While evolving toward their terminal white-dwarf cooling branches, some low-mass helium-core white dwarf stellar models experience a number of nuclear flashes. Just before the occurrence of each flash, stable hydrogen burning may be able to drive global pulsations that could shed some light on the internal structure of these stars through asteroseismology. In this work, we perform a pulsational stability analysis considering the effects of the ε mechanism in destabilizing gravity-mode periods for sequences of low-mass white dwarfs evolving through CNO flashes. We show that the ε mechanism due to stable hydrogen burning can excite low-order (ℓ=1,2) gravity modes with periods between ∼80 and 500 s, for stars with 0.2025≲M⋆/M⊙≲0.3630 located i...
Context. In the absence of a third dredge-up episode during the asymptotic giant-branch phase, white...
Context. In recent years, many low-mass (≲ 0.45 M⊙) white dwarf stars expected to harbor He cores ha...
The ε mechanism is a self-excitation mechanism of stellar pulsations which acts in regions where nuc...
Context. Before reaching their quiescent terminal white-dwarf cooling branch, some low-mass helium-c...
The detection of pulsations in white dwarfs with low mass offers the possibility of probing their i...
Context. Two of the possible channels for the formation of low-mass (M⋆ ≲ 0.5 M⊙) hydrogen-deficient...
Context. Low-mass (M⋆/M⊙ ≲ 0.45) white dwarfs, including the so-called extremely low-mass white dwar...
Context. The ∈ mechanism is a self-excitation mechanism of stellar pulsations that acts in regions i...
Context. In the absence of a third dredge-up episode during the asymptotic giant-branch ph...
We present a pulsational stability analysis on high-luminosity H-rich (DA) white dwarf models evolve...
Context. Many low-mass (M /M <∼ 0.45) and extremely low-mass (ELM, M /M <∼ 0.18−0.20) white-dwarf st...
We calculated a grid of evolutionary models for white dwarfs with helium cores (he-WDs) and investig...
The ϵ mechanism is a self-excitation mechanism of pulsations which acts on the regions where nuclear...
Context. In the absence of a third dredge-up episode during the asymptotic giant-branch phase, white...
Context. In recent years, many low-mass (≲ 0.45 M⊙) white dwarf stars expected to harbor He cores ha...
The ε mechanism is a self-excitation mechanism of stellar pulsations which acts in regions where nuc...
Context. Before reaching their quiescent terminal white-dwarf cooling branch, some low-mass helium-c...
The detection of pulsations in white dwarfs with low mass offers the possibility of probing their i...
Context. Two of the possible channels for the formation of low-mass (M⋆ ≲ 0.5 M⊙) hydrogen-deficient...
Context. Low-mass (M⋆/M⊙ ≲ 0.45) white dwarfs, including the so-called extremely low-mass white dwar...
Context. The ∈ mechanism is a self-excitation mechanism of stellar pulsations that acts in regions i...
Context. In the absence of a third dredge-up episode during the asymptotic giant-branch ph...
We present a pulsational stability analysis on high-luminosity H-rich (DA) white dwarf models evolve...
Context. Many low-mass (M /M <∼ 0.45) and extremely low-mass (ELM, M /M <∼ 0.18−0.20) white-dwarf st...
We calculated a grid of evolutionary models for white dwarfs with helium cores (he-WDs) and investig...
The ϵ mechanism is a self-excitation mechanism of pulsations which acts on the regions where nuclear...
Context. In the absence of a third dredge-up episode during the asymptotic giant-branch phase, white...
Context. In recent years, many low-mass (≲ 0.45 M⊙) white dwarf stars expected to harbor He cores ha...
The ε mechanism is a self-excitation mechanism of stellar pulsations which acts in regions where nuc...