G. Vianello
Stanford University
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Featured researches published by G. Vianello.
The Astrophysical Journal | 2014
J. M. Burgess; Robert D. Preece; V. Connaughton; M. S. Briggs; Adam Goldstein; P. N. Bhat; J. Greiner; D. Gruber; Andreas von Kienlin; C. Kouveliotou; S. McGlynn; Charles A. Meegan; W. S. Paciesas; S. Xiong; Magnus Axelsson; Matthew G. Baring; C. D. Dermer; Shabnam Iyyani; D. Kocevski; N. Omodei; F. Ryde; G. Vianello
Time-resolved spectroscopy is performed on eight bright, long gamma-ray bursts (GRBs) dominated by single emission pulses that were observed with the Fermi Gamma-Ray Space Telescope. Fitting the prompt radiation of GRBs by empirical spectral forms such as the Band function leads to ambiguous conclusions about the physical model for the prompt radiation. Moreover, the Band function is often inadequate to fit the data. The GRB spectrum is therefore modeled with two emission components consisting of optically thin non-thermal synchrotron radiation from relativistic electrons and, when significant, thermal emission from a jet photosphere, which is represented by a blackbody spectrum. To produce an acceptable fit, the addition of a blackbody component is required in five out of the eight cases. We also find that the low-energy spectral index α is consistent with a synchrotron component with α = –0.81 ± 0.1. This value lies between the limiting values of α = –2/3 and α = –3/2 for electrons in the slow- and fast-cooling regimes, respectively, suggesting ongoing acceleration at the emission site. The blackbody component can be more significant when using a physical synchrotron model instead of the Band function, illustrating that the Band function does not serve as a good proxy for a non-thermal synchrotron emission component. The temperature and characteristic emission-region size of the blackbody component are found to, respectively, decrease and increase as power laws with time during the prompt phase. In addition, we find that the blackbody and non-thermal components have separate temporal behaviors as far as their respective flux and spectral evolutions.
Science | 2014
W. T. Vestrand; J. A. Wren; A. Panaitescu; P. R. Wozniak; H. Davis; D. M. Palmer; G. Vianello; N. Omodei; S. Xiong; M. S. Briggs; M. Elphick; W. S. Paciesas; W. Rosing
Bright Lights Gamma-ray bursts (GRBs), bright flashes of gamma-ray light, are thought to be associated with the collapse of massive stars. GRB 130427A was detected on 27 April 2013, and it had the longest gamma-ray duration and one of the largest isotropic energy releases observed to date (see the Perspective by Fynbo). Ackermann et al. (p. 42, published online 21 November) report data obtained with the Fermi Gamma-Ray Space Telescope, which reveal a high-energy spectral component that cannot be accounted for by the standard external shock synchrotron radiation model. Vestrand et al. (p. 38, published online 21 November) report the detection of an extremely bright flash of visible light and unexpected similarities between the variations of optical light and the highest-energy gamma rays that indicate a common origin. A detailed analysis of the first pulse of GRB 130427A by Preece et al. (p. 51, published online 21 November) suggests that existing models cannot explain all the observed spectral and temporal behaviors simultaneously. Maselli et al. (p. 48, published online 21 November) present x-ray and optical light curves of the bursts prompt emission as well as of its afterglow as recorded by the Swift satellite and a range of ground-based telescopes. Multiwavelength data from an extremely bright stellar explosion provide details of the physics of these violent events. The optical light generated simultaneously with x-rays and gamma rays during a gamma-ray burst (GRB) provides clues about the nature of the explosions that occur as massive stars collapse. We report on the bright optical flash and fading afterglow from powerful burst GRB 130427A. The optical and >100–megaelectron volt (MeV) gamma-ray flux show a close correlation during the first 7000 seconds, which is best explained by reverse shock emission cogenerated in the relativistic burst ejecta as it collides with surrounding material. At later times, optical observations show the emergence of emission generated by a forward shock traversing the circumburst environment. The link between optical afterglow and >100-MeV emission suggests that nearby early peaked afterglows will be the best candidates for studying gamma-ray emission at energies ranging from gigaelectron volts to teraelectron volts.
The Astrophysical Journal | 2013
C. Kouveliotou; Jonathan Granot; Judith Lea Racusin; Eric C. Bellm; G. Vianello; S. R. Oates; Christopher L. Fryer; S. E. Boggs; Finn Erland Christensen; William W. Craig; C. D. Dermer; Neil Gehrels; Charles J. Hailey; Fiona A. Harrison; Andrea Melandri; J. E. McEnery; Carole G. Mundell; D. Stern; G. Tagliaferri; William W. Zhang
GRB 130427A occurred in a relatively nearby galaxy; its prompt emission had the largest GRB fluence ever recorded. The afterglow of GRB 130427A was bright enough for the Nuclear Spectroscopic Telescope ARray (NuSTAR) to observe it in the 3-79 keV energy range long after its prompt emission (~1.5 and 5 days). This range, where afterglow observations were previously not possible, bridges an important spectral gap. Combined with Swift, Fermi, and ground-based optical data, NuSTAR observations unambiguously establish a single afterglow spectral component from optical to multi-GeV energies a day after the event, which is almost certainly synchrotron radiation. Such an origin of the late-time Fermi/Large Area Telescope >10 GeV photons requires revisions in our understanding of collisionless relativistic shock physics.
Astronomy and Astrophysics | 2009
G. Vianello; Diego Gotz; S. Mereghetti
We present a catalogue with the properties of all the bursts detected and localized by the IBIS instrument onboard the INTEGRAL satellite from November 2002 to September 2008. The sample is composed of 56 bursts, corresponding to a rate of ∼0.8 GRB per month. Thanks to the performances of the INTEGRAL Burst Alert System, 50% of the IBIS GRBs have detected afterglows, while 5% have redshift measurements. A spectral analysis of the 43 bursts in the INTEGRAL public archive has been carried out using the most recent software and calibration, deriving an updated, homogeneous and accurate catalogue with the spectral features of the sample. When possible a time-resolved spectral analysis also has been carried out. The GRBs in the sample have 20–200 keV fluences in the range 5 × 10 −8 –2.5 × 10 −4 erg cm −2 , and peak fluxes in the range 0.11–56 ph cm −2 s −1 . While most of the spectra are well fitted by a power law with photon index ∼1.6, we found that 9 bursts are better described by a cut-off power law, resulting in Ep values in the range 35–190 keV. Altough these results are comparable to those obtained with BAT onboard Swift, there is marginal evidence that ISGRI detects dimmer bursts than Swift/BAT. Using the revised spectral parameters and an updated sky exposure map that also takes into account the effects of the GRB trigger efficiency, we strengthen the evidence for a spatial correlation with the super galactic plane of the faint bursts with long spectral lag.
Monthly Notices of the Royal Astronomical Society | 2014
L. Nava; G. Vianello; N. Omodei; Gabriele Ghisellini; G. Ghirlanda; A. Celotti; F. Longo; R. Desiante; R. Barniol Duran
The physical origin of the > 0.1GeV emission detected from Gamma-Ray Bursts (GRBs) by the Fermi satellite has not yet been completely understood. In this work we consider the GeV light curves of ten GRBs with measured redshift detected by the Fermi-LAT. These light curves are characterised by a long-lived (& 10 2 seconds) emission, whose luminosity decays in time as a power-law. While the decay rate is similar for all GRBs (i.e. LLAT / t 1.2 ), the normalisation spans about two orders of magnitude in luminosity. However, after re-normalising the luminosities to the prompt energetics Eprompt the light curves overlap. We consider the scenario in which the temporally extended LAT emission is dominated by synchrotron radiation from electrons accelerated at the forward external shock. According to this model, at high-energies (i.e. above the typical synchrotron frequencies) a small dispersion of the Epromptnormalised light curves is expected. The fact that the LAT temporally extended emission follows this behaviour reinforces its interpretation in terms of afterglow radiation from external shocks. Assuming this scenario, we argue that the parameters ǫe and η (i.e., the fraction of shock-dissipated energy gained by the electrons, and the efficiency of the mechanism producing the prompt radiation, respectively) must be narrowly distributed.
The Astrophysical Journal | 2017
M. Ackermann; A. Allafort; L. Baldini; G. Barbiellini; D. Bastieri; R. Bellazzini; E. Bissaldi; R. Bonino; E. Bottacini; J. Bregeon; P. Bruel; R. Buehler; R. A. Cameron; M. Caragiulo; P. A. Caraveo; E. Cavazzuti; C. Cecchi; E. Charles; S. Ciprini; F. Costanza; S. Cutini; F. D'Ammando; F. de Palma; R. Desiante; S. W. Digel; N. Di Lalla; M. Di Mauro; L. Di Venere; P. S. Drell; C. Favuzzi
We report on the Fermi-LAT detection of high-energy emission from the behind-the-limb (BTL) solar flares that occurred on 2013 October 11, and 2014 January 6 and September 1. The Fermi-LAT observations are associated with flares from active regions originating behind both the eastern and western limbs, as determined by STEREO. All three flares are associated with very fast coronal mass ejections (CMEs) and strong solar energetic particle events. We present updated localizations of the >100 MeV photon emission, hard X-ray (HXR) and EUV images, and broadband spectra from 10 keV to 10 GeV, as well as microwave spectra. We also provide a comparison of the BTL flares detected by Fermi-LAT with three on-disk flares and present a study of some of the significant quantities of these flares as an attempt to better understand the acceleration mechanisms at work during these occulted flares. We interpret the HXR emission to be due to electron bremsstrahlung from a coronal thin-target loop top with the accelerated electron spectra steepening at semirelativistic energies. The >100 MeV gamma-rays are best described by a pion-decay model resulting from the interaction of protons (and other ions) in a thick-target photospheric source. The protons are believed to have been accelerated (to energies >10 GeV) in the CME environment and precipitate down to the photosphere from the downstream side of the CME shock and landed on the front side of the Sun, away from the original flare site and the HXR emission.
arXiv: High Energy Astrophysical Phenomena | 2016
G. Vianello; R. Lauer; Patrick Younk; L. Tibaldo; James Michael Burgess; Hugo Ayala Solares; J. Patrick Harding; C. Michelle Hui; N. Omodei; Hao Zhou
Astrophysical sources are now observed by many different instruments at different wavelengths, from radio to high-energy gamma-rays, with an unprecedented quality. Putting all these data together t ...
Astronomy and Astrophysics | 2007
G. Vianello; A. Tiengo; S. Mereghetti
Two new expanding X-ray rings were detected by the Swift XRT instrument during early follow-up observations of GRB 061019 and GRB 070129, increasing to 5 the number of dust scattering X-ray halos observed around GRBs. Although these two halos were particularly faint, a sensitive analysis can be performed that optimizes the method originally developed by Tiengo & Mereghetti (2006, A&A, 449, 203) to analyze dust scattering rings observed with XMM-Newton for the Swift satellite. In the case of GRB 061019, a known giant molecular cloud is identified as the one responsible for the scattering process, and its distance is accurately measured (d = 940 ± 40 pc) through the dynamics of the expanding ring. In the second case, XRT observed both the main peak of the prompt emission of GRB 070129 and the scattering halo, but the small number of detected halo photons prevents us from distinguish between different dust models.
The Astrophysical Journal | 2018
A. Albert; R. Alfaro; C. Alvarez; J. D. Álvarez; R. Arceo; J.C. Arteaga-Velázquez; D. Avila Rojas; H. A. Ayala Solares; N. Bautista-Elivar; A. Becerril; E. Belmont-Moreno; S. BenZvi; A. Bernal; Jürgen Braun; C. Brisbois; K. S. Caballero-Mora; T. Capistrán; Alberto Carraminana; S. Casanova; M. Castillo; U. Cotti; J. Cotzomi; S. Coutiño de León; C. De León; E. de la Fuente; R. Diaz Hernandez; B. L. Dingus; M. A. DuVernois; J. C. Diaz-Velez; R. W. Ellsworth
The High Altitude Water Cherenkov (HAWC) gamma-ray observatory is a wide field of view observatory sensitive to 500 GeV - 100 TeV gamma rays and cosmic rays. It can also perform diverse indirect searches for dark matter (DM) annihilation and decay. Among the most promising targets for the indirect detection of dark matter are dwarf spheroidal galaxies. These objects are expected to have few astrophysical sources of gamma rays but high dark matter content, making them ideal candidates for an indirect dark matter detection with gamma rays. Here we present individual limits on the annihilation cross section and decay lifetime for 15 dwarf spheroidal galaxies within the HAWC field-of-view, as well as their combined limit. These are the first limits on the annihilation cross section and decay lifetime using data collected with HAWC.
Monthly Notices of the Royal Astronomical Society | 2017
L. Nava; R. Desiante; F. Longo; A. Celotti; N. Omodei; G. Vianello; E. Bissaldi; Tsvi Piran
It is largely recognized that Gamma-Ray Burst (GRB) jets involve ultra-relativistic motion. However, the value of the Lorentz factor Gamma_0 is still not clear and only lower limits are known for most bursts. We suggest here a new method to obtain upper limits on Gamma_0. The early high-energy synchrotron afterglow flux depends strongly on Gamma_0. Upper limits on GeV emission therefore provide uppers limit on Gamma_0. Applying this method to 190 Fermi GRBs that have not been detected by the Fermi-LAT we place upper limits on the high-energy afterglow flux, and in turn on Gamma_0. For bursts at a typical redshift z=2, we find values of the order of 200 (and above) for a homogeneous density medium, and in the range 100-400 for a wind-like medium. These upper limits are consistent with (and are very close to) lower limits and direct estimates inferred using other methods, suggesting that the typical Lorentz factors of GRB jets are of order a few hundred.