The $\gamma$-ray deposition histories of Calcium-rich supernovae

TL;DR

This study investigates the gamma-ray deposition histories of Calcium-rich supernovae to constrain their progenitor systems, finding that their properties suggest a continuum between Type Ia and stripped-envelope supernovae, with certain models fitting the observations.

Contribution

It provides the first gamma-ray escape time measurements for Ca-rich SNe and compares these with theoretical models to narrow down potential progenitor scenarios.

Findings

Gamma-ray escape time $t_0$ is approximately 35-65 days.

Ca-rich SNe form a continuum between Type Ia and SESNe in $t_0$-$M_{Ni56}$ space.

Models of low-mass white dwarf explosions and stripped star core-collapse match observed data.

Abstract

Calcium-rich supernovae (Ca-rich SNe) are faint, rapidly evolving transients whose progenitor system is yet to be determined. We derive the $\gamma$-ray deposition histories of five Ca-rich SNe from the literature in order to place constraints on possible progenitor systems. We find that the $ \gamma $-ray escape time, $ t_0 $, of the Ca-rich SNe sample is $\approx35$-$65 \,\rm{d}$, within the unoccupied region between Type Ia SNe and stripped envelope supernovae (SESNe). The $ t_0$-$M_\mathrm{Ni56} $ distribution of these SNe, where $M_\mathrm{Ni56}$ is the synthesised $^{56}$Ni mass in the explosion, creates a continuum between the Type Ia and SESNe $ t_0$-$M_\mathrm{Ni56} $ distribution, hinting at a possible connection between all the events. By comparing our results to models from the literature, we were able to determine that helium shell detonation models and core-collapse models of ultra-stripped stars are unlikely to explain Ca-rich SNe, since the gamma-ray escape time in these models is smaller than the observed values. Models that agree with the observed $ t_0$-$M_\mathrm{Ni56} $ distribution are explosions of low mass, $M\approx0.75$-$0.8\,M_\odot $, white dwarfs and core-collapse models of stripped stars with an ejecta mass of $M\approx1$-$3\,M_{\odot}$.