Search arXiv⌕ Search

arXiv · 2610.20262

HD 120678: a classical Be star with a tilting heartbeat disk

Abstract

Classical Oe/Be/Ae stars possess Keplerian circum-equatorial decretion disks which produce not just the eponymous emission lines but also the bewildering diversity of photometric variations on timescales above a few days. The variability is due to varying amounts and geometric distributions of the circumstellar gas. The ASAS-3 V-band light curve of HD 120678 between March 2005 and November 2008 resembled an inverse P Cygni profile, which may have been a one-off event. The peak-to-valley amplitude reached ~0.9 mag. Before and after this photometric event, the Balmer emission lines and their variability matched those of classical Be stars with an intermediate to low inclination angle. At the sharp minimum of the light curve, Gamen et al. (2012) observed shell-type profiles implying an edge-on (high-inclination) view. For the historical activity phases of gamma Cas and 59 Cyg, such a Be => Be-shell => Be sequence has been successfully interpreted as rotations of the disk plane. HD 120678 and a few other Be stars add a not previously recognized phenomenon to the plethora of Be-star variabilities, namely heartbeat light curves. Analogously to the distortion of heartbeat stars, the variability is due to heartbeat disks gravitationally tilted by an additional star as modeled by Marr et al. (2022) for Pleione. While the typical amplitudes of heartbeat stars are only a few 0.01 mag, heartbeat disks can explain the ten times larger amplitudes observed in Be stars.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Dietrich Baade, Jonathan Labadie-Bartz, Thomas Rivinius. 2026-10-14. HD 120678: a classical Be star with a tilting heartbeat disk. https://arxiv.org/abs/2610.20262

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Confidently Wrong: Why Ignoring Binaries Biases IMF Inference at Large Sample Sizes

The stellar initial mass function (IMF) high-mass slope $α$ is routinely measured by fitting single-star models to photometric samples that contain unresolved binaries. This practice introduces a systematic negative bias on $α$ that is constant with sample size $N$. Posterior credible intervals shrink as $1/\sqrt{N}$, so at sufficiently large $N$ the bias exceeds the full 95% credible-interval width and the true value falls outside the credible interval - a regime we call "confidently wrong." Building on earlier studies of the bias magnitude, we quantify the sample size at which this bias exceeds the statistical uncertainty. We quantify this bias using two idealized observation operators: mass-addition ($m_{\mathrm{obs}}=m_1+m_2$), a formal upper bound on unresolved-system mass overestimation, and luminosity-addition ($m_{\mathrm{obs}}=L^{-1}(L_1+L_2)$), an idealized lower-bias photometric case based on the ZAMS mass-luminosity relation. Across four astrophysical environments spanning $α=1.60$-$2.30$, we find: (1) mass-addition bias of 0.054-0.086 with crossover to confidently wrong at $N_{\mathrm{cross}}\sim5{,}000$-$10{,}000$; (2) luminosity-addition bias of 0.011-0.021 with $N_{\mathrm{cross}}\sim75{,}000$-$150{,}000$; and (3) a binary-aware mixture likelihood that marginalizes over the Moe & Di Stefano (2017) binary population model recovers the true slope in the synthetic tests presented here. Published single-star IMF slopes can therefore plausibly carry systematic errors of order 0.01-0.09 if unresolved binaries are not modeled, comparable to or exceeding reported uncertainties in some regimes. Since current and upcoming surveys (Gaia, JWST, Roman, LSST) will deliver large resolved-star samples, binary-aware inference is likely necessary to avoid binary-driven systematic bias in the large-$N$ single-star-fitting regime.

astro-ph.SR↗

Finite-Element Asteroseismology I: Two-Dimensional Adiabatic Oscillations of Rapidly Rotating N=3 Polytropes

We develop a finite-element formulation for linear adiabatic oscillations of axisymmetric uniformly rotating, centrifugally distorted, self-gravitating N=3 polytropes. Equilibrium models are constructed using self-consistent-field iteration and then remeshed on a surface-fitted oblate meridional domain. The quadratic eigenvalue problem describing oscillations for each azimuthal wavenumber $m$ is solved using a conforming two-domain mesh. The density-weighted displacement, $\boldsymbol{u}=ρ^{1/2}\boldsymbolξ$, is defined in the stellar interior, whereas the gravitational-potential perturbation $δΦ$ is solved both inside the star and in an exterior vacuum. The coupled displacement--potential problem is assembled and solved within FEniCSx as a polynomial eigenvalue problem. Without rotation, the axisymmetric modes agree closely with an independent one-dimensional calculation. For finite rotation rates, several clean axisymmetric $p$-mode branches of the spheroidal star successfully reproduce the frequencies tabulated by Reese (2006). The relative frequency differences induced by rotation are smaller than $3\times10^{-4}$ for the low-order mode branches up to $\sim 60$\% of the critical rotation rate. These tests validate both the centrifugally distorted equilibrium and the finite-element implementation. We develop a method to track eigenfunctions continuously as a function of rotation and decompose their angular structure to quantify rotational mode mixing and progressive coupling between different spherical harmonic components. This reveals continuous deformation of individual mode branches from nearly single-$\ell$ structures to strongly mixed states at rapid rotation. This work is intended as a step toward finite-element multidimensional asteroseismology frameworks for modelling realistic rotationally and tidally distorted stellar configurations.

astro-ph.SR↗

Probing the magnetic field of a coronal mass ejection with PSR J1022+1001

We investigate whether low-frequency pulsar observations can provide LoS magnetic field estimates and whether these are consistent with synthetic LoS signatures extracted from a three-dimensional CME reconstruction constrained by Solar Orbiter data. We analyze a CME occultation of the LoS to PSR J1022+1001 on 20 August 2021 at a projected heliocentric distance of 24.6 R_sun, observed simultaneously with LOFAR and NenuFAR. From LOFAR, we derive time-resolved dispersion measure (DM) and rotation measure (RM) and isolate the CME contributions using background estimates for interstellar, solar wind and ionospheric components. We then infer the density-weighted LoS-averaged magnetic field component _PSR from the ratio delta-RM/delta-DM. In parallel, we reconstruct the CME using a semi-empirical 3DCORE model fitted to Solar Orbiter in-situ magnetic field observations at 0.65 au. We sample the modeled magnetic field along the pulsar LoS using fixed spatial sampling points and compute synthetic LoS-averaged signatures _3D for different flux rope configurations. The derived _PSR increases from approximately -9 nT to a peak near 63 nT during the observed interval. Comparison with synthetic signatures shows that the polarity and temporal evolution of the LoS signal are strongly dependent on the flux rope configuration and only a South-West-North (SWN) configuration (confirmed by Solar Orbiter in-situ data) reproduces the observed sign and overall evolution, whereas alternative configurations are incompatible. The modeled amplitudes, however, are systematically larger than the pulsar-derived values by roughly a factor of five. We show that simultaneous low-frequency pulsar DM and RM measurements can provide LoS magnetic field estimates for a CME and can be used to test CME magnetic structure against data-constrained three-dimensional reconstructions.

astro-ph.SR↗