1,724 research outputs found
Discovery of the Very Red Near-Infrared and Optical Afterglow of the Short-Duration GRB 070724A
[Abridged] We report the discovery of the near-infrared and optical afterglow
of the short-duration gamma-ray burst GRB070724A. The afterglow is detected in
i,J,H,K observations starting 2.3 hr after the burst with K=19.59+/-0.16 mag
and i=23.79+/-0.07 mag, but is absent in images obtained 1.3 years later.
Fading is also detected in the K-band between 2.8 and 3.7 hr at a 4-sigma
significance level. The optical/near-IR spectral index, beta_{O,NIR}=-2, is
much redder than expected in the standard afterglow model, pointing to either
significant dust extinction, A_{V,host}~2 mag, or a non-afterglow origin for
the near-IR emission. The case for extinction is supported by a shallow optical
to X-ray spectral index, consistent with the definition for ``dark bursts'',
and a normal near-IR to X-ray spectral index. Moreover, a comparison to the
optical discovery magnitudes of all short GRBs with optical afterglows
indicates that the near-IR counterpart of GRB070724A is one of the brightest to
date, while its observed optical emission is one of the faintest. In the
context of a non-afterglow origin, the near-IR emission may be dominated by a
mini-supernova, leading to an estimated ejected mass of M~10^-4 Msun and a
radioactive energy release efficiency of f~0.005 (for v~0.3c). However, the
mini-SN model predicts a spectral peak in the UV rather than near-IR,
suggesting that this is either not the correct interpretation or that the
mini-SN models need to be revised. Finally, the afterglow coincides with a star
forming galaxy at z=0.457, previously identified as the host based on its
coincidence with the X-ray afterglow position (~2" radius). Our discovery of
the optical/near-IR afterglow makes this association secure.Comment: Submitted to ApJ; 10 pages, 5 figures, 1 tabl
X-ray Brightening and UV Fading of Tidal Disruption Event ASASSN-15oi
We present late-time observations by Swift and XMM-Newton of the tidal
disruption event (TDE) ASASSN-15oi that reveal that the source brightened in
the X-rays by a factor of one year after its discovery, while it faded
in the UV/optical by a factor of . The XMM-Newton observations
measure a soft X-ray blackbody component with eV,
corresponding to radiation from several gravitational radii of a central black hole. The last Swift epoch taken almost 600 days after
discovery shows that the X-ray source has faded back to its levels during the
UV/optical peak. The timescale of the X-ray brightening suggests that the X-ray
emission could be coming from delayed accretion through a newly forming debris
disk, and that the prompt UV/optical emission is from the prior circularization
of the disk through stream-stream collisions. The lack of spectral evolution
during the X-ray brightening disfavors ionization breakout of a TDE "veiled" by
obscuring material. This is the first time a TDE has been shown to have a
delayed peak in soft X-rays relative to the UV/optical peak, which may be the
first clear signature of the real-time assembly of a nascent accretion disk,
and provides strong evidence for the origin of the UV/optical emission from
circularization, as opposed to reprocessed emission of accretion radiation.Comment: Accepted for publication in ApJ Letter
The physical origin of optical flares following GRB 110205A and the nature of the outflow
The optical emission of GRB 110205A is distinguished by two flares. In this
work we examine two possible scenarios for the optical afterglow emission. In
the first scenario, the first optical flare is the reverse shock emission of
the main outflow and the second one is powered by the prolonged activity of
central engine. We however find out that it is rather hard to interpret the
late ( day) afterglow data reasonably unless the GRB efficiency is very
high (). In the second scenario, the first optical flare is the low
energy prompt emission and the second one is the reverse shock of the initial
outflow. Within this scenario we can interpret the late afterglow emission
self-consistently. The reverse shock region may be weakly magnetized and the
decline of the second optical flare may be dominated by the high latitude
emission, for which strong polarization evolution accompanying the quick
decline is possible, as suggested by Fan et al. in 2008. Time-resolved
polarimetry by RINGO2-like polarimeters will test our prediction directly.Comment: Accepted for publication in RAA,8 pages, 2 figure
Establishing a Place at the Table: The Growing Influence of Non-Governmental Organizations in International Negotiations
Honors (Bachelor's)Political ScienceUniversity of Michiganhttp://deepblue.lib.umich.edu/bitstream/2027.42/91812/1/cenkobry.pd
The No-Reflow Phenomenon: Clinical and Angiographic Correlates
No-reflow occurring during PCI has been associated with poor outcomes. The objectives of this study were to evaluate the incidence of no-reflow as independent predictor of adverse events and to assess whether baseline pre-procedural treatment options may affect clinical outcomes. Data were derived from the ISACS-TC (NCT01218776) registry, a prospective survey of patients presenting with ACS over a 5-year period. Data were prospectively collected from 5997 patients undergoing PCI, identifying those with no-reflow, and analyzed their treatments and outcomes. No-reflow was defined as post-PCI TIMI flow grade 0-1, in the absence of post-procedural significant (≥25%) residual stenosis, abrupt vessel closure, dissection, perforation, thrombus of the original target lesion, or epicardial spasm. The outcome measure was in-hospital mortality. No-reflow was identified in 128 (2.1%) patients. On multivariate analysis, patients with no-reflow were more likely to be older (OR:1.20, 95%CI:1.01–1.44) and to be admitted with a diagnosis of ST-elevation myocardial infarction (OR:2.96, 95%CI:1.85–4.72). No-reflow was highly predictive of in-hospital mortality (17.2% vs. 4.2%, P<0.001) and remained a significant independent predictor of death after adjustment for demographic and clinical variables (OR:4.60,95%CI:2.61–8.09). Multivariable regression analysis was also performed to identify independent relationship between pre-procedural treatment regimens, angiographic characteristics and no-reflow phenomenon. Administration of pre-procedural unfractioned heparin, showed a strong inverse predictive value in terms of post-PCI TIMI flow and no-reflow phenomenon (OR: 0.65, 95%CI:0.43–0.99). Similarly, a 600-mg loading dose of clopidogrel showed a trend associated with a reduction in the likehood of no-reflow (OR:0.61,95%CI:0.37–1.00). Angiographic characteristics associated with no-reflow phenomenon were stenosis≥50% of the right coronary artery, presence of multivessel coronary disease and pre-procedural TIMI blood flow grade 0-1. In conclusion, no-reflow during PCI is a strong independent predictor of mortality. Pre-procedural administration of 600-mg loading dose of clopidogrel and/or unfractioned heparin is associated with reduced incidence of no-reflow
Gamma-Ray Bursts as a Threat to Life on Earth
Gamma-ray bursts (GRBs) are likely to have made a number of significant
impacts on the Earth during the last billion years. The gamma radiation from a
burst within a few kiloparsecs would quickly deplete much of the Earth's
protective ozone layer, allowing an increase in solar ultraviolet radiation
reaching the surface. This radiation is harmful to life, damaging DNA and
causing sunburn. In addition, NO2 produced in the atmosphere would cause a
decrease in visible sunlight reaching the surface and could cause global
cooling. Nitric acid rain could stress portions of the biosphere, but the
increased nitrate deposition could be helpful to land plants. We have used a
two-dimensional atmospheric model to investigate the effects on the Earth's
atmosphere of GRBs delivering a range of fluences, at various latitudes, at the
equinoxes and solstices, and at different times of day. We have estimated DNA
damage levels caused by increased solar UVB radiation, reduction in solar
visible light due to NO2 opacity, and deposition of nitrates through rainout of
HNO3. In this paper I give a concise review of this work and discuss current
and future work on extending and improving our estimates of the terrestrial
impact of a GRB.Comment: 8 pages; submitted as part of proceedings of the ESLAB Symposium on
'Cosmic Cataclysms and Life', November 2008; to be published in a special
issue of the International Journal of Astrobiolog
The Anticipated Supernova Associated with GRB090618
We use the cannonball model of gamma ray bursts (GRBs) and public data from
the first day of observations of GRB 090618 to predict its X-ray and optical
lightcurves until very late times, and, in particular, the emergence of a
photometric and spectroscopic signature of an SN akin to SN1998bw in its
optical afterglow with an anticipated peak brightness of magnitude 23 in the R
band around July 10, 2009, if extinction in the host galaxy can be neglected.Comment: 10 pages, 2 Figure
Observational implications of gamma-ray burst afterglow jet simulations and numerical light curve calculations
We discuss jet dynamics for narrow and wide gamma-ray burst (GRB) afterglow
jets and the observational implications of numerical simulations of
relativistic jets in two dimensions. We confirm earlier numerical results that
sideways expansion of relativistic jets during the bulk of the afterglow
emission phase is logarithmic in time and find that this also applies to narrow
jets with half opening angle of 0.05 radians. As a result, afterglow jets
remain highly nonspherical until after they have become nonrelativistic.
Although sideways expansion steepens the afterglow light curve after the jet
break, the jet edges becoming visible dominates the jet break, which means that
the jet break is sensitive to the observer angle even for narrow jets. Failure
to take the observer angle into account can lead to an overestimation of the
jet energy by up to a factor 4. This weakens the challenge posed to the
magneter energy limit by extreme events such as GRB090926A. Late time radio
calorimetry based on a spherical nonrelativistic outflow model remains relevant
when the observer is approximately on-axis and where differences of a few in
flux level between the model and the simulation are acceptable. However, this
does not imply sphericity of the outflow and therefore does not translate to
high observer angles relevant to orphan afterglows. For more accurate
calorimetry and in order to model significant late time features such as the
rise of the counterjet, detailed jet simulations remain indispensable.Comment: 7 Figures. Replaced with accepted version. Significantly expanded,
including additional discussion of time scale
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