J/A+A/704/L13       Internal magnetic field in HD 192575   (Vandersnickt+, 2025)

Asteroseismic detection of an internal magnetic field in the B0.5V pulsator HD 192575. Vandersnickt J., Vanlaer V., Vanrespaille M., Aerts C. <Astron. Astrophys. 704, L13 (2025)> =2025A&A...704L..13V 2025A&A...704L..13V (SIMBAD/NED BibCode)
ADC_Keywords: Stars, OB ; Stars, variable ; Magnetic fields ; Models ; Photometry Keywords: asteroseismology - stars: evolution - stars: interiors - stars: magnetic field - stars: oscillations - stars: rotation Abstract: Internal magnetic fields are an elusive component of stellar structure. However, they can play an important role in stellar structure and evolution models through efficient angular momentum transport and through their impact on internal mixing. We strive to explain the nine components of one frequency multiplet identified as a low-order quadrupole gravity mode detected in the light curve of the β Cep pulsator HD 192575 assembled by the Transiting Exoplanet Survey Satellite (TESS). We updated the frequencies of the quadrupole mode under investigation using a standard pre-whitening method applied to the 1951.46 d TESS light curve. This showed that an internal magnetic field is required to simultaneously explain all nine components. We implemented theoretical pulsation computations applicable to the low-order modes of a β Cep pulsator including the Coriolis force as well as a magnetic field that is misaligned with respect to the rotation axis. We applied the theoretical description to perform asteroseismic modelling of the amplitudes and frequencies in the multiplet of the quadrupole g-mode of this evolved β Cep star. Pulsation predictions based on the measured internal rotation frequency of the star cannot explain the observed nine-component frequency splittings of the quadrupole low-order gravity mode. By contrast, we show that the combined effect of the Coriolis force caused by the near-core rotation with a period of ∼5.3d and the Lorentz force due to an internal inclined magnetic field with a maximum strength of ∼24kG does provide a proper explanation of the nine multiplet frequencies and their relative amplitudes. Given HD 192575's stellar mass of about 12M, this work presents the detection and magneto-gravito-asteroseismic modelling of a stable internal magnetic field buried inside an evolved rotating supernova progenitor. Description: In the photometry Transiting Exoplanet Survey Satellite (TESS) photometry of the beta Cep pulsator HD 192575, the signatures of nonradial oscillation modes with both rotationally and magnetically induced frequency splitting have been detected. This discovery was enabled by the detection of very fine magnetic splitting in a rotationally split multiplet, which could only be detected thanks to the extensive TESS light curve and an appropriate Fourier analysis. From these split components, the star's rotational and magnetic properties can be constrained. Photometric signals from TESS's stitched light curve from cycles 2, 4, 5, and 6, analysed with an adapted version of the STAR SHADOW code of IJspeert et al. (2024, see https://github.com/LucIJspeert/star_shadow). We include all frequencies detected at a signal-to-noise ratio greater than 2. Objects: ----------------------------------------------------- RA (2000) DE Designation(s) ----------------------------------------------------- 20 10 56.91 +68 16 19.9 HD 192575 = TIC 402894425 ----------------------------------------------------- File Summary: -------------------------------------------------------------------------------- FileName Lrecl Records Explanations -------------------------------------------------------------------------------- ReadMe 80 . This file signals.dat 100 215 The photometric signals detected in the TESS light curve -------------------------------------------------------------------------------- Byte-by-byte Description of file: signals.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 12 F12.9 d-1 Freq Frequency 14- 23 E10.5 d-1 e_Freq Uncertainty on frequency 25- 44 F20.15 umag Ampl Photometric amplitude 46- 60 F15.13 umag e_Ampl Uncertainty on photometric amplitude 62- 73 F12.9 rad Phase Phase 75- 85 F11.9 rad e_Phase Uncertainty on phase 87-100 F14.9 --- SNR Signal-to-noise ratio -------------------------------------------------------------------------------- Acknowledgements: Mathijs Vanrespaille, mathijs.vanrespaille(at)kuleuven.be
(End) Patricia Vannier [CDS] 27-Nov-2025
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