Constraints on the Spindown of Fully Convective M Dwarfs Using Wide Field Binaries

• Published in: The Astrophysical journal 2022-09, Vol.936 (2), p.109
• Main Authors: Pass, Emily K., Charbonneau, David, Irwin, Jonathan M., Winters, Jennifer G.
• Format: Article
• Language: English
• Subjects: Angular momentum; Astrophysics; Binary systems; Cooling curves; Extrasolar planets; Lithium; Low mass stars; M dwarf stars; Magnetic fields; Planet detection; Planetary atmospheres; Red dwarf stars; Stellar activity; Stellar ages; Stellar rotation; Transit; White dwarf stars; Wide binary stars
• ISSN: 0004-637X; 1538-4357
• DOI: 10.3847/1538-4357/ac7da8

M dwarfs remain active over longer timescales than their Sunlike counterparts, with potentially devastating implications for the atmospheres of their planets. However, the age at which fully convective M dwarfs transition from active and rapidly rotating to quiescent and slowly rotating is poorly understood, as these stars remain rapidly rotating in the oldest clusters that are near enough for a large sample of low-mass M dwarfs to be studied. To constrain the spindown of these low-mass stars, we measure photometric rotation periods for field M dwarfs in wide binary systems, primarily using the Transiting Exoplanet Survey Satellite and MEarth. Our analysis includes M–M pairs, which are coeval but of unknown age, as well as M dwarfs with white dwarf or Sunlike primaries, for which we can estimate ages using techniques like white-dwarf cooling curves, gyrochronology, and lithium abundance. We find that the epoch of spindown is strongly dependent on mass. Fully convective M dwarfs initially spin down slowly, with the population of 0.2–0.3 M ⊙ rapid rotators evolving from P rot < 2 days at 600 Myr to 2 < P rot < 10 days at 1–3 Gyr before rapidly spinning down to long rotation periods at older ages. However, we also identify some variability in the spindown of fully convective M dwarfs, with a small number of stars having substantially spun down by 600 Myr. These observations are consistent with models of magnetic morphology-driven spindown, where angular momentum loss is initially inefficient until changes in the magnetic field allow spindown to progress rapidly.