Issue |
A&A
Volume 496, Number 2, March III 2009
|
|
---|---|---|
Page(s) | 475 - 494 | |
Section | Stellar structure and evolution | |
DOI | https://doi.org/10.1051/0004-6361/200810883 | |
Published online | 09 February 2009 |
Equation-of-state dependent features in shock-oscillation modulated neutrino and gravitational-wave signals from supernovae
Max-Planck-Institut für Astrophysik, Karl-Schwarzschild-Str.1, 85748 Garching, Germany e-mail: thj@mpa-garching.mpg.de
Received:
29
August
2008
Accepted:
28
January
2009
We present two-dimensional (axisymmetric)
neutrino-hydrodynamic simulations of the long-time
accretion phase of a 15 progenitor star after core
bounce and before the launch of a supernova explosion, when
non-radial hydrodynamic instabilities like convection occur
in different regions of the collapsing stellar core and
the standing accretion shock instability (SASI) leads
to large-amplitude oscillations of the stalled shock with a
period of tens of milliseconds. Our simulations were
performed with the Prometheus-Vertex code, which includes a
multi-flavor, energy-dependent neutrino transport scheme and employs
an effective relativistic gravitational potential. Testing
the influence of a stiff and a soft equation of state for hot
neutron star matter, we find that the non-radial mass motions
in the supernova core impose a time variability on the neutrino
and gravitational-wave signals with larger amplitudes, as well as
higher frequencies in the case of a more compact nascent neutron
star.
After the prompt shock-breakout burst of electron neutrinos, a
more compact accreting remnant produces higher neutrino luminosities
and higher mean neutrino energies. The observable neutrino emission
in the SASI sloshing direction exhibits a modulation of several
ten percent in the luminosities and around 1 MeV in the mean
energies with most power at typical SASI frequencies
between roughly 20 and 100 Hz. The modulation
is caused by quasi-periodic variations in the mass accretion rate
of the neutron star in each hemisphere. At times later
than ~50–100 ms after bounce, the gravitational-wave
amplitude is dominated by the growing low-frequency (
200 Hz)
signal associated with anisotropic neutrino emission.
A high-frequency wave signal results from nonradial
gas flows in the outer layers of the anisotropically accreting
neutron star. Right after bounce such nonradial mass motions occur
due to prompt post-shock convection in both considered cases
and contribute mostly to the early wave production around 100 Hz.
Later they are instigated by the SASI and by convective overturn
that vigorously stir the neutrino-heating and cooling layers,
and also by
convective activity developing below the neutrinosphere. The
gravitational-wave power then peaks at about 300–800 Hz, connected
to changes in the mass quadrupole moment on a timescale of milliseconds.
Distinctively higher spectral frequencies originate from the
more compact and more rapidly contracting neutron star. Both the
neutrino and gravitational-wave emission therefore carry information
that is characteristic of the properties of the nuclear equation of
state in the hot remnant. The detectability of the SASI effects
in the neutrino and gravitational-wave signals is briefly discussed.
Key words: stars: supernovae: general / hydrodynamics / neutrinos / gravitational waves / dense matter
© ESO, 2009
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