Thermonuclear and electron-capture supernovae from stripped-envelope stars

Abstract

Context. When stripped from their hydrogen-rich envelopes, stars with initial masses between ∼7 and 11 M ⊙ may develop massive degenerate cores and collapse. Depending on the final structure and composition, the outcome can range from a thermonuclear explosion, to the formation of a neutron star in an electron-capture supernova (ECSN). It has recently been demonstrated that stars in this mass range may be more prone to disruption than previously thought: they may initiate explosive oxygen burning when their central densities are still below ρ c ≲ 10 9.6 g cm −3 . At the same time, their envelopes expand significantly, leading to the complete depletion of helium. This combination makes them interesting candidates for type Ia supernovae-which we call (C)ONe SNe Iaand this might have broader implications for the formation of neutron stars via ECSNe. Aims. To constrain the observational counterparts of (C)ONe SNe Ia and the key properties that enable them, it is crucial to constrain the evolution, composition, and precollapse structure of their progenitors, as well as the evolution of these quantities with cosmic time. In turn, this requires a detailed investigation of the final evolutionary stages preceding the collapse, and their sensitivity to input physics. Methods. Here, we modeled the evolution of 252 single, nonrotating helium stars covering the initial mass range 0.8-3.5 M ⊙ , with metallicities between Z = 10 −4 and 0.02, and overshoot efficiency factors from f OV = 0.0 to 0.016 across all convective boundaries. We used these models to constrain several properties of these stars, including their central densities, compositions, envelope masses, and radii at the onset explosive oxygen ignition, as well as the final outcome as a function of initial helium star mass. We further investigate the sensitivity of these properties to mass loss rate assumptions using an additional grid of 110 models with varying wind efficiencies.Results. We find that helium star models with masses between ∼1.8 and 2.7 M ⊙ are able to evolve onto 1.35-1.37 M ⊙ (C)ONe cores that initiate explosive burning at central densities between log 10 (ρ c /g cm −3 ) ∼ 9.3 and 9.6. We constrained the amount of residual carbon retained after core carbon burning as a function of initial conditions, and conclude that it plays a critical role in determining the final outcome: Chandrasekhar-mass degenerate cores that retain more than approximately 0.005 M ⊙ of carbon result in (C)ONe SNe Ia, while those with lower carbon mass become ECSNe. We find that (C)ONe SNe Ia are more likely to occur at high metallicities, whereas at low metallicities ECSNe dominate. However, both SN Ia and ECSN progenitors expand significantly during the final evolutionary stages, so that for the most extended models, a further binary interaction may occur. We constrain the relative ratio between (C)ONe SNe Ia and SNe Ib/c to be 0.17-0.30 at Z = 0.02, and 0.03-0.13 at Z ≤ 10 −3 . Conclusions. We conclude with a discussion on potential observational properties of (C)ONe SNe Ia ...

Stripped-envelope stars in different metallicity environments

“…This will result in different lifetimes and lead to significant differences in evolution, particularly in the lower-mass regime. Overshooting in low-mass helium stars will most significantly affect the locations of the boundaries in initial mass that lead to different final outcomes Chanlaridis et al (2022). This uncertainty is perhaps the largest in our population models, as it might imply that the minimum mass at which stars become core-collapse SNe is dependent on metallicity.…”

“…Therefore, we cannot assess the mini-mum mass at which stars produce SNe, and stars with masses smaller than our least massive core-collapse model that produce SNe cannot be analysed using the Müller et al (2016) model; which does not allow us to infer their explosion properties. To account for the number of successful SNe regardless of the results of our evolutionary calculations, we follow Chanlaridis et al (2022) and set the lower limit in the initial helium core mass for core collapse at 3 M , which they find to be metallicity independent if no core overshooting is included during helium burning. This is further justified since strippedenvelope stars of this mass are always below L tau min,WN , implying that their mass-loss rates are very small during core helium burning (although they may experience intense mass loss after core helium depletion; see Chanlaridis et al 2022).…”

“…To account for the number of successful SNe regardless of the results of our evolutionary calculations, we follow Chanlaridis et al (2022) and set the lower limit in the initial helium core mass for core collapse at 3 M , which they find to be metallicity independent if no core overshooting is included during helium burning. This is further justified since strippedenvelope stars of this mass are always below L tau min,WN , implying that their mass-loss rates are very small during core helium burning (although they may experience intense mass loss after core helium depletion; see Chanlaridis et al 2022). Consequently, the evolution of stripped-envelope stars near the boundary between core-collapse progenitors and white dwarfs or thermonuclear explosions is similar, independent of their initial chemical composition.…”

“…We further justify this assumption a posteriori arguing that this makes our estimates for the ejecta masses resemble the observed distribution more closely. For these stars, we assume that the NS gravitational mass is 1.22-1.3 M , and we assume that the minimum mass at which stars explode as SNe is 3 M , following Chanlaridis et al (2022).…”