Multi-Wavelength Observations of Short-Duration Gamma-Ray Bursts: Recent Results

The number of detections as well as significantly deep non-detections of optical/NIR afterglows of Type I (short-duration population) Gamma-Ray Bursts (GRBs) has become large enough that statistically meaningful samples can now be constructed. I present within some recent results on the luminosity distribution of Type I GRB afterglows in comparison to those of Type II GRBs (collapsar population), the issue of the existence of jet breaks in Type I GRB afterglows, and the discovery of dark Type I GRBs.Comment: 10 pages, 3 figures, based on an invited talk, to appear in the proceedings of the Gamma-Ray Burst Symposium 2012- IAA-CSIC - Marbella, editors: Castro-Tirado, A. J., Gorosabel, J. and Park, I. H; v2: accepted, slightly expanded, minor changes after referee repor

Afterglows of Gamma-Ray Bursts: Short vs. Long GRBs

We compiled a large sample of Swift-era photometric data on long (Type II) and short (Type I) GRB afterglows. We compare the luminosity and energetics of the different samples to each other and to the afterglows of the pre-Swift era. Here, we present the first results of these studies.Comment: Conference Proceedings, "Gamma-Ray Bursts 2007", Santa Fe, shortened poster presentation; 4 pages, 3 figures; for full updated papers, go here to arXiv:0712.2186 and also here to arXiv:0804.195

Gamma-Ray Burst/Supernova Associations: Energy Partition and the Case of a Magnetar Central Engine

The favored progenitor model for Gamma-ray Bursts (GRBs) with Supernova (SN) association is the core collapse of massive stars. One possible outcome of such a collapse is a rapidly spinning, strongly magnetized neutron star ( magnetar ). We systematically analyze the multi-wavelength data of GRB/SN associations detected by several instruments before 2017 June. Twenty GRB/SN systems have been confirmed via direct spectroscopic evidence or a clear light curve bump, as well as some spectroscopic evidence resembling a GRB-SN. We derive/collect the basic physical parameters of the GRBs and the SNe, and look for correlations among these parameters. We find that the peak brightness, 56Ni mass, and explosion energy of SNe associated with GRBs are statistically higher than other Type Ib/c SNe. A statistically significant relation between the peak energy of GRBs and the peak brightness of their associated SNe is confirmed. No significant correlations are found between the GRB energies (either isotropic or beaming-corrected) and the supernova energy. We investigate the energy partition within these systems and find that the beaming-corrected GRB energy of most systems is smaller than the SN energy, with less than 30% of the total energy distributed in the relativistic jet. The total energy of the systems is typically smaller than the maximum available energy of a millisecond magnetar (2 × 1052 erg), especially if aspherical SN explosions are considered. The data are consistent with—although not proof of—the hypothesis that most, but not all, GRB/SN systems are powered by millisecond magnetars

The afterglows of swift-era short and long gamma-ray bursts

The phenomenon of Gamma-Ray Bursts (GRBs) has been a great mystery since their discovery four decades ago. Even today, over a decade into the "afterglow age", many questions are still unanswered. The canonical picture which satisfies most of the data is that GRBs are produced when a massive celestial body (either a post-main sequence star or merging compact objects) at cosmological distances collapses to a rapidly rotating compact object (a black hole, for example) which launches ultra-relativistic polar jets. The internal dissipation of energy within the jets leads to collimated non-thermal high-energy emission (the actual GRB), whereas shocks created from the interactions of the jets with the interstellar medium create a long-lasting fading afterglow. The collected physical processes describing this emission are called the standard fireball model. GRBs have been found to be the most luminous electromagnetic sources in the universe for short time periods. In this Thesis, I present my study of the afterglows of Type I (not associated with massive star formation, probably due to the merger of compact objects) and Type II (associated with massive star formation, the late optical emission includes a component due to a Type Ic supernova with high expansions speeds) GRBs, and compare them with each other, especially in terms of host-galaxy dust extinction and the luminosity distribution. To accomplish this, I have collected the largest sample of photometric afterglow data available worldwide, and from this, selected GRBs with data sufficient for a more detailed analysis.Das Phänomen der Gammastrahlenausbrüche (Gamma-Ray Bursts, GRBs) war auch lange nach ihrer Entdeckung vor über vier Jahrzehnten ein großes Rätsel. Selbst heute, über ein Jahrzehnt seit Beginn der "Ära der Nachglühen" (engl.: Afterglows) sind noch viele Fragen unbeantwortet. Das akzeptierte Bild, welches einen Großteil der Daten erklären kann ist, dass GRBs erzeugt werden, wenn ein massereicher Himmelskörper (entweder ein Stern, der die Hauptreihe verlassen hat, oder miteinander verschmelzende kompakte Objekte) in kosmologischer Distanz zu einem schnell rotierenden Objekt kollabiert (z.B. ein Schwarzes Loch), welches ultrarelativistische Materieauswürfe ("Jets") entlang der Polachse ausschleudert. Die interne Dissipation von Energie in dem Jet führt zu kollimierter nicht-thermischer Strahlung bei hohen Energien (der GRB), während Schockfronten, die bei der Interaktion des Jets mit der interstellaren Materie erzeugt werden, zu einem langlebigen abklingenden Afterglow führen. Die gesammelten physikalischen Prozesse, die die GRB-Emission beschreiben, werden als das Standard-Feuerballmodell bezeichnet. GRBs sind für kurze Zeiträume nachweislich die leuchtkräftigsten elektromagnetischen Quellen des Universums. In dieser Dissertation präsentiere ich meine Untersuchungen zu den Afterglows von Typ I (nicht mit massereicher Sternentstehung verknüpft, vermutlich durch die Verschmelzung kompakter Objekte ausgelöst) und Typ II (mit massereicher Sternentstehung verknüpft, die optische Emission zu späten Zeiten enthält eine Komponente, die einer Typ Ic Supernova mit hoher Ausbreitungsgeschwindigkeit zuzuschreiben ist) GRBs, und vergleiche sie miteinander, insbesondere, was die Extinktion durch Staub in den Muttergalaxien sowie die Leuchtkraftverteilung angeht. Um dies zu ermöglichen, habe ich das weltweit größte Archiv an photometrischen Daten zu Afterglows zusammengestellt und habe aus diesem GRBs selektiert, die ausreichende Daten für eine weitergehende Analyse boten

GRB 180325A: dust grain-size distribution and interstellar iron nanoparticles contribution

We modelled dust grain-size distributions for carbonaceous and silicates dust, as well as for free-flying iron nanoparticles in the environment of a $\gamma$-ray burst (GRB) afterglow, GRB 180325A. This GRB, at $z=2.2486$, has an unambiguous detection of the 2175 \r{A} extinction feature with $R_V=4.58$ and $A_V=1.58$. In addition to silicates, polycyclic aromatic hydrocarbons (PAH), and graphite, we used iron nanoparticles grain-size distributions for the first time to model the observed extinction curve of GRB 180325A. We fit the observed extinction for four model permutations, using 232 sets of silicates, graphite, carbon abundance in hydrocarbon molecules ($b_C$), and fraction of iron abundance in free-flying nanoparticles ($b_{\text{Fe}}$). These four different permutations were chosen to test iron nanoparticles significance and carbon abundance in hydrocarbons. Our results indicate that iron nanoparticles contribution is insignificant and there is a degeneracy of carbon abundances, with the range $(0.0 \leq b_C \leq 0.7)\times10^{-5}$ providing the best-fit to the observed extinction curve of GRB 180325A. We therefore favour the simplest model of silicates and polycyclic aromatic hydrocarbons. The silicates are dominant and contribute to the entire wavelength range of the GRB extinction curve while graphite contributes towards both the 2175 \r{A} bump and the UV extinction. The afterglow peak luminosity ($1.5\times10^{51}$ ergs/s) indicates dust destruction may have taken place. We conclude that further investigations into other potential contributors of extinction are warranted, particularly for steep UV extinction.Comment: 13 pages, 7 figures, accepted for publication in MNRA

Unique type of isolated cardiac valvular amyloidosis

BACKGROUND: Amyloid deposition in heart is a common occurrence in systemic amyloidosis. But localised valvular amyloid deposits are very uncommon. It was only in 1922 that the cases of valvular amyloidosis were reported. Then in 1980, Goffin et al reported another type of valvular amyloidosis, which he called the dystrophic valvular amyloidosis. We report a case of aortic valve amyloidosis which is different from the yet described valvular amyloidosis. CASE PRESENTATION: A 72 years old gentleman underwent urgent aortic valve replacement. Intraoperatively, a lesion was found attached to the inferior surface of his bicuspid aortic valve. Histopathology examination of the valve revealed that the lesion contained amyloid deposits, identified as AL amyloidosis. The serum amyloid A protein (SAP) scan was normal and showed no evidence of systemic amyloidosis. The ECG and echocardiogram were not consistent with cardiac amyloidosis. CONCLUSION: Two major types of cardiac amyloidosis have been described in literature: primary-myelomatous type (occurs with systemic amyolidosis), and senile type(s). Recently, a localised cardiac dystrophic valvular amyloidosis has been described. In all previously reported cases, there was a strong association of localised valvular amyloidosis with calcific deposits. Ours is a unique case which differs from the previously reported cases of localised valvular amyloidosis. In this case, the lesion was not associated with any scar tissue. Also there was no calcific deposit found. This may well be a yet unknown type of isolated valvular amyloidosis

Combined X-ray and optical analysis to probe the origin of the plateau emission in γ\gamma-ray bursts afterglows

A large fraction of gamma-ray bursts (GRBs) shows a plateau phase during the X-ray afterglow emission, whose physical origin is still debated. In this work we define a sample of 30 GRBs with simultaneous X-ray and optical data during and after the plateau phase. Through a time-resolved spectral analysis of the X-ray plateaus, we test the consistency of the unabsorbed optical fluxes with those obtained via X-ray-to-optical spectral extrapolation by assuming a synchrotron spectrum. Combining X-ray with optical data, we find that 63% (19/30) GRBs are compatible with a single synchrotron spectrum thus suggesting that both the optical and X-ray radiations are produced from a single emitting region. For these GRBs we derive the temporal evolution of the break frequency and we compare it with the expectations predicted by several models. For 11/30 GRBs the optical emission is above the predicted range of values extrapolated from the X-rays in at least one temporal bin of the light curve. These GRBs may not be explained with a single zone emission, indicating the necessity of invoking two cooperating processes in order to explain the broad band spectral behaviour during X-ray plateaus. We discuss our findings in the framework of different scenarios invoked to explain the plateau feature, including the energy injection from a spinning-down magnetar and the high latitude emission from a structured jet.Comment: submitted to A&