Open AccessThe formation of a helium white dwarf in a close binary system with diffusion
Author(s) -
Benvenuto O. G.,
De Vito M. A.
Publication year - 2004
Publication title -
monthly notices of the royal astronomical society
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 2.058
H-Index - 383
eISSN - 1365-2966
pISSN - 0035-8711
DOI - 10.1111/j.1365-2966.2004.07918.x
Subject(s) - physics , white dwarf , binary number , helium , astrophysics , binary system , orbit (dynamics) , mass transfer , binary star , diffusion , neutron star , stellar evolution , thermodynamics , atomic physics , stars , arithmetic , mathematics , engineering , aerospace engineering
ABSTRACT We study the evolution of a system composed of a 1.4‐M ⊙ neutron star and a normal, solar composition star of 2 M ⊙ in orbit with a period of 1 d. Calculations were performed employing the binary hydro code presented by Benvenuto & De Vito that handle the mass transfer rate in a fully implicit way. We then included the main standard physical ingredients together with the diffusion processes and a proper outer boundary condition. We have assumed fully non‐conservative mass transfer episodes. In order to study the interplay of mass loss episodes and diffusion we considered evolutionary sequences with and without diffusion in which all Roche lobe overflows (RLOFs) produce mass transfer. Another two sequences in which thermonuclearly driven RLOFs were not allowed to drive mass transfer have been computed with and without diffusion. As far as we are aware, this study represents the first binary evolution calculations in which diffusion is considered. The system produces a helium white dwarf of ∼0.21 M ⊙ in an orbit with a period of ∼4.3 d for the four cases. We find that mass transfer episodes induced by hydrogen thermonuclear flashes drive a tiny amount of mass transfer. As diffusion produces stronger flashes, the amount of hydrogen‐rich matter transferred is slightly higher than in the models without diffusion. We find that diffusion is the main agent in determining the evolutionary time‐scale of low‐mass white dwarfs even in the presence of mass transfer episodes.