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In-depth characterization of the Kepler-10 three-planet system with HARPS-N radial velocities and Kepler transit timing variations

  • A. S. Bonomo*
  • , L. Borsato
  • , V. M. Rajpaul
  • , L. Zeng
  • , M. Damasso
  • , N. C. Hara
  • , M. Cretignier
  • , A. Leleu
  • , N. Unger
  • , X. Dumusque
  • , F. Lienhard
  • , A. Mortier
  • , L. Naponiello
  • , L. Malavolta
  • , A. Sozzetti
  • , D. W. Latham
  • , K. Rice
  • , R. Bongiolatti
  • , L. Buchhave
  • , A. C. Cameron
  • A. F. Fiorenzano, A. Ghedina, R. D. Haywood, G. Lacedelli, A. Massa, F. Pepe, E. Poretti, S. Udry
*Corresponding author for this work
  • National Institute for Astrophysics
  • Astronomical Observatory of Padua
  • University of Cambridge
  • Harvard University
  • CNRS
  • University of Oxford
  • University of Geneva
  • University of Birmingham
  • University of Padua
  • Harvard-Smithsonian Center for Astrophysics
  • University of Edinburgh
  • University of Milan
  • University of St Andrews
  • INAF - Fundacion Galileo Galilei
  • University of Exeter
  • University of Turin

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Abstract

The old G3V star Kepler-10 is known to host two transiting planets, the ultra-short-period super-Earth Kepler-10 b (Pb = 0.837 d; Rb = 1.47 R) and the long-period sub-Neptune Kepler-10 c (Pc = 45.294 d; Rc = 2.35 R), and a non-transiting planet that causes variations in the Kepler-10 c transit times. Measurements of the mass of Kepler-10 c in the literature have shown disagreement, depending on the radial-velocity dataset and/or the modeling technique used. Here we report on the analysis of almost 300 high-precision radial velocities gathered with the HARPS-N spectrograph at the Telescopio Nazionale Galileo over ∼11 years, and extracted with the YARARA-v2 tool, which corrects for possible systematics and/or low-level activity variations at the spectrum level. To model these radial velocities, we used three different noise models and various numerical techniques, which all converged to the solution: Mb = 3.24 ± 0.32 M (10σ) and ρb = 5.54 ± 0.64 g cm−3 for planet b; Mc = 11.29 ± 1.24 M (9σ) and ρc = 4.75 ± 0.53 g cm−3 for planet c; and Md sin i = 12.00 ± 2.15 M (6 σ) and Pd = 151.06 ± 0.48 d for the non-transiting planet Kepler-10 d. This solution is further supported by the analysis of the Kepler-10 c transit timing variations and their simultaneous modeling with the HARPS-N radial velocities. While Kepler-10 b is consistent with a rocky composition and a small or no iron core, Kepler-10 c may be a water world that formed beyond the water snowline and subsequently migrated inward.
Original languageEnglish
Article numberA233
JournalAstronomy and Astrophysics
Volume696
Number of pages21
ISSN0004-6361
DOIs
Publication statusPublished - 2025

Keywords

  • Planets and satellites: composition
  • Planets and satellites: detection
  • Planets and satellites: fundamental parameters
  • Techniques: photometric
  • Techniques: radial velocities

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