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Evolution of the Progenitors of SNe 1993J and 2011dh Revealed through Late-time Radio and X-Ray Studies

Esha KunduThe Oskar Klein Centre, AlbaNova, SE-10691 Stockholm, SwedenPeter LundqvistDepartment of Astronomy, AlbaNova, Stockholm University, SE-10691 Stockholm, SwedenE. I. SorokinaSternberg Astronomical Institute, M.V. Lomonosov Moscow State University, Universitetski pr. 13, 119234 Moscow, RussiaPerez-Torres, M.A.Instituto de Astrofísica de Andalucía, Glorieta de las Astronomía, s/n, E-18008 Granada, SpainС. И. БлинниковInstitute for Theoretical and Experimental Physics (ITEP), Moscow, RussiaO''Connor, E.Department of Astronomy, AlbaNova, Stockholm University, SE-10691 Stockholm, SwedenM. ErgonThe Oskar Klein Centre, AlbaNova, SE-10691 Stockholm, SwedenP. ChandraDepartment of Astronomy, AlbaNova, Stockholm University, SE-10691 Stockholm, SwedenBarnali DasNational Centre for Radio Astronomy, Tata Institute of Fundamental Research, Pune University Campus, Pune-411007, India
2020en
ABI

Аннотация

We perform hydrodynamical simulations of the interaction between supernova (SN) ejecta and circumstellar medium (CSM) for SN 1993J and SN 2011dh, and calculate the radio and X-ray emissions expected from the shocked gas at late epochs (t). Considering the ejecta structure from multi-group radiation hydrodynamics simulation, we find that the observed rapid drop in radio and X-ray light curves of SN 1993J at t > 3000 days may be due to a change in the mass-loss rate ((M)over dot) similar to 6500 yr prior to the explosion of the SN. The exact epoch scales inversely with the assumed wind velocity of nu(w) = 10 km s(-1). The progenitor of this SN very likely belonged to a binary system, where, during its evolution, the primary had transferred material to the secondary. It is argued in this paper that the change in (M)over dot can happen because of a change in the mass accretion efficiency (eta) of the companion star. It is possible that before similar to 6500. (nu(w)/10 km s(-1))(-1) yr prior to the explosion, eta was high, and thus the CSM was tenuous, which causes the late-time downturn in fluxes. In the case of SN. 2011dh, the late-time evolution is found to be consistent with a wind medium with (M)over dot/nu(w) = 4 x 10(-6) M-circle dot yr(-1)/10 km s(-1). It is difficult from our analysis to predict whether the progenitor of this SN had a binary companion; however, if future observations show a similar decrease in radio and X-ray fluxes, then this would give strong support to a scenario where both SNe had undergone a similar kind of binary evolution before explosion.

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