TY - JOUR
T1 - Multidimensional simulations of the accretion-induced collapse of white dwarfs to neutron stars
AU - Dessart, L.
AU - Burrows, A.
AU - Ott, C.D.
AU - Livne, E.
AU - Yoon, S.C.
AU - Langer, N.
PY - 2006
Y1 - 2006
N2 - We present 2.5-dimensional radiation-hydrodynamics simulations of the accretion-induced collapse (AIC) of
white dwarfs, starting from two-dimensional rotational equilibrium configurations, thereby accounting consistently
for the effects of rotation prior to and after core collapse.We focus our study on a 1.46 and a 1.92M a model. Electron
capture leads to the collapse to nuclear densities of these cores a few tens of milliseconds after the start of the
simulations. The shock generated at bounce moves slowly, but steadily, outward. Within 50–100 ms, the stalled
shock breaks out of the white dwarf along the poles. The blast is followed by a neutrino-driven wind that develops
within the white dwarf, in a cone of 40 opening angle about the poles, with a mass loss rate of (5 8) ; 10 3 M s 1.
The ejecta have an entropy on the order of (20–50)kB baryon 1 and an electron fraction that is bimodal. By the end of
the simulations, at k600 ms after bounce, the explosion energy has reached (3 4) ; 1049 ergs and the mass has
reached a few times 10 3M .We estimate the asymptotic explosion energies to be lower than 1050 ergs, significantly
lower than those inferred for standard core collapse. The AIC of white dwarfs thus represents one instance where a
neutrino mechanism leads undoubtedly to a successful, albeit weak, explosion.We document in detail the numerous
effects of the fast rotation of the progenitors: the neutron stars are aspherical; the ‘‘ ’’ and ¯ e neutrino luminosities
are reduced compared to the e neutrino luminosity; the deleptonized region has a butterfly shape; the neutrino flux
and electron fraction depends strongly upon latitude (a la von Zeipel ); and a quasi-Keplerian 0.1–0.5 M accretion
disk is formed.
AB - We present 2.5-dimensional radiation-hydrodynamics simulations of the accretion-induced collapse (AIC) of
white dwarfs, starting from two-dimensional rotational equilibrium configurations, thereby accounting consistently
for the effects of rotation prior to and after core collapse.We focus our study on a 1.46 and a 1.92M a model. Electron
capture leads to the collapse to nuclear densities of these cores a few tens of milliseconds after the start of the
simulations. The shock generated at bounce moves slowly, but steadily, outward. Within 50–100 ms, the stalled
shock breaks out of the white dwarf along the poles. The blast is followed by a neutrino-driven wind that develops
within the white dwarf, in a cone of 40 opening angle about the poles, with a mass loss rate of (5 8) ; 10 3 M s 1.
The ejecta have an entropy on the order of (20–50)kB baryon 1 and an electron fraction that is bimodal. By the end of
the simulations, at k600 ms after bounce, the explosion energy has reached (3 4) ; 1049 ergs and the mass has
reached a few times 10 3M .We estimate the asymptotic explosion energies to be lower than 1050 ergs, significantly
lower than those inferred for standard core collapse. The AIC of white dwarfs thus represents one instance where a
neutrino mechanism leads undoubtedly to a successful, albeit weak, explosion.We document in detail the numerous
effects of the fast rotation of the progenitors: the neutron stars are aspherical; the ‘‘ ’’ and ¯ e neutrino luminosities
are reduced compared to the e neutrino luminosity; the deleptonized region has a butterfly shape; the neutrino flux
and electron fraction depends strongly upon latitude (a la von Zeipel ); and a quasi-Keplerian 0.1–0.5 M accretion
disk is formed.
M3 - Meeting Abstract
SN - 0004-637X
VL - 644
SP - 1063
EP - 1084
JO - Astrophysical Journal
JF - Astrophysical Journal
ER -