Abstract

Abstract The slowly pulsating B star HD 50230, which is in fact a hybrid B-type pulsator, has been observed by CoRoT for at least 137 days. Nearly equidistant period spacing patterns are found among eight modes that are extracted from the oscillation spectrum with more than 500 frequencies. However, it is thought to be most likely accidental by Szewczuk et al. In the present work, we analyze the eight modes in depth with the χ 2-matching method. Based on the best-fitting model (model MA), we find that they can be well explained as sequences of consecutive dipolar (l, m) = (1, 0). The period discrepancies between observations and the best-fitting model are within 100 s except for the outlier, which is up to 300 s. Based on the calculated χ 2-minimization models, we find that, for pure g-mode oscillations, the buoyancy radius, Λ0, can be precisely measured with the χ 2-matching method between observations and calculations. It represents the “propagation time” of the g-mode from the stellar surface to the center. It is of Λ0 = 245.78 ± 0.59 μHz with a precision of 0.24%. In addition, we also find that HD 50230 is a metal-rich (Z init = 0.034–0.043) star with a mass of M = 6.15–6.27 M ⊙. It is still located in the hydrogen-burning phase with central hydrogen of X C = 0.298–0.316 (or ); therefore, it has a convective core with a radius of R cc = 0.525–0.536 R ⊙ (or ). In order to interpret the structure of the observed period spacing pattern well, the convective core overshooting (f ov = 0.0175–0.0200) and the extra diffusion mixing ( ) should be taken into account in theoretical models.

Highlights

  • Pulsating B stars are the upper main-sequence stars of intermediate mass (2.5 ∼ 8 M⊙)

  • SPB star HD 50230 is the primary component of a binary system

  • There are 8 modes to be identified as likely low-order g-mode with l = 1 and m = 0 among the extracted modes due to almost uniform period spacings among them

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Summary

INTRODUCTION

Pulsating B stars (hereafter SPB stars) are the upper main-sequence stars of intermediate mass (2.5 ∼ 8 M⊙) (more descriptions see e.g., Aerts, Christensen-Dalsgaard, & Kurtz 2010). They found that the magnetic field cause a suppression of near-core mixing in this star and it has a lower convective core overshooting parameter (fov = 0.004+−00..001042) These previous works, Moravveji et al (2015), Moravveji et al (2016), and Buysschaert et al (2018), give us so much new insights in seismically modelling SPB stars and make us on a higher level to learn the interior structure of SPB stars, such as the connection among the extra diffusive mixing, the shape of buoyancy frequency N , and the structure of period spacing pattern, the relationship and/or interaction among convective core overshooting, rotation, and magnetic field.

HD50230
Physical inputs
Modelling and Finding the Best Fitting Model
RESULTS
Buoyancy radius Λ0
Fundamental parameters
Statistical Analysis
Asteroseismic analysis
SUMMARY
Full Text
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