A warm Neptune's methane reveals core mass and vigorous atmospheric mixing.

Sing, David K; Rustamkulov, Zafar; Thorngren, Daniel P; Barstow, Joanna K; Tremblin, Pascal; Alves de Oliveira, Catarina; Beck, Tracy L; Birkmann, Stephan M et al. · Nature · 2024

basic_science · Level V

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Abstract

Observations of transiting gas giant exoplanets have revealed a pervasive depletion of methane<sup>1-4</sup>, which has only recently been identified atmospherically<sup>5,6</sup>. The depletion is thought to be maintained by disequilibrium processes such as photochemistry or mixing from a hotter interior<sup>7-9</sup>. However, the interiors are largely unconstrained along with the vertical mixing strength and only upper limits on the CH<sub>4</sub> depletion have been available. The warm Neptune WASP-107b stands out among exoplanets with an unusually low density, reported low core mass<sup>10</sup>, and temperatures amenable to CH<sub>4</sub>, though previous observations have yet to find the molecule<sup>2,4</sup>. Here we present a JWST-NIRSpec transmission spectrum of WASP-107b that shows features from both SO<sub>2</sub> and CH<sub>4</sub> along with H<sub>2</sub>O, CO<sub>2</sub>, and CO. We detect methane with 4.2σ significance at an abundance of 1.0 ± 0.5 ppm, which is depleted by 3 orders of magnitude relative to equilibrium expectations. Our results are highly constraining for the atmosphere and interior, which indicate the envelope has a super-solar metallicity of 43 ± 8 × solar, a hot interior with an intrinsic temperature of T<sub>int</sub> = 460 ± 40 K, and vigorous vertical mixing which depletes CH<sub>4</sub> with a diffusion coefficient of K<sub>zz</sub> = 10<sup>11.6±0.1</sup> cm<sup>2</sup> s<sup>-1</sup>. Photochemistry has a negligible effect on the CH<sub>4</sub> abundance but is needed to account for the SO<sub>2</sub>. We infer a core mass of <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow> <msubsup><mrow><mn>11.5</mn></mrow> <mrow><mo>-</mo> <mn>3.6</mn></mrow> <mrow><mo>+</mo> <mn>3.0</mn></mrow> </msubsup> <msub><mrow><mi>M</mi></mrow> <mrow><mo>⊕</mo></mrow> </msub> </mrow> </math> , which is much higher than previous upper limits<sup>10</sup>, releasing a tension with core-accretion models<sup>11</sup>.