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

¹ Institute of Astronomy and NAO, Bulgarian Academy of Sciences, Tsarigradsko Shausse 72, 1784 Sofia, Bulgaria
e-mail: mtomova@astro.bas.bg
² Department of Physics and Astronomy, Shumen University Episkop Konstantin Preslavski, 115 Universitetska Str., 9700 Shumen, Bulgaria
³ Institute of Astronomy of the Russian Academy of Sciences, 48 Pyatnitskaya Str., 119017 Moscow, Russia

Received: 8 January 2022
Accepted: 13 December 2022

Abstract

Context. 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.

Aims. The goal of this work is to analyse the structure of the outflows from the outbursting object.

Methods. Based on broad-band U, B, V, R_C, and I_C photometry and high-resolution Hα 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.

Results. The effective temperature of a warm shell (pseudophotosphere) produced by the ejected material and occulting the hot component of the system was T_eff = 15 000 ± 1000 K and the electron temperature of the nebula was T_e = 17 000 ± 3000 K throughout the observations. The effective radius of the pseudophotosphere was R_eff = 13.3 ± 2.0 R_⊙ and the emission measure of the nebula EM = (9.50 ± 0.59) × 10⁶¹ cm⁻³ for day 11 and R_eff = 10.3 ± 1.6 R_⊙ and EM = (5.60 ± 0.35) × 10⁶¹ 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/1.6 kpc)^3/2 M_⊙ yr^–1. The streams are not highly collimated. Their mean outflowing velocities are υ_b = −3680 ± 60 km s^–1 for the approaching stream and υ_r = 3520 ± 50 km s^–1 for the receding one if the orbit inclination is 50°.