacobsen 2005, Jacobsen et al. 2009,
Hansen 2009).
A remaining problem in inner system evolution is the origin
of the Earth’s oceans, sometimes discussed under the heading of “water delivery.” Numerous
studies have argued that proto-Earth was dry, since its birth environment
inside the ice line was too hot to sustain freely orbiting volatiles. Water
must have arrived from cooler regions of the system, with the Asteroid Belt
favored over the Kuiper Belt as its source on the basis of hydrogen isotopes in
Earth’s current oceans (Morbidelli et al. 2000).
However, the delivery of just the right amount of water at just the right time may
have required an implausible degree of fine-tuning.
Not to worry, because along with so much else, the Grand
Tack can also explain the origin of our biogenic oceans (Brasser 2012, Morbidelli et al. 2012). Jupiter’s early migration
through the inner system scattered plenty of wet planetesimals from beyond the
ice line into the terrestrial birth ring, making them available for accretion
by all four protoplanets. In the end, Earth was the only one with the right
stuff – mass, temperature, magnetic field, atmosphere – to retain its precious
inheritance. The match between the isotopic content of our oceans and that of carbonaceous
chondritic meteorites is then explained, not by a bombardment of such objects
after Earth formed, but by their presence among the building blocks that originally
assembled it.
Figure 13.
Late Heavy Bombardment. a. At the end of the Grand Tack, two gas giants
and two ice giants orbited inside 15 AU (Jupiter = green, Saturn = orange,
Neptune = blue, Uranus = turquoise).
b. All four giants suffer orbital instabilities, and Neptune and Uranus switch orbits, scattering asteroids and comets throughout the Solar System. c. The four giants achieve their final orbits amid a dramatically depleted field of leftover planetesimals. Credit: Wikimedia
b. All four giants suffer orbital instabilities, and Neptune and Uranus switch orbits, scattering asteroids and comets throughout the Solar System. c. The four giants achieve their final orbits amid a dramatically depleted field of leftover planetesimals. Credit: Wikimedia
late heavy bombardment
After the Moon-forming event, the inner Solar System settled
into a long period of relative stability. For several hundred million years,
asteroid and comet strikes happened intermittently, while the four (or more) outer
giants revolved in their clockwork orbits. Trouble was brewing, nevertheless.
The presence of a large, encircling field of planetesimals – ancestor of the
present-day Kuiper Belt – resulted in a steady enlargement of the orbits of the
gas dwarfs (Uranus, Neptune, and maybe “Amphitrite”) located beyond Saturn.
Eventually, interactions between Saturn and the next planet out resulted in a
scattering event that disrupted the outer system
(Morbidelli et al. 2007, 2009a). As Morbidelli and colleagues describe
it:
The migration of the giant planets,
induced by the interaction with this [planetesimal] disk, increases the ratios
of the orbital periods between each pair of planets. Thus, the planets are
extracted from their mutual quadruple resonance. Because the system is very
compact, new resonances are crossed during the migration. These resonances
excite the eccentricities of the planets, triggering a global instability of
the system. The orbits of the planets are eventually stabilized by the
dynamical friction exerted by the planetesimal disk during its dispersal. (Morbidelli et al. 2007)
During this violent epoch, Uranus and Neptune may have
switched orbits, and “Amphitrite” may have collided with Uranus, producing the
extreme axial tilt we observe today. Thereafter, any extra gas dwarfs must have
been ejected from the system, since we have only two left.
Regardless of the details, Neptune migrated steadily outward
across a distance of 15 AU, to its present semimajor axis of 30 AU. In the
process, it scattered planetesimals far and wide and dramatically reduced the
overall mass of the Kuiper Belt. The storm of eccentric comets and asteroids launched
by Neptune is the Late Heavy Bombardment, whose scars are still visible as
craters on the surfaces of the Moon and the larger satellites of Jupiter and
Saturn. Earth and the giant planets must also have experienced an intense hail
of impactors, but their dynamic local environments have erased all evidence of
this cataclysm.
The starting point of the Late Heavy Bombardment has been
variously placed between 600 and 800 million years after the birth of the Solar
System, while its duration was in the vicinity of 10 to 150 million years (Gomes et al. 2005). By the time the dust
settled, the eight major planets had established the orbital architecture we
see today, and the second act of our drama of origin had
given way to the third.
life
The Earth as we know it was born in the Moon-forming event, meaning
that the Earth and the Moon share the same birthday. The epoch between that
date and the Late Heavy Bombardment is known as the Hadean, after the hellish
conditions once thought to prevail then. Recent evidence, however, demonstrates
that Earth cooled rapidly after the Moon’s formation, so that a global ocean was
established within 100 million years (Arndt
& Nisbet 2012), or about 4.4 billion years ago. That ocean has
persisted to the present day, rising and falling ceaselessly in response to lunar
and solar tides. (Update August 2014: for a more recent a far less benevolent picture of the Hadean, see A Billion Years of Hell on Earth.)
Already in the Hadean, then, Earth was a blue planet, with an
even smaller ratio of dry land to water than at present. Volcanism was common
on land and undersea, but no significant mountain ranges had yet developed (Arndt & Nisbet 2012). The global
temperature at that epoch remains a matter of debate, with many researchers
favoring a climate cool enough for flotillas of icebergs to populate the seas. Some
have argued that the first microbial life may have emerged during the Hadean,
perhaps in the vicinity of submerged volcanoes (Arndt
& Nisbet 2012).
The Late Heavy Bombardment that ended the era was a
catastrophe of literally cosmic proportions, yet it did not evaporate the
planetary ocean. Nor was it sufficient to sterilize our planet, if any life already
existed (Abramov & Mojzsis 2009). In
fact, the first signs of life appear right after this event, leading to some
interesting speculations. Perhaps the bombardment triggered the evolution of
the first organisms on Earth, or perhaps the impactors themselves brought
dormant organisms with them, or at least the amino acids that became their building blocks. In any event, microbial life
was abundant on Earth by 3.8 billion years ago, when the Solar System had
reached an age of about 800 million years (Arndt
& Nisbet 2012). It has survived ever since.
The emergence of multicellular organisms, however, is a far
more recent phenomenon. The Ediacaran Period, which was under way just 575 million years
ago, when the Earth was already 4 billion years old, marks “the appearance of the first
large and architecturally complex organisms in Earth history” (Narbonne 2005). The Ediacaran was immediately
followed by the better-known Cambrian Period around 540 million years ago.
Modern humans, of course, are no older than about 100,000 years or so. All our works
represent a thin veneer on a very ancient world.
Because simple organisms appeared in the Solar System well within
the first billion years after its creation, similar life forms may also have
emerged elsewhere in the system. For example, the early environments of Venus
and Mars may have been much more biophilic than they are at present, even if
nothing could survive on either planet today. Still more hopeful speculations
have addressed the icy moons of Jupiter and Saturn, some of which – Europa,
Ganymede, Enceladus – may support bodies of liquid water beneath their frozen
crusts. If they have water today, then maybe they have microbes also. Finally,
the unique environment of Titan – Saturn’s
largest moon, and the only Solar System object besides Earth that is known to
support surface bodies of liquid – may hold still more surprises in store for
us. Nothing resembling Earthly organisms could live in such a frigid place,
whose rivers run with ethane, and whose lakes are liquid hydrocarbons. Nonetheless,
it is conceivable that some as yet unimagined form of life may be drinking that
liquid or floating down those streams.
Then there are the hundreds and hundreds of exoplanetary
systems waiting for us in the Sun’s back yard. It’s becoming progressively
clearer that very few of them resemble our home system (see How Weird Is Our Solar System?). The formation scenarios presented here – Grand Tack, Terrestrial
Birth Ring, Late Heavy Bombardment – explain why our system is so unusual.
These theoretical constructs detail a highly specific evolutionary history that
is unlikely to be repeated with much regularity around other stars. Again,
however, the sheer abundance of worlds points to a similar abundance of
potential sites for life – life that is weird, unearthly, perhaps even unrecognizable
– throughout the Milky Way.
REFERENCES
Abramov O, Mojzsis SJ. (2009) Microbial habitability of the Hadean Earth
during the late heavy bombardment. Nature
459, 419-422.
Adams F, Proszkow EM, Fatuzzo M, Myers PC.
(2006) Early evolution of stellar groups and clusters: environmental effects on
forming planetary systems. Astrophysical
Journal 641, 504-525. Abstract: http://adsabs.harvard.edu/abs/2006ApJ...641..504A
Adams FC. (2010) The birth
environment of the Solar System. Annual
Review of Astronomy & Astrophysics 48, 47-85. Abstract: http://adsabs.harvard.edu/abs/2010ARA%26A..48...47A
Andrews SM, Williams JP.
(2005) Circumstellar dust disks in Taurus-Auriga: the submillimeter
perspective. Astrophysical Journal
631, 1134-1160.
Arndt NT, Nisbet EG. (2012)
Processes on the young Earth and the habitats of early life. Annual Review
of Earth & Planetary Sciences 40,
521-549. Abstract: http://adsabs.harvard.edu/abs/2012AREPS..40..521A
Batygin K, Brown ME. (2010)
Early dynamical evolution of the Solar System: pinning down the initial
conditions of the Nice model. Astrophysical
Journal 716, 1323-1331. Abstract: http://adsabs.harvard.edu/abs/2010ApJ...716.1323B
Brasser R. (2012) The
formation of Mars: Building blocks and accretion time scale. Space Science
Reviews. Abstract: http://adsabs.harvard.edu/doi/10.1007/s11214-012-9904-2
Canup RM. (2004) Dynamics of
Lunar Formation. Annual Review of
Astronomy & Astrophysics 42, 2004: 441-475.
Canup RM, Ward WR. (2006) A
common mass scaling for satellite systems of gaseous planets. Nature, 441:
834-839. Abstract: http://www.nature.com/nature/journal/v441/n7095/abs/nature04860.html
Desch SJ. (2007) Mass
distribution and planet formation in the Solar Nebula. Astrophysical Journal 671, 878-893.
Desch S, Porter S. (2010) Amphitrite:
A Twist on Triton’s Capture. 41st Lunar
and Planetary Science Conference.
Gomes R, Levison HF, Tsiganis
K, Morbidelli A. (2005) Origin of the cataclysmic Late Heavy Bombardment period
of the terrestrial planets. Nature,
435: 466-469. Abstract: http://adsabs.harvard.edu/abs/2005Natur.435..466G
Hansen B. (2009) Formation of
the terrestrial planets from a narrow annulus. Astrophysical Journal 703, 1131-1140. Abstract: http://adsabs.harvard.edu/abs/2009ApJ...703.1131H
Ida S, Lin DNC. (2004) Toward
a deterministic model of planetary formation. I. A desert in the mass and
semimajor axis distributions of extrasolar planets. Astrophysical Journal, 604: 388-413. Abstract: http://adsabs.harvard.edu/abs/2004ApJ...604..388I
Jacobsen SB. (2005) The Hf-W
isotopic system and the origin of the Earth and Moon. Annual Review of Earth
& Planetary Sciences 33, 531-70.
Jacobsen SB, Remo JL, Petaev
MI, Sasselov DD. (2009) Hf-W Chronometry and the timing of the giant
Moon-forming impact on Earth. 40th Lunar
and Planetary Science Conference.
Johansen A, Oishi JS, Mac Low
MM, Klahr H, Henning T, Youdin A. (2007) Rapid planetesimal formation in
turbulent circumstellar disks. Nature
448, 1022-1025. Abstract: http://www.nature.com/nature/journal/v448/n7157/abs/nature06086.html
Johnson JA, Aller KM, Howard
AW, Crepp JR. (2010) Giant planet occurrence in the stellar mass-metallicity
plane. Publications of the Astronomical
Society of the Pacific 122, 905-915.
Johnson JL, Li H. (2012) The
first planets: the critical metallicity for planet formation. Astrophysical Journal 751, 81. Abstract:
http://adsabs.harvard.edu/abs/2012ApJ...751...81J
Kennedy GM, Kenyon SJ. (2008)
Planet formation around stars of various masses: The snow line and the
frequency of giant planets. Astrophysical
Journal, 673:502-512.
Kirkpatrick JD, Gelino CR,
Cushing MC, Mace GN, Griffith RL, Skrutskie MF, et al. (2012) Further defining
spectral type “Y” and exploring the low-mass end of the field brown dwarf mass
function. In press. Abstract: http://arxiv.org/abs/1205.2122
Lada
CJ, Lada EA. (2003) Embedded clusters in
molecular clouds. Annual Review of
Astronomy & Astrophysics 41, 57-115. Abstract: http://adsabs.harvard.edu/abs/2003ARA%26A..41...57L
Laine RO, Lin DNC, Dong S.
(2008) Interaction of close-in planets with the magnetosphere of their host
stars. I. Diffusion, ohmic dissipation of time dependent field, planetary
inflation, and mass loss. Astrophysical
Journal 685, 521-542.
Laughlin G,
Bodenheimer P, Adams FC. (2004) The core accretion model predicts few
Jovian-mass planets orbiting red dwarfs. Astrophysical Journal, 612: L73-L76.
Abstract: http://adsabs.harvard.edu/abs/2004ApJ...612L..73L
Levison HF, Morbidelli A.
(2003) The formation of the Kuiper belt by the outward transport of bodies
during Neptune’s migration. Nature
426, 419-421.
Lin DNC. (2008) The genesis
of planets. Scientific American 298,
50-59.
Mann AW, Gaidos E, Gaudi BS.
The invisible majority? Evolution and detection of outer planetary systems
without gas giants. (2010) Astrophysical
Journal 719, 1454–1469. Abstract: http://adsabs.harvard.edu/abs/2010ApJ...719.1454M
McKee CF, Ostriker EC. (2007)
Theory of star formation. Annual Review
of Astronomy & Astrophysics 45:565-687.
Morbidelli A, Chambers J,
Lunine JI, Petit JM, Robert F, Valsecchi GB, Cyr KE. (2000) Source regions and
time scales for the delivery of water to Earth. Meteoritics and Planetary Science 35, 1309-1320.
Morbidelli A, Tsiganis K,
Crida A, Levison H, Gomes R. (2007) Dynamics of the giant planets of the Solar System
in the gaseous protoplanetary disk and their relationship to the current
orbital architecture. Astronomical Journal
134, 1790-1798.
Morbidelli A, Brasser R,
Tsiganis K, Gomes R, Levison HF. (2009a) Constructing the secular architecture
of the Solar System. I. The giant planets. Astronomy
& Astrophysics 507, 1041-1052. Abstract: http://adsabs.harvard.edu/abs/2009A%26A...507.1041M
Morbidelli A, Bottke WF,
Nesvorny D, Levison HF. (2009b) Asteroids were born big. Icarus 204, 558-573.
Morbidelli A, Walsh K,
Raymond S, O'Brien D, Mandell A. (2011) The Grand Tack scenario: Reconstructing
the migration history of Jupiter and Saturn in the disk of gas. American
Astronomical Society, ESS meeting #2, #8.02. September 2011.
Morbidelli A, Lunine JI,
O’Brien DP, Raymond SN, Walsh KJ. (2012) Building terrestrial planets. Annual Review of Earth & Planetary Sciences 40, 251-275. Abstract: http://adsabs.harvard.edu/abs/2012AREPS..40..251M
Mordasini
C, Alibert Y, Benz W, Klahr H, Henning T. (2012) Extrasolar planet population
synthesis. IV. Correlations with disk metallicity, mass, and lifetime. Astronomy &
Astrophysics 541, A97.
Narbonne GM. (2005) The
Ediacara Biota: Neoproterozoic origin of animals and their ecosystems. Annual
Review of Earth & Planetary Sciences 33, 421-442.
Parisi MG, Carraro G, Maris
M, Brunini A. (2008) Constraints to Uranus’ Great Collision IV. The origin of
Prospero. Astronomy & Astrophysics,
482: 657-664.
Pierens A, Raymond SN. (2011)
Two phase, inward-then-outward migration of Jupiter and Saturn in the gaseous
Solar Nebula. Astronomy &
Astrophysics 533, A131. Abstract: http://adsabs.harvard.edu/abs/2011A%26A...533A.131P
Patterson CC.
(1956) Age of meteorites and the earth. Geochimica
et Cosmochimica Acta 10, 230-237. Abstract: http://adsabs.harvard.edu/abs/1956GeCoA..10..230P
Russell
CT, Raymond CA, Coradini A, McSween HY, Zuber MT, Nathues A, et al. (2012) Dawn
at Vesta: Testing the protoplanetary paradigm. Science 336, 684-686.
Slattery
WL, Benz W, Cameron AG. (1992) Giant impacts on a primitive Uranus. Icarus, 99: 167-174.
Throop
HB, Bally J. (2008) "Tail-end"
Bondi-Hoyle accretion in young star clusters: Implications for disks, planets,
and stars. Astronomical Journal 135,
2380-2397.
Tsiganis K, Gomes R,
Morbidelli A, Levison HF. (2005) Origin of the orbital architecture of the
giant planets of the Solar System. Nature
435, 459-461. Abstract: http://adsabs.harvard.edu/abs/2005Natur.435..459T
Walsh KJ, Morbidelli A,
Raymond SN, O'Brien DP, Mandell AM. (2011) A low mass for Mars from Jupiter’s
early gas-driven migration. Nature
475, 206-209. Abstract: http://adsabs.harvard.edu/abs/2011Natur.475..206W
Williams JP. (2010) The astrophysical
environment of the Solar birthplace. Contemporary
Physics 51, 1-18.
Williams JP, Cieza L. (2011)
Protoplanetary disks and their evolution. Annual
Review of Astronomy & Astrophysics 49, 67-117. Abstract: http://adsabs.harvard.edu/abs/2011ARA%26A..49...67W