The fundamentals of Lyman α exoplanet transits

Author:

Owen James E1ORCID,Murray-Clay Ruth A2,Schreyer Ethan1,Schlichting Hilke E345,Ardila David6,Gupta Akash3ORCID,Loyd R O Parke78,Shkolnik Evgenya L7,Sing David K910,Swain Mark R6

Affiliation:

1. Astrophysics Group, Imperial College London , Blackett Laboratory, Prince Consort Road, London SW7 2AZ, UK

2. Department of Astronomy and Astrophysics, University of California , Santa Cruz, CA 95064, USA

3. Department of Earth, Planetary, and Space Sciences, University of California , Los Angeles, CA 90095, USA

4. Department of Physics and Astronomy, University of California , Los Angeles, CA 90095, USA

5. Department of Earth, Atmospheric and Planetary Sciences, Massachusetts Institute of Technology , MA 02139, USA

6. Jet Propulsion Laboratory, California Institute of Technology , 4800 Oak Grove Drive, Pasadena, CA 91109, USA

7. School of Earth and Space Exploration, Arizona State University , Tempe, AZ 85287, USA

8. Eureka Scientific , 2452 Delmer Street Suite 100, Oakland, CA 94602-3017, USA

9. Department of Earth & Planetary Sciences, Johns Hopkins University , Baltimore, MD 21210, USA

10. Department of Physics & Astronomy, Johns Hopkins University , Baltimore, MD 21210, USA

Abstract

ABSTRACT Lyman α transits have been detected from several nearby exoplanets and are one of our best insights into the atmospheric escape process. However, due to ISM absorption, we typically only observe the transit signature in the blue-wing, making them challenging to interpret. This challenge has been recently highlighted by non-detections from planets thought to be undergoing vigorous escape. Pioneering 3D simulations have shown that escaping hydrogen is shaped into a cometary tail receding from the planet. Motivated by this work, we develop a simple model to interpret Lyman α transits. Using this framework, we show that the Lyman α transit depth is primarily controlled by the properties of the stellar tidal field rather than details of the escape process. Instead, the transit duration provides a direct measurement of the velocity of the planetary outflow. This result arises because the underlying physics is the distance a neutral hydrogen atom can travel before it is photoionized in the outflow. Thus, higher irradiation levels, expected to drive more powerful outflows, produce weaker, shorter Lyman α transits because the outflowing gas is ionized more quickly. Our framework suggests that the generation of energetic neutral atoms may dominate the transit signature early, but the acceleration of planetary material produces long tails. Thus, Lyman α transits do not primarily probe the mass-loss rates. Instead, they inform us about the velocity at which the escape mechanism is ejecting material from the planet, providing a clean test of predictions from atmospheric escape models.

Funder

European Research Council

NSF

NASA

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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1. Using Ly α transits to constrain models of atmospheric escape;Monthly Notices of the Royal Astronomical Society;2024-08-17

2. TOI-1173 A b: The First Inflated Super-Neptune in a Wide Binary System;The Astronomical Journal;2024-07-25

3. 3D aeronomy of two mini-neptunes in the HD 63433 system and their in-transit absorption in Ly α and metastable He i lines;Monthly Notices of the Royal Astronomical Society;2024-07-02

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