Abstract

We present our analysis of HD~35502 based on high- and medium-resolution spectropolarimetric observations. Our results indicate that the magnetic B5IVsnp star is the primary component of a spectroscopic triple system and that it has an effective temperature of 18.4±0.6 kK18.4\pm0.6\,{\rm kK}, a mass of 5.7±0.6 M⊙5.7\pm0.6\,M_\odot, and a polar radius of 3.0−0.5+1.1 R⊙3.0^{+1.1}_{-0.5}\,R_\odot. The two secondary components are found to be essentially identical A-type stars for which we derive effective temperatures (8.9±0.3 kK8.9\pm0.3\,{\rm kK}), masses (2.1±0.2 M⊙2.1\pm0.2\,M_\odot), and radii (2.1±0.4 R⊙2.1\pm0.4\,R_\odot). We infer a hierarchical orbital configuration for the system in which the secondary components form a tight binary with an orbital period of 5.66866(6) d5.66866(6)\,{\rm d} that orbits the primary component with a period of over 40 yrs40\,{\rm yrs}. Least-Squares Deconvolution (LSD) profiles reveal Zeeman signatures in Stokes VV indicative of a longitudinal magnetic field produced by the B star ranging from approximately −4-4 to 0 kG0\,{\rm kG} with a median uncertainty of 0.4 kG0.4\,{\rm kG}. These measurements, along with the line variability produced by strong emission in Hαα, are used to derive a rotational period of 0.853807(3) d0.853807(3)\,{\rm d}. We find that the measured vsin⁡i=75±5 km s−1v\sin{i}=75\pm5\,{\rm km\,s}^{-1} of the B star then implies an inclination angle of the star's rotation axis to the line of sight of 24−10+6°24^{+6}_{-10}\degree. Assuming the Oblique Rotator Model, we derive the magnetic field strength of the B star's dipolar component (14−3+9 kG14^{+9}_{-3}\,{\rm kG}) and its obliquity (63±13°63\pm13\degree). Furthermore, we demonstrate that the calculated Alfvén radius (41−6+17 R∗41^{+17}_{-6}\,R_\ast) and Kepler radius (2.1−0.7+0.4 R∗2.1^{+0.4}_{-0.7}\,R_\ast) place HD~35502's central B star well within the regime of centrifugal magnetosphere-hosting stars.

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