This study compares the theoretical pulsation periods from an extensivegrid of evolutionary DA white dwarf models with the observed periods ofthe ZZ Ceti white dwarfs L19-2 and GD 165, in order to constrain theirinternal structure. Our analysis of the rotational fine-structuresplitting and comparison of our theoretical periods with observationsfor L19-2 and GD 165 enable us to identify the observed modes aslow-order l=1 and 2 g-modes. Because the period structure of GD 165 isquite similar to that of L19-2, we believe that the interior structureof GD 165 is similar. The short period of the l=1 118.5 s mode of L19-2(120.4 s mode of GD 165) implies a hydrogen layer mass of about10^{-4} M_{*}, independent of constraints from the otherpulsation modes. Detailed model fitting shows that L19-2 has a hydrogenlayer mass of 1.0{\times}10^{-4} M_{*}, a helium layermass of 1.0{\times}10^{-2} M_{*}, a 20:80 C/O core thatextends out to 0.60 M_{*}, a stellar mass of 0.72M_{solar}, and a rotation period of about 13 hr. Thebest-fitting models for GD 165 have a hydrogen layer mass of 1.5 to2.0{\times}10^{-4} M_{*}, a helium layer mass of 1.5 to2.0{\times}10^{-2} M_{*}, a 20:80 C/O core that extendsout to 0.65 M_{*}, a stellar mass of 0.65-0.68M_{solar}, and a rotation period of about 58 hr. In both cases,the best-fitting models are consistent with the spectroscopic logg-value, and the seismological parallax is within 1 {$σ$} of theobserved parallax value.
CITATION STYLE
Bradley, P. A. (2001). Asteroseismological Constraints on the Structure of the ZZ Ceti Stars L19‐2 and GD 165. The Astrophysical Journal, 552(1), 326–339. https://doi.org/10.1086/320454
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