Credit: NASA’s Goddard Space Flight Center Conceptual Image Lab
Title: Formation History of HD106906 and the Vertical Warping of Debris Disks by an External Inclined Companion
Authors: Nathaniel Moore et al.
First Author’s Institution: Georgia Institute of Technology
Status: Accepted to ApJ
There are two main theories for the formation of planets: core accretion and gravitational instability (also called the gas-collapse model). Figure 1 shows the two different scenarios. In both cases, the planets form in a protoplanetary disk, which means that the planets initially start in the same orbital plane. A system like HD 106906 challenges this notion, since it has a very massive planet far away from the disk and in a different orbital plane. The authors of this article explore the idea that the planet HD 106906 b actually formed from the disk, but a recent (about 1–5 million years ago) close encounter with a free-floating planet knocked the planet away from the disk into an eccentric orbit, and the interactions from this close encounter actually caused the disk to become more eccentric as well. The authors explore this idea using N-body simulations (a simulation of how bodies interact over a period of time) of the system combined with simulations of how the observational data would look for this scenario. They then compare the simulations to real observations.
Figure 1. The two possible scenarios for planet formation: accretion model (“bottom-up”) and gravitational instability (“top-down”). Click to enlarge. Credit: NASA and A. Feild (STScI); CC BY 4.0
Companion and Disk Interactions
The authors first try to determine whether the HD 106906 system has been
like this for a long time or if its current configuration is the result
of a recent event. To do this, they simulate different variations of
the planet’s eccentricity, inclination, and semi-major axis. For the simulations, they include the effects of radiation pressure.
They also use two different central body configurations: one with a
binary star system and another with a single central body and an extra J2 potential
term, which emulates the binary system but is more computationally
efficient. The main results from these simulations are shown in Figure
2.
Knock, Knock. Who’s There?
The team’s final results are shown in Figure 4. From the figure, we
can see that a few outcomes in which either the free-floating planet
stays in the system or the native planet stays in the system agree with
observations. The authors conclude that an encounter with a
free-floating planet is a possible explanation for the current
architecture of this system. The close encounter only reproduces
observational results 0.2% of the time, but this system is quite unusual
— so a low probability of a system forming like this is expected!
Figure 4: The final results of the close encounter simulations of the free-floating planet and the HD 106906 system. The dots within the dashed square fall within the expected observational constraints of the companion (i.e., that agree with current estimates for the orbital eccentricity, semi-major axis, and inclination of the companion). The blue dots represent the outcomes that agree with observations where the native planet remains bound to the system. The red dots represent the outcomes where the free-floating planet remains bound to the system. The gray dots represent the other parameters of the 100,000 simulations. Credit: Moore et al. 2022
Original astrobite edited by H Perry Hatchfield.
About the author, Clarissa Do O: