Mass outflow from the symbiotic binary RS Oph during its 2021 outburst

TL;DR

This study analyzes the outflows from RS Oph during its 2021 outburst, revealing details about the structure, temperature, and velocity of the ejected material and streams, indicating a super-Eddington luminosity and high-velocity winds.

Contribution

First detailed spectroscopic and photometric analysis of RS Oph's 2021 outburst, characterizing outflow structure, temperature, and velocity changes during early eruption phases.

Findings

Effective temperature of pseudophotosphere: 15000 K.

Outflow velocities: approximately 3700 km/s.

Mass-loss rate exceeds 4-5 x 10^{-5} M_sun/yr.

Abstract

RS Oph is a symbiotic recurrent nova containing a massive white dwarf with heavy mass loss during activity. In August 2021, it underwent its seventh optical eruption since the end of the 19th century. The goal of this work is to analyse the structure of the outflows from the outbursting object. Based on broad-band $U$, $B$, $V$, $R_{\rm C}$, and $I_{\rm C}$ photometry and high-resolution H$\alpha$ spectroscopy obtained at days 11--15 of the outburst, we derived some parameters of the system's components and outflows and their changes during our observation. The effective temperature of a warm shell (pseudophotosphere) produced by the ejected material and occulting the hot component of the system was $T_{eff}=15000\pm1000$ K and the electron temperature of the nebula was $T_{e}=17000\pm3000$ K throughout the observations. The effective radius of the pseudophotosphere was $R_{ eff}=13.3\pm2.0$ R$_{\odot}$ and the emission measure of the nebula $EM=(9.50\pm0.59) $10$^{61}$ cm$^{-3}$ for day 11 and $R_{eff}=10.3\pm1.6$ R$_{\odot}$ and $EM=(5.60\pm0.35)$10$^{61}$ cm$^{-3}$ for day 15. To provide this emission measure, the bolometric luminosity of the outbursting object must exceed its Eddington limit. The mass-loss rate of the outbursting object through its wind is much greater than through its streams. The total rate (from wind + streams) was less than $(4-5)$ 10$^{-5}$ (d/1.6kpc)$^{3/2}$ M$_{\odot}$yr$^{-1}$. The streams are not highly collimated. Their mean outflowing velocities are $\upsilon_{b}=-3680\pm60$ km s$^{-1}$ for the approaching stream and $\upsilon_{r}=3520\pm50$ km s$^{-1}$ for the receding one if the orbit inclination is 50$^\circ$.