Abstract.White dwarfs represent the end point of stellar evolution for the majority of stars. As such, they are excellent astrophysical laboratories. They are structurally simple, with electron degenerate cores surrounded by thin surface layers of helium and/or hydrogen. The g-mode pulsations provide a window into their internal structure. The Whole Earth Telescope has been conducting a long-term survey of pulsating white dwarfs with the goal of providing an empirical map of convection parameters across the DA and DB instability strips. We present an overview of white dwarf asteroseismology, and discuss the current status of our survey.
White dwarf asteroseismology and diagnosticsAsteroseismology provides us with a window through which to peer into stellar interiors. Through asteroseismology, we can study fundamental problems in stellar evolution such as energy transport, thermodynamics, and magnetism. White dwarfs (WDs) are particularly important targets for asteroseismology. WDs are the most numerous inhabitants of the stellar graveyard. WDs are structurally simple: an electron degenerate carbon/oxygen core surrounded by thin non-degenerate layers of hydrogen and helium. In broad brush strokes, WDs are divided into two classes by their atmospheric compositions. DA white dwarfs have nearly pure hydrogen layers on top of a layer of helium. DAs represent ≈80% of the population ([2]). DB white dwarfs are characterized by a layer of nearly pure helium overlying their carbon/oxygen cores. Lacking substantial nuclear reactions, white dwarfs simply cool as they age, passing through specific temperature ranges (the DBV and DAV instability strips) within which they pulsate. These pulsators are otherwise normal objects, so what we learn about their structure can be applied to the WD entire population to further our understanding of stellar evolution.WDs are g-mode pulsators, and we assume that each pulsation mode can be described by a spherical harmonic of degree , radial overtone k, and azimuthal number m, where m takes integer values between − and . A key diagnostic for g-mode pulsators is the mean period spacing ΔP between modes of the same ( , m) but consecutive radial overtone k (Fig. 1). ΔP depends primarily on stellar mass. Deviations of individual spacings from this mean value provide information on both the Figure 1. A schematic representation of the distribution of pulsation frequencies for the prototype DBV GD358. The systematic distribution of frequencies into a series of modes is evident.structure of the surface layers and the degenerate core ([4]). A second diagnostic is the presence of multiplets. The multiplet components have the same ( , k) but different values of the azimuthal index m. In the limit of slow rotation, the frequency difference between multiplet components is an indicator of rotation as sampled by a given mode. Multiplet structure is also a strong indication of a mode's value. We expect a triplet for = 1, a quintuplet for = 2, and so on. Deviations from equal frequency splitting within a s...