Abstract

Abstract Two magnetic braking models are implemented in MESA for use in the MIST stellar model grids. Stars less than about 1.3 solar masses are observed to spin down over time through interaction with their magnetized stellar winds (i.e., magnetic braking). This is the basis for gyrochronology and is fundamental to the evolution of lower-mass stars. The detailed physics behind magnetic braking are uncertain, as are 1D stellar evolution models. Thus, we calibrate our models and compare to data from open clusters. Each braking model tested here is capable of reproducing aspects of the data, with important distinctions; neither fully accounts for the observations. The Matt et al. prescription matches the slowly rotating stars observed in open clusters but tends to overestimate the presence of rapidly rotating stars. The Garraffo et al. prescription often produces too much angular momentum loss to accurately match the observed slow sequence for lower-mass stars but reproduces the bimodal nature of slowly and rapidly rotating stars observed in open clusters fairly well. Our models additionally do not reproduce the observed solar lithium depletion, corroborating previous findings that effects other than rotation may be important. We find additional evidence that some level of mass dependency may be missing in these braking models to match the rotation periods observed in clusters older than 1 Gyr better.

Highlights

  • Stellar rotation rate is one of the fundamental properties of stars, determining all other properties of a star throughout their evolution, alongside stellar mass and metallicity

  • Two magnetic braking models are implemented in MESA for use in the MIST stellar model grids

  • This may aid in reproducing the solar lithium abundance, and in matching the behavior of rapidly rotating low mass stars at ages of the Praesepe and prior, and as a possible mechanism for the observed stall in angular momentum loss (Agueros et al 2018; Curtis et al 2019) at later ages

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Summary

Introduction

Stellar rotation rate is one of the fundamental properties of stars, determining all other properties of a star throughout their evolution, alongside stellar mass and metallicity. Due to the immense challenges of full, 3D stellar modeling, we rely on have only recently become available. Grids that fully model 1D stellar rotation have been limited by a lack of models that describe the spin evolution of low mass stars (i.e., with about M < 1.3M ) in this context. The magnetic coupling between star and stellar wind, leading to a slowing of the stellar rotation rate is commonly called magnetic braking. This phenomenon was inferred early on by Kraft (1967) and Skumanich (1972) in nearby stars, but was theoretically anticipated beforehand as in e.g., Schatzman (1962); Brandt (1966); Weber & Davis (1967)

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