2021/08/24 by Keighley E. Rockcliffe, Elisabeth Newton, Elisabeth R. Newton +9
Chemistry · Physics and Astronomy · #Astro and Planetary Science #Astronomy #Astrophysics #Astrophysics and Star Formation Studies #Atmosphere (unit) #Atmospheric escape #Chemistry #Exoplanet #Flux (metallurgy) #Ion #Ionization #Meteorology #Photoionization #Physics #Planet #Stellar, planetary, and galactic studies #Sunset #astro-ph.EP
paper · pdf · doi:10.3847/1538-3881/ac126f
published as AJ, 162, 116 (2021)
openalex publication_date 2021/08/24 · openalex created_date 2021/08/30 · arxiv created 2021/09/09 · arxiv updated 2021/09/10 · openalex updated_date 2026/08/05
Abstract K2-25b is a Neptune-sized exoplanet (3.45 R ⊕ ) that orbits its M4.5 host with a period of 3.48 days. Due to its membership in the Hyades Cluster, the system has a known age (727 ± 75 Myr). K2-25b’s youth and its similarities with Gl 436b suggested that K2-25b could be undergoing strong atmospheric escape. We observed two transits of K2-25b at Ly α using HST/STIS in order to search for escaping neutral hydrogen. We were unable to detect an exospheric signature, but placed an upper limit of ( R p / R ⋆ )∣ Ly α < 0.56 at 95% confidence by fitting the light curve of the Ly α red wing, or < 1.20 in the blue wing. We reconstructed the intrinsic Ly α profile of K2-25 to determine its Ly α flux, and analyzed XMM-Newton observations to determined its X-ray flux. Based on the total X-ray and extreme ultraviolet irradiation of the planet (8763 ± 1049 erg s −1 cm −2 ), we estimated the maximum energy-limited mass-loss rate of K2-25b to be <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:msubsup> <mml:mrow> <mml:mn>10.6</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>6.13</mml:mn> </mml:mrow> <mml:mrow> <mml:mo>+</mml:mo> <mml:mn>15.2</mml:mn> </mml:mrow> </mml:msubsup> <mml:mo>×</mml:mo> <mml:msup> <mml:mrow> <mml:mn>10</mml:mn> </mml:mrow> <mml:mrow> <mml:mn>10</mml:mn> </mml:mrow> </mml:msup> </mml:math> g s −1 (0.56 M ⊕ per 1 Gyr), five times larger than the similarly estimated mass-loss rate of Gl 436b (2.2 × 10 10 g s −1 ). The photoionization time is about 3 hr, significantly shorter than Gl 436b’s 14 hr. A nondetection of a Ly α transit could suggest K2-25b is not significantly losing its atmosphere, or factors of the system are resulting in the mass loss being unobservable (e.g., atmosphere composition or the system’s large high-energy flux). Further observations could provide more stringent constraints.