Using the helium triplet as a tracer of the physics of giant planet outflows

TL;DR

This paper uses radiation-hydrodynamic simulations to study helium triplet emissions as tracers of giant planet outflows, revealing insights into their cooling, ionization, and observational signatures.

Contribution

It introduces a novel application of helium triplet observations to understand the physics of giant planet atmospheric outflows, including adiabatic cooling and fractionation effects.

Findings

Helium triplet excess explains observed spectral broadening in HD 189733b.

Adiabatic cooling confirms hydrodynamic outflow nature on several planetary radii.

Helium triplet is less prone to fractionation than ground-state helium, affecting transit depth predictions.

Abstract

Hydrodynamic outflows, such as those observed escaping close-in gas giant planets, are not isothermal in structure. Their highly ionized nature allows them to cool adiabatically at distances beyond several planetary radii. The contrast between the hottest gas temperatures at around 10,000K and the coldest at around 1,000K triggers an excess population of the observable helium triplet. This excess is caused by the suppression of collisional de-excitation from the triplet state at cool temperatures. Using radiation-hydrodynamic simulations, we show that this helium triplet excess may explain the excess broadening seen in HD 189733b's observed transmission spectrum, demonstrating adiabatic cooling of its outflow, confirming its hydrodynamic nature on scales of several planetary radii. However, further observations are required to confirm this conclusion. Furthermore, we explore a range of electron transitions for neutral helium which were not considered in the previous literature. We find that the He$2^1$S state is unavailable as a potential reservoir for He$2^3$S electrons. Additionally, the de-excitation to the ground state must be considered for stellar spectra later than K2 in predicting the correct helium triplet population. Importantly, since triplet helium inherits momentum from ionized helium as it is generated by recombination, it is significantly less prone to fractionation than ground-state neutral helium. However at separations of $\gtrsim 0.05$~au, ionization at the flow base and drag on helium weaken, leading to significant fractionation of the then mostly neutral helium. This in turn, can cause a suppression of the Helium transit depth, even though the helium line width remains large.