11 research outputs found
Winds from Neutron Stars and Strong Type I X--Ray Bursts
A model for stationary, radiatively driven winds from X--ray bursting neutron
stars is presented. General relativistic hydrodynamical and radiative transfer
equations are integrated from the neutron star surface outwards, taking into
account for helium nuclear burning in the inner, dense, nearly hydrostatic
shells. Radiative processes include both bremsstrahlung emission--absorption
and Compton scattering; only the frequency--integrated transport is considered
here. It is shown that each solution is characterized by just one parameter:
the mass loss rate \Mdot, or, equivalently, the envelope mass \Menv. We
found that, owing to the effects of Comptonization, steady, supersonic winds
can exist only for \Mdot larger than a limiting value \Mdot_{min}
\approx\Mdot_{E}. Several models, covering about two decades in mass loss
rate, have been computed for given neutron star parameters. We discuss how the
sequence of our solutions with decreasing \Menv can be used to follow the
time evolution of a strong X--ray burst during the expansion/contraction phase
near to the luminosity maximum. The comparison between our numerical results
and the observational data of Haberl {\it et al.\/} (1987) for the bursts in
4U/MXB 1820-30 gives an estimate for both the spectral hardening factor and the
accretion rate in this source.Comment: 32 pages (10 postsript figures available on request), PlainTe
Accretion Rates in X--Ray Bursting Sources
We present estimates for the accretion rates in 13 X--ray bursting sources
which exhibit photospheric expansion, basing on theoretical models of
stationary, radiatively driven winds from neutron stars. The relatively high
values obtained, \Mdot_{acc}\magcir 10^{-9} \MS, are in accordance with
theoretical limits for unstable helium burning, and, at the same time, almost
never exceed the ``dynamical'' limit for stationary accretion, \sim 10
\Mdot_{Edd}. The only exceptions are 1820-30, already known to be a very
peculiar object, and 1608-522; there are indications, however, that in both
sources, accretion could be non--stationary.Comment: 21 pages, PlainTe
On the Nature of Photospheric Oscillations in Strong X--Ray Bursts
A possible sound origin for the photospheric oscillations in the X--ray
bursting sources 1608-522 and 2127+119 is suggested. It is shown that standing
sound waves in an expanding spherical envelope can have periods very close to
the observed ones. The quite large ratio, 10, of the periods in the two
sources is explained in terms of different wave regimes. The relevance of sound
oscillations to the observed QPO in type II bursts of the Rapid Burster is also
discussed.Comment: 14 pages, PlainTe
On the Amplitude of Burst Oscillations in 4U 1636-54: Evidence for Nuclear Powered Pulsars
We present a study of 581 Hz oscillations observed during a thermonuclear
X-ray burst from the low mass X-ray binary (LMXB) 4U 1636-54 with the Rossi
X-ray Timing Explorer (RXTE). We argue that the combination of large pulsed
amplitudes near burst onset and the spectral evidence for localized emission
during the rise strongly supports rotational modulation as the mechanism for
the oscillations. We discuss how theoretical interpretation of spin modulation
amplitudes, pulse profiles and pulse phase spectroscopy can provide constraints
on the masses and radii of neutron stars. We also discuss the implication of
these findings for the beat frequency models of kHz X-ray variability in LMXB.Comment: AASTEX Latex, 13 pages including 5 figures. Accepted for publication
in the Astrophysical Journal Letter
The Long Term Stability of Oscillations During Thermonuclear X-ray Bursts: Constraining the Binary X-ray Mass Function
We report on the long term stability of the millisecond oscillations observed
with the Rossi X-ray Timing Explorer (RXTE) during thermonuclear X-ray bursts
from the low mass X-ray binaries (LMXB) 4U 1728-34 and 4U 1636-53. We show that
bursts from 4U 1728-34 spanning more than 1.5 years have observed asymptotic
oscillation periods which are within 0.2 microsec. of each other, well within
the magnitude which could be produced by the orbital motion of the neutron star
in a typical LMXB. This stability implies a timescale to change the oscillation
period of > 23,000 years, suggesting a highly stable process such as stellar
rotation as the oscillation mechanism. We show that period offsets in three
distinct bursts from 4U 1636-53 can be plausibly interpreted as due to orbital
motion of the neutron star in this 3.8 hour binary system. We discuss the
constraints on the mass function which can in principle be derived using this
technique.Comment: 11 pages, 4 figures. AASTeX, to be published in the Astrophysical
Journal Letter
Mechanisms for High-frequency QPOs in Neutron Star and Black Hole Binaries
We explain the millisecond variability detected by Rossi X-ray Timing
Explorer (RXTE) in the X-ray emission from a number of low mass X-ray binary
systems (Sco X-1, 4U1728-34, 4U1608-522, 4U1636-536, 4U0614+091, 4U1735-44,
4U1820-30, GX5-1 and etc) in terms of dynamics of the centrifugal barrier, a
hot boundary region surrounding a neutron star. We demonstrate that this region
may experience the relaxation oscillations, and that the displacements of a gas
element both in radial and vertical directions occur at the same main
frequency, of order of the local Keplerian frequency. We show the importance of
the effect of a splitting of the main frequency produced by the Coriolis force
in a rotating disk for the interpretation of a spacing between the QPO peaks.
We estimate a magnitude of the splitting effect and present a simple formula
for the whole spectrum of the split frequencies. It is interesting that the
first three lowest-order overtones fall in the range of 200-1200 Hz and match
the kHz-QPO frequencies observed by RXTE. Similar phenomena should also occur
in Black Hole (BH) systems, but, since the QPO frequency is inversely
proportional to the mass of a compact object, the frequency of the
centrifugal-barrier oscillations in the BH systems should be a factor of 5-10
lower than that for the NS systems. The X-ray spectrum formed in this region is
a result of upscattering of a soft radiation (from a disk and a NS surface) off
relatively hot electrons in the boundary layer. We also briefly discuss some
alternative QPO models, including a possibility of acoustic oscillations in the
boundary layer, the proper stellar rotation, and g-mode disk oscillations.Comment: The paper is coming out in the Astrophysical Journal in the 1st of
May issue of 199