Relation of X-ray activity and rotation in M dwarfs and predicted time-evolution of the X-ray luminosity

preprint2020arXivOpen access

Abstract

We present a sample of 14 M dwarf stars observed with XMM-Newton and Chandra, for which we also computed rotational periods from Kepler Two-Wheel (K2) Mission light curves. We compiled X-ray and rotation data from the literature and homogenized all data sets to provide the largest uniform sample of M dwarfs (302 stars) for X-ray activity and rotation studies to date. We then fit the relation between Lx−ProtL_{\rm x} - P_{\rm rot} using three different mass bins to separate partially and fully convective stars. We found a steeper slope in the unsaturated regime for fully convective stars and a nonconstant LxL_{\rm x} level in the saturated regime for all masses. In the Lx/Lbol−ROL_{\rm x}/L_{\rm bol}-R_{\rm O} space we discovered a remarkable double gap that might be related to a discontinuous period evolution. Then we combined the evolution of ProtP_{\rm rot} predicted by angular momentum evolution models with our new results on the empirical Lx−ProtL_{\rm x} - P_{\rm rot} relation to provide an estimate for the age decay of X-ray luminosity. We compare predictions of this relationship with the actual X-ray luminosities of M stars with known ages from 100 Myr to a few billion years. We find remarkably good agreement between the predicted LxL_{\rm x} and the observed values for partially convective stars. However, for fully convective stars at ages of a few billion years, the constructed Lx−L_{\rm x}-age relation overpredicts the X-ray luminosity because the angular momentum evolution model underpredicts the rotation period of these stars. Finally, we examine the effect of different parameterizations for the Rossby number (ROR_{\rm O}) on the shape of the activity-rotation relation in Lx/Lbol−ROL_{\rm x}/L_{\rm bol}-R_{\rm O} space, and we find that the slope in the unsaturated regime and the location of the break point of the dual power-law depend sensitively on the choice of ROR_{\rm O}.

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