On the rotational evolution of solar- and late-type stars, its magnetic origins, and the possibility of stellar gyrochronology

Details On the rotational evolution of solar- and late-type stars, its magnetic origins, and the possibility of stellar gyrochronology On the rotational evolution of solar- and late-type stars, its magnetic origins, and the possibility of stellar gyrochronology

2003-03-28

arxiv.org/abs/astro-ph/0303631v1

Astrophys.J. 586 (2003) 464

Astronomy and Astrophysics

Astrophysics

32 pages, 6 figures (4 in color), accepted by ApJ

Scientific paper

10.1086/367639

We propose a simple interpretation of the rotation period data for solar- and late-type stars. The open cluster and Mt. Wilson star observations suggest that rotating stars lie primarily on two sequences, initially called I and C. Some stars lie in the intervening gap. These sequences, and the fractional numbers of stars on each sequence evolve systematically with cluster age, enabling us to construct crude rotational isochrones allowing `stellar gyrochronology', a procedure, upon improvement, likely to yield ages for individual field stars. The age and color dependences of the sequences allow the identification of the underlying mechanism, which appears to be primarily magnetic. The majority of solar- and late-type stars possess a dominant Sun-like, or Interface magnetic field, which connects the convective envelope both to the radiative interior of the star and to the exterior where winds can drain off angular momentum. These stars spin down Skumanich-style. An age-decreasing fraction of young G, K, and M stars, which are rapid rotators, possess only a Convective field which is not only inefficient in depleting angular momentum, but also incapable of coupling the surface convection zone to the inner radiative zone, so that only the outer zone is spun down, and on an exponential timescale. These stars do not yet possess large-scale dynamos. The large-scale magnetic field associated with the dynamo, apparently created by the shear between the decoupled radiative and convective zones, (re)couples the convective and radiative zones and drives a star from the Convective to the Interface sequence through the gap on a timescale that increases as stellar mass decreases. (Abstract is truncated here.)

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