Forbidden Line Emission from Type Ia Supernova Remnants Containing Balmer-Dominated Shells

TL;DR

This study investigates forbidden line emissions in Type Ia supernova remnants with Balmer-dominated shells, revealing dense knots likely from circumstellar material and their ionization mechanisms, challenging previous expectations.

Contribution

It provides new insights into the dense knots in SNRs, their origins from circumstellar material, and the ionization processes responsible for forbidden line emissions.

Findings

Dense knots have densities >10^4 cm^-3.

Forbidden line emissions originate from photoionized oxygen in shock precursors.

Dense knots likely originate from circumstellar rather than interstellar medium.

Abstract

Balmer-dominated shells in supernova remnants (SNRs) are produced by collisionless shocks advancing into a partially neutral medium, and are most frequently associated with Type Ia supernovae. We have analyzed Hubble Space Telescope (HST) images and VLT/MUSE or AAT/WiFeS observations of five Type Ia SNRs containing Balmer-dominated shells in the LMC: 0509-67.5, 0519-69.0, N103B, DEM L71, and 0548-70.4. Contrary to expectations, we find bright forbidden line emission from small dense knots embedded in four of these SNRs. The electron densities in some knots are higher than 10$^4$ cm$^{-3}$. The size and density of these knots are not characteristic for interstellar medium (ISM) -- they most likely originate from a circumstellar medium (CSM) ejected by the SN progenitor. Physical property variations of dense knots in the SNRs appear to reflect an evolutionary effect. The recombination timescales for high densities are short, and HST images of N103B taken 3.5 yr apart already show brightness changes in some knots. VLT/MUSE observations detect [Fe XIV] line emission from reverse shocks into SN ejecta as well as forward shocks into the dense knots. Faint [O III] line emission is also detected from the Balmer shell in 0519-69.0, N103B, and DEM L71. We exclude the postshock origin because the [O III] line is narrow. For the preshock origin, we considered three possibilities: photoionization precursor, cosmic ray precursor, and neutral precursor. We conclude that the [O III] emission arises from oxygen that has been photoionized by [He II] $\lambda$304 photons and is then collisionally excited in a shock precursor heated mainly by cosmic rays.