Formation of circumstellar material during double-white-dwarf mergers and the early excess emissions in Type Ia supernovae

TL;DR

This study models the formation of circumstellar material during double white-dwarf mergers and demonstrates how the interaction between this material and supernova ejecta explains early excess emissions in certain Type Ia supernovae.

Contribution

It provides detailed hydrodynamical simulations linking double WD mergers to early supernova light-curve features, supporting the violent merger origin of 03fg/02es-like SNe Ia.

Findings

CSM density follows a specific power-law distribution at merger.

Simulated light curves match observed early flux excesses.

Supports violent merger scenario for certain SNe Ia.

Abstract

Early excess emission observed in Type Ia supernovae (SNe Ia) within $\sim1$ day of explosion provides a critical window into their progenitor systems. In the present study, we investigate formation of the circumstellar matter (CSM) in double white-dwarf (WD) mergers. We further study the interaction between the CSM and the SN ejecta. We first model the orbital evolution and super-Eddington mass transfer/ejection in the double WD systems. We then conduct hydrodynamical and light-curve (LC) simulations of the SN-CSM interaction, assuming a prompt SN Ia explosion in a context of the carbon-ignited violent merger (C-ignited VM). Our simulations show that at the moment of the merger, the binary system has the CSM distribution following $\rho_{\mathrm{CSM}}\simeq D(r/10^{14}\ \mathrm{cm})^{-3.5}\ (D\simeq 10^{-14}\text{--}10^{-13}\ \rm g\ cm^{-3})$. The simulated LCs reproduce the early flux excesses across optical to UV bands, as well as their color evolution, observed in the VM candidates, i.e., 03fg/02es-like SNe Ia. This supports that 03fg/02es-like objects originate from the VM explosions. We also discuss the case of the helium-ignited VM, which might be realized in some WD-WD mergers depending on the He content in the system. Focused here is the timing when the explosion is initiated, and we find that the explosion is initiated after the companion WD is, at least partially, tidally disrupted also in this case; we thus expect the formation of the CSM through the mass transfer phase also for the helium-ignited VM scenario.