Hydrodynamical evolution of merging carbon-oxygen white dwarfs: their pre-supernova structure and observational counterparts

TL;DR

This study uses hydrodynamical simulations to explore the pre-supernova structures of merging white dwarfs and assesses their potential to produce observable Type Ia supernovae through various explosion mechanisms.

Contribution

It provides new insights into the conditions under which merging CO white dwarfs can lead to different types of supernova explosions and predicts observable signatures of merger ejecta.

Findings

Helium-ignited violent mergers can produce SNe Ia with asymmetric ejecta.

Carbon-ignited mergers result in larger envelopes than some observed SNe Ia.

Chandrasekhar mass model does not produce SNe Ia for studied masses.

Abstract

We perform smoothed particle hydrodynamics (SPH) simulations for merging binary carbon-oxygen (CO) white dwarfs (WDs) with masses of $1.1$ and $1.0$ $M_\odot$, until the merger remnant reaches a dynamically steady state. Using these results, we assess whether the binary could induce a thermonuclear explosion, and whether the explosion could be observed as a type Ia supernova (SN Ia). We investigate three explosion mechanisms: a helium-ignition following the dynamical merger (`helium-ignited violent merger model'), a carbon-ignition (`carbon-ignited violent merger model'), and an explosion following the formation of the Chandrasekhar mass WD (`Chandrasekhar mass model'). An explosion of the helium-ignited violent merger model is possible, while we predict that the resulting SN ejecta are highly asymmetric since its companion star is fully intact at the time of the explosion. The carbon-ignited violent merger model can also lead to an explosion. However, the envelope of the exploding WD spreads out to $\sim 0.1R_\odot$; it is much larger than that inferred for SN 2011fe ($< 0.1R_\odot $) while much smaller than that for SN 2014J ($\sim 1R_\odot$). For the particular combination of the WD masses studied in this work, the Chandrasekhar mass model is not successful to lead to an SN Ia explosion. Besides these assessments, we investigate the evolution of unbound materials ejected through the merging process (`merger ejecta'), assuming a case where the SN Ia explosion is not triggered by the helium- or carbon-ignition during the merger. The merger ejecta interact with the surrounding interstellar medium, and form a shell. The shell has a bolometric luminosity of more than $2 \times 10^{35}$ ergs$^{-1}$ lasting for $\sim 2 \times 10^4$ yr. If this is the case, Milky Way should harbor about $10$ such shells at any given time.