157 research outputs found
Extended Emission from Short Gamma-Ray Bursts Detected with SPI-ACS/INTEGRAL
The short duration (T90 < 2 s) gamma-ray bursts (GRBs) detected in the
SPI-ACS experiment onboard the INTEGRAL observatory are investigated. Averaged
light curves have been constructed for various groups of events, including
short GRBs and unidentified short events. Extended emission has been found in
the averaged light curves of both short GRBs and unidentified short events. It
is shown that the fraction of the short GRBs in the total number of SPI-ACS
GRBs can range from 30 to 45%, which is considerably larger than has been
thought previously.Comment: 27 pages, 10 figure
Observations of giant outbursts from Cygnus X-1
We present interplanetary network localization, spectral, and time history
information for 7 episodes of exceptionally intense gamma-ray emission from
Cygnus X-1. The outbursts occurred between 1995 and 2003, with durations up to
\~28000 seconds. The observed 15 - 300 keV peak fluxes and fluences reached
3E-7 erg /cm2 s, and 8E-4 erg / cm2 respectively. By combining the
triangulations of these outbursts we derive an ~1700 square arcminute (3 sigma)
error ellipse which contains Cygnus X-1 and no other known high energy sources.
The outbursts reported here occurred both when Cyg X-1 was in the hard state as
well as in the soft one, and at various orbital phases. The spectral data
indicate that these outbursts display the same parameters as those of the
underlying hard and soft states, suggesting that they represent another
manifestation of these states.Comment: 27 pages, 9 figures. Revised version. Accepted for publication in the
Astrophysical Journal, tentatively scheduled for October 20, 2003 Part
Reactivation and Precise IPN Localization of the Soft Gamma Repeater SGR1900+14
In 1998 May, the soft gamma repeater SGR1900+14 emerged from several years of
quiescence and emitted a series of intense bursts, one with a time history
unlike any previously observed from this source. Triangulation using Ulysses,
BATSE, and KONUS data give a 1.6 square arcminute error box near the galactic
supernova remnant G42.8+0.6. This error box contains a quiescent soft X-ray
source which is probably a neutron star associated with the soft repeater.Comment: Accepted for publication in the Astrophysical Journal Letter
The Current Performance of the Third Interplanetary Network
The 3rd Interplanetary Network (IPN) has been operating since April 2001 with
two distant spacecraft, Ulysses and Mars Odyssey, and numerous near-Earth
spacecraft, such as BeppoSAX, Wind, and HETE-II. Mars Odyssey is presently in
orbit about Mars, and the network has detected approximately 30 cosmic, SGR,
and solar bursts. We discuss the results obtained to date and use them to
predict the future performance of the network.Comment: To appear in the proceedings of the conference on Gamma-Ray Bursts
and Afterglow Astronomy 2001: A Workshop Celebrating the First Year of the
HETE Mission, to be published by AI
Study of the Fast X-Ray Transient XTE J1901+014 Based on INTEGRAL, RXTE and ROSAT Data
The source XTE J1901+014 discovered by the RXTE observatory during an intense
outburst of hard radiation and classified as a fast X-ray transient is studied.
The source's spectral characteristics in the quiescent state have been
investigated for the first time both in the soft X-ray energy range (0.6-20
keV) based on ROSAT and RXTE data and in the hard energy range (>20 keV) based
on INTEGRAL data. A timing analysis of the source's properties has revealed
weak nonperiodic bursts of activity on time scales of several tens of seconds
and two intense (0.5-1 Crab) outbursts more than several hundred seconds
in duration. Certain assumptions about the nature of the object under study are
made.Comment: 19 pages, 7 figure
Electrodynamics of Magnetars: Implications for the Persistent X-ray Emission and Spindown of the Soft Gamma Repeaters and Anomalous X-ray Pulsars
(ABBREVIATED) We consider the structure of neutron star magnetospheres
threaded by large-scale electrical currents, and the effect of resonant Compton
scattering by the charge carriers (both electrons and ions) on the emergent
X-ray spectra and pulse profiles. In the magnetar model for the SGRs and AXPs,
these currents are maintained by magnetic stresses acting deep inside the star.
We construct self-similar, force-free equilibria of the current-carrying
magnetosphere with a power-law dependence of magnetic field on radius, B ~
r^(-2-p), and show that a large-scale twist softens the radial dependence to p
< 1. The spindown torque acting on the star is thereby increased in comparison
with a vacuum dipole. We comment on the strength of the surface magnetic field
in the SGR and AXP sources, and the implications of this model for the narrow
measured distribution of spin periods. A magnetosphere with a strong twist,
B_\phi/B_\theta = O(1) at the equator, has an optical depth ~ 1 to resonant
cyclotron scattering, independent of frequency (radius), surface magnetic field
strength, or charge/mass ratio of the scattering charge. When electrons and
ions supply the current, the stellar surface is also heated by the impacting
charges at a rate comparable to the observed X-ray output of the SGR and AXP
sources, if B_{dipole} ~ 10^{14} G. Redistribution of the emerging X-ray flux
at the ion and electron cyclotron resonances will significantly modify the
emerging pulse profile and, through the Doppler effect, generate a non-thermal
tail to the X-ray spectrum. The sudden change in the pulse profile of SGR
1900+14 after the 27 August 1998 giant flare is related to an enhanced optical
depth to electron cyclotron scattering, resulting from a sudden twist imparted
to the external magnetic field.Comment: 31 January 2002, minor revisions, new section 5.4.
Multi-Wavelength Studies of the Optically Dark Gamma-Ray Burst 001025A
We identify the fading X-ray afterglow of GRB 001025A from XMM-Newton
observations obtained 1.9-2.3 days, 2 years, and 2.5 years after the burst. The
non-detection of an optical counterpart to an upper limit of R=25.5, 1.20 days
after the burst, makes GRB 001025A a ``dark'' burst. Based on the X-ray
afterglow spectral properties of GRB 001025A, we argue that some bursts appear
optically dark because their afterglow is faint and their cooling frequency is
close to the X-ray band. This interpretation is applicable to several of the
few other dark bursts where the X-ray spectral index has been measured. The
X-ray afterglow flux of GRB 001025A is an order of magnitude lower than for
typical long-duration gamma-ray bursts. The spectrum of the X-ray afterglow can
be fitted with an absorbed synchrotron emission model, an absorbed thermal
plasma model, or a combination thereof. For the latter, an extrapolation to
optical wavelengths can be reconciled with the R-band upper limit on the
afterglow, without invoking any optical circumburst absorption, provided the
cooling frequency is close to the X-ray band. Alternatively, if the X-ray
afterglow is due to synchrotron emission only, seven magnitudes of extinction
in the observed R-band is required to meet the R-band upper limit, making GRB
001025A much more obscured than bursts with detected optical afterglows. Based
on the column density of X-ray absorbing circumburst matter, an SMC gas-to-dust
ratio is insufficient to produce this amount of extinction. The X-ray tail of
the prompt emission enters a steep temporal decay excluding that the tail of
the prompt emission is the onset of the afterglow (abridged).Comment: 32 pages, 8 figures, ApJ in pres
The Collimation and Energetics of the Brightest Swift Gamma-Ray Bursts
Long-duration gamma-ray bursts (GRBs) are widely believed to be
highly-collimated explosions (opening angle theta ~ 1-10 deg). As a result of
this beaming factor, the true energy release from a GRB is usually several
orders of magnitude smaller than the observed isotropic value. Measuring this
opening angle, typically inferred from an achromatic steepening in the
afterglow light curve (a "jet" break), has proven exceedingly difficult in the
Swift era. Here we undertake a study of five of the brightest (in terms of the
isotropic prompt gamma-ray energy release, E(gamma, iso)) GRBs in the Swift era
to search for jet breaks and hence constrain the collimation-corrected energy
release. We present multi-wavelength (radio through X-ray) observations of GRBs
050820A, 060418, and 080319B, and construct afterglow models to extract the
opening angle and beaming-corrected energy release for all three events.
Together with results from previous analyses of GRBs 050904 and 070125, we find
evidence for an achromatic jet break in all five events, strongly supporting
the canonical picture of GRBs as collimated explosions. The most natural
explanation for the lack of observed jet breaks from most Swift GRBs is
therefore selection effects. However, the opening angles for the events in our
sample are larger than would be expected if all GRBs had a canonical energy
release of ~ 10e51 erg. The total energy release we measure for those
"hyper-energetic" (E(total) >~ 10e52 erg) events in our sample is large enough
to start challenging models with a magnetar as the compact central remnant.Comment: Submitted to ApJ, comments welcom
Constraining GRB Emission Physics with Extensive Early-Time, Multiband Follow-up
Understanding the origin and diversity of emission processes responsible for
Gamma-ray Bursts (GRBs) remains a pressing challenge. While prompt and
contemporaneous panchromatic observations have the potential to test
predictions of the internal-external shock model, extensive multiband imaging
has been conducted for only a few GRBs. We present rich, early-time, multiband
datasets for two \swift\ events, GRB 110205A and GRB 110213A. The former shows
optical emission since the early stages of the prompt phase, followed by the
steep rising in flux up to ~1000s after the burst ( with
). We discuss this feature in the context of the
reverse-shock scenario and interpret the following single power-law decay as
being forward-shock dominated. Polarization measurements, obtained with the
RINGO2 instrument mounted on the Liverpool Telescope, also provide hints on the
nature of the emitting ejecta. The latter event, instead, displays a very
peculiar optical to near-infrared lightcurve, with two achromatic peaks. In
this case, while the first peak is probably due to the onset of the afterglow,
we interpret the second peak to be produced by newly injected material,
signifying a late-time activity of the central engine.Comment: 48 pages,11 figures, 24 tables. Accepted to The Astrophysical Journa
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