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Asteroseismology of ultra-massive white dwarfs: New results from a multi-telescope survey

Uzundag, Murat

Abstract

Ultra-massive white dwarfs (UMWDs) are key astrophysical laboratories, potentially composing oxygen-neon (ONe) or carbon-oxygen (CO) cores, depending on the evolutionary history of their progenitor stars. These compact remnants provide a unique window into a wide range of physical phenomena, including the final stages of stellar mergers, the crystallization process in dense matter, and the progenitors of Type Ia supernovae. To explore their internal structure, we have initiated an ambitious photometric survey aimed at discovering new pulsating UMWDs and probing their interiors through asteroseismology. This campaign utilizes a coordinated multi-telescope strategy involving HiPERCAM on the Gran Telescopio Canarias, GMOS on Gemini, and the ARC 3.5-meter telescope at Apache Point Observatory. In this talk, I will review our recent findings and present a detailed asteroseismological analysis of pulsating ultra-massive white dwarfs.

Full text

Asteroseismology of ultra-massive white dwarfs: New results from a multi-telescope survey Murat Uzundag FWO Postdoctoral Fellow Francisco C. De Gerónimo, Mukremin Kilic, Alberto Rebassa-Mansergas, Alex Brown, Alejandro H. Corsico 9th TESS/16th Kepler Asteroseismic Science Consortium Workshop DAV pulsating white dwarfs General Properties ●Atmosphere: Hydrogen-rich (DA type) ● 10,400 ≲ Teff ≲ 13,000 K & log g∼7 to ∼9.5 ●Population: Most common class of pulsating white dwarfs → Over 500 confirmed members (Bognar & Sódor 2016; Córsico et al. 2019a; Vincent et al. 2020; Guidry et al. 2021; Romero et al. 2022, 2024) Ultra-massive pulsating white dwarfs Pulsation Characteristics ●Mode Type: Non-radial g-mode pulsations ●κ–γ mechanism (Dolez & Vauclair 1981; Winget et al. 1982) ●Convective-driving mechanism (Brickhill 1991; Goldreich & Wu 1999) ●Harmonic Degree: ℓ ≤ 2 ●Radial Order: 1 ≲ k ≲ 15 ●Period Range: 100 s ≲ Π ≲1500 s ●Amplitude Range: 0.01 to 0.3 mma Ultra-massive pulsating white dwarfs Star Name Mass(M☉) N. Modes Reference BPM37093 1.13 8 modes Metcalfe et al. 2004 GD518 1.24 ≤3 modes Hermes et al. 2013 SDSSJ0840 1.16 ≤3 modes Curd et al. 2017 WDJ2124 1.16 ≤3 modes Rowan et al. 2019 WDJ0049 1.31 ≤2 modes Kilic et al. 2023 WDJ0551 1.13 ≤2 modes Hollands et al. 2020 Ultra-massive white dwarfs Formation Channel Degeneracy ● Two main paths: ➤ Single-star evolution from intermediate-mass stars (Althaus et al. 2010) ➤ Double WD mergers (~40%, Jewett et al. 2024) ● Observables (mass, temperature, log g) often can’t distinguish between them. ● Understanding formation is critical to link UMWDs to broader phenomena (e.g. SNe Ia, magnetism, Q-branch pileup). Our Goal: Combine asteroseismology, high-quality observations, and improved evolutionary models to resolve these fundamental questions. Image: NASA/CXC/M Weiss Core composition of DAVs Core Composition of White Dwarfs by Mass ●Low-Mass WDs: MWD <0.5 M⊙→ Expected to harbor helium (He) cores (Norris 2004; Althaus et al. 2017) Core composition of DAVs Core Composition of White Dwarfs by Mass ●Typical Mass Range: Most white dwarfs have masses in the range: 0.5 ≲ M⊙ ≲ 1.05 → Expected to have carbon–oxygen (CO) cores (Althaus et al. 2010) Core composition of UMWDs Core Composition of White Dwarfs by Mass ●Ultra-Massive WDs: MWD ≳ 1.05 M⊙ → Core composition remains uncertain! ● Possible options: ○Carbon–oxygen (CO) (Althaus et al. 2022) ○Oxygen–neon (ONe) (Siess 2010; Althaus et al. 2021) ○Hybrid CO–Ne (Denissenkov 2013, De Gerónimo et al. 2024) Searching for pulsating ultra-massive white dwarfs Selection Criteria define based on Jiménez-Esteban et al. 2023 and Jewett et al. 2024 focusing on the ZZ Ceti instability strip. Teff ≥ 11 000 K 0.9 M⊙ 1.1 M⊙ 1.3 M⊙ ●Unique pulsating DAQ white dwarf (C+H atmosphere) ● Atmospheric composition & kinematics suggest a merger origin ●19 nights of time-series photometry. ● Displays large amplitude and frequency modulations ●12 independent modes detected → Periods: ~595–1000 sec In prep. Conclusions What is the internal composition of UMWDs? ● UMWDs may have ONe, CO, or hybrid CO-Ne cores ● Current models cannot decisively constrain the core composition ● Disentangling core makeup is key to understanding progenitors and fate (e.g., SNe Ia) Conclusions What is the internal composition of UMWDs? ● UMWDs may have ONe, CO, or hybrid CO-Ne cores ● Current models cannot decisively constrain the core composition ● Disentangling core makeup is key to understanding progenitors and fate (e.g., SNe Ia) Conclusions What is the internal composition of UMWDs? ● UMWDs may have ONe, CO, or hybrid CO-Ne cores ● Current models cannot decisively constrain the core composition ● Disentangling core makeup is key to understanding progenitors and fate (e.g., SNe Ia) Crystallization & mode trapping in pulsating ultramassive WDs ● Core crystallization (>85–99%) alters mode propagation ● Complex pulsation spectra (e.g. WD J0135+5722: 19 modes) ● Requires advanced seismic modeling with tailored CO & ONe grids Conclusions What is the internal composition of UMWDs? ● UMWDs may have ONe, CO, or hybrid CO-Ne cores ● Current models cannot decisively constrain the core composition ● Disentangling core makeup is key to understanding progenitors and fate (e.g., SNe Ia) Crystallization & mode trapping in pulsating ultramassive WDs ● Core crystallization (>85–99%) alters mode propagation - key feature in the distribution on period spacing. ● Complex pulsation spectra (e.g. WD J0135+5722: 19 modes) ● Requires advanced seismic modeling with tailored CO & ONe grids How do mergers influence pulsational properties? ● Some UMWDs likely originate from WD mergers ● Pulsators like WD J0551+4135 exhibit unstable, modulated modes ● We lack constraints on how mergers affect internal rotation & pulsation modes Conclusions What is the internal composition of UMWDs? ● UMWDs may have ONe, CO, or hybrid CO-Ne cores ● Current models cannot decisively constrain the core composition ● Disentangling core makeup is key to understanding progenitors and fate (e.g., SNe Ia) Crystallization & mode trapping in pulsating ultramassive WDs ● Core crystallization (>85–99%) alters mode propagation - key feature in the distribution on period spacing. ● Complex pulsation spectra (e.g. WD J0135+5722: 19 modes) ● Requires advanced seismic modeling with tailored CO & ONe grids How do mergers influence pulsational properties? ● Some UMWDs likely originate from WD mergers ● Pulsators like WD J0551+4135 exhibit unstable, modulated modes ● We lack constraints on how mergers affect internal rotation & pulsation modes Thank you!