Signatures of the Core-Powered Mass-Loss Mechanism in the Exoplanet Population: Dependence on Stellar Properties and Observational Predictions

Akash Gupta; Hilke E. Schlichting

doi:10.1093/mnras/staa315

paper

Signatures of the Core-Powered Mass-Loss Mechanism in the Exoplanet Population: Dependence on Stellar Properties and Observational Predictions

arXiv:1907.03732 · doi:10.1093/mnras/staa315

Abstract

Recent studies have shown that atmospheric mass-loss powered by the cooling luminosity of a planet's core can explain the observed radius valley separating super-Earths and sub-Neptunes, even without photoevaporation. In this work, we investigate the dependence of this core-powered mass-loss mechanism on stellar mass ( $M_{*}$ ), metallicity ( $Z_{*}$ ) and age ( $τ_{*}$ ). Without making any changes to the underlying planet population, we find that the core-powered mass-loss model yields a shift in the radius valley to larger planet sizes around more massive stars with a slope given by $d log R_{p} / d log M_{*} ≃ 0.35$ , in agreement with observations. To first order, this slope is driven by the dependence of core-powered mass-loss on the bolometric luminosity of the host star and is given by $d log R_{p} / d log M_{*} ≃ (3 α - 2) /36 ≃ 0.33$ , where $(L_{*} / L_{⊙}) = (M_{*} / M_{⊙})^{α}$ is the stellar mass-luminosity relation and $α ≃ 4.6$ for the CKS dataset. We therefore find, in contrast to photoevaporation models, no evidence for a linear correlation between planet and stellar mass, but can't rule it out either. In addition, we show that the location of the radius valley is, to first order, independent of stellar age and metallicity. Since core-powered mass-loss proceeds over Gyr timescales, the abundance of super-Earths relative to sub-Neptunes increases with age but decreases with stellar metallicity. Finally, due the dependence of the envelope's cooling timescale on metallicity, we find that the radii of sub-Neptunes increase with metallicity and decrease with age with slopes given by $d log R_{p} / d log Z_{*} ≃ 0.1$ and $d log R_{p} / d log τ_{*} ≃ - 0.1$ , respectively. We conclude with a series of observational tests that can differentiate between core-powered mass-loss and photoevaporation models.

arXiv comment16 pages and 11 figures. Submitted to MNRAS. Revised version

Signatures of the Core-Powered Mass-Loss Mechanism in the Exoplanet Population: Dependence on Stellar Properties and Observational Predictions

Abstract

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