4.7 Article

A deep radius valley revealed by Kepler short cadence observations

Journal

MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY
Volume 519, Issue 3, Pages 4056-4073

Publisher

OXFORD UNIV PRESS
DOI: 10.1093/mnras/stac3802

Keywords

planets and satellites; composition - planets and satellites; formation - planets and satellites; fundamental parame-ters

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The lack of planets between 1.5 and 2 Earth radii at periods shorter than about 100 days, known as the radius valley, sheds light on the formation and evolution of close-in planets. By reanalyzing the transits of 431 planets using Kepler's 1-min short cadence observations, we reveal a deeper radius valley than previously observed, indicating a more homogeneous core composition during formation. Our findings suggest that the location of the radius valley strongly depends on orbital period and stellar mass, with a weak dependence on stellar age. This study emphasizes the importance of precise transit observations with a short photometric cadence in determining planet radii, and provides an updated list of accurately determined parameters for the studied planets.
The characteristics of the radius valley, i.e. an observed lack of planets between 1.5 and 2 Earth radii at periods shorter than about 100 d, provide insights into the formation and evolution of close-in planets. We present a novel view of the radius valley by refitting the transits of 431 planets using Kepler 1-min short cadence observations, the vast majority of which have not been previously analysed in this way. In some cases, the updated planetary parameters differ significantly from previous studies, resulting in a deeper radius valley than previously observed. This suggests that planets are likely to have a more homogeneous core composition at formation. Furthermore, using support vector machines, we find that the radius valley location strongly depends on orbital period and stellar mass and weakly depends on stellar age, with $\partial \log {\left(R_{\rm p, \text{valley}} \right)}/ \partial \log {P} = -0.096_{-0.027}<^>{+0.023}$, $\partial \log {\left(R_{\rm p, \text{valley}} \right)}/ \partial \log {M_{\star }} = 0.231_{-0.064}<^>{+0.053}$, and $\partial \log {\left(R_{\rm p, \text{valley}} \right)}/ \partial \log {\left(\text{age} \right)} = 0.033_{-0.025}<^>{+0.017}$. These findings favour thermally driven mass-loss models such as photoevaporation and core-powered mass-loss, with a slight preference for the latter scenario. Finally, this work highlights the value of transit observations with a short photometric cadence to precisely determine planet radii, and we provide an updated list of precisely and homogeneously determined parameters for the planets in our sample.

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