2025A&A...696A.174C


Query : 2025A&A...696A.174C

2025A&A...696A.174C - Astronomy and Astrophysics, volume 696A174 (2025/4-1)

Can metal-rich worlds form by giant impacts?

CAMBIONI S., WEISS B.P., ASPHAUG E., VOLK K., EMSENHUBER A., BIERSTEKER J.B., LIN Z. and MELIKYAN R.

Abstract (from CDS):

Context. Astronomical observations revealed the existence of exoplanets whose densities are far higher than what is expected from cosmochemistry. This high-density planetary population may account for 9% of terrestrial planets, suggesting the existence of processes that form planets with compositions dramatically different from their starting materials.
Aims. A commonly invoked theory is that these high-density exoplanets are the metallic cores of super-Earth-sized planets whose rocky mantle was stripped by giant impacts. Here we aim to test this hypothesis.
Methods. To maximize the likelihood that metal-rich giant-impact remnants form, we model the late orbital instability of tightly packed super-Earths orbiting a host star at small stellocentric distances (“compact systems”). We combine orbital dynamics, impact physics, and machine learning to explore the stability and collisional evolution of 100 observed compact systems. In each unstable compact system, we assume that the super-Earths undergo giant impacts and explore 1000 possible collision scenarios. We repeat the simulations with different initial conditions, such as the initial masses and composition of the super-Earths.
Results. We find that giant impacts are capable of stripping the mantles of super-Earths and form metal-rich worlds as massive and large as the observed high-density exoplanets. However, we also find that, in most of the explored scenarios, mantle-stripping giant impacts between super-Earths are unlikely to occur at rates sufficient to explain the size and currently estimated abundance of the observed high-density exoplanets. We explain this as the interplay of three factors: the size of the super-Earths being in most cases smaller than 2 Earth radii; the efficiency of mantle stripping decreasing with increasing planetary size; and the likelihood of compact system instability decreasing with increasing average sizes of the planets in the compact system.
Conclusions. We conclude that most of the observed high-density exoplanets are unlikely to be metal-rich giant-impact remnants.

Abstract Copyright: © The Authors 2025

Journal keyword(s): methods: numerical - planets and satellites: composition - planets and satellites: dynamical evolution and stability - planets and satellites: formation - planets and satellites: physical evolution - planets and satellites: terrestrial planets

Simbad objects: 17

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Number of rows : 17
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 K2-106b Pl 00 52 19.1415736296 +10 47 40.906374828           ~ 67 0
2 LSPM J0106+1913b Pl 01 06 36.9754315896 +19 13 33.163383396           ~ 21 0
3 CD-26 2288b Pl 05 33 04.6005234792 -26 43 28.268361984           ~ 37 0
4 HD 42813d Pl 06 12 13.9672254588 -14 39 00.061845960           ~ 6 0
5 CD-45 5378b Pl 09 44 29.8367689785 -45 46 35.427639685           ~ 86 0
6 BD-05 3504b Pl 12 27 29.5846968120 -06 43 18.766944228           ~ 58 0
7 HD 137496b Pl 15 26 58.0705591632 -16 30 31.676789772           ~ 19 0
8 NAME G 180-18b Pl 15 58 18.7976355993 +35 24 24.279816765           ~ 28 0
9 K2-38b Pl 16 00 08.0580517944 -23 11 21.329133720           ~ 42 0
10 Kepler-105c Pl 19 11 32.9514004104 +46 16 34.384220652           ~ 53 0
11 Kepler-402 Er* 19 13 28.8534589176 +43 21 16.582563936   13.884 13.317 13.177   F2 75 0
12 Kepler-245c Pl 19 26 33.3541730304 +42 26 10.779132804           ~ 27 0
13 Kepler-406b Pl 19 27 23.5375431360 +44 58 05.726111052           ~ 77 0
14 Kepler-80 Er* 19 44 27.0200680656 +39 58 43.594100688   16.303 15.201 14.866   M0V 177 1
15 Kepler-80d Pl 19 44 27.0200680656 +39 58 43.594100688           ~ 54 1
16 Kepler-107c Pl 19 48 06.7734610824 +48 12 30.964175676           ~ 75 0
17 CD-60 8051b Pl 23 20 07.5245143451 -60 03 54.644648069           ~ 67 0

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