Matteo Perri
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Featured researches published by Matteo Perri.
The Astrophysical Journal | 2013
Fiona A. Harrison; William W. Craig; Finn Erland Christensen; Charles J. Hailey; William W. Zhang; Steven E. Boggs; Daniel Stern; W. Rick Cook; Karl Forster; Paolo Giommi; Brian W. Grefenstette; Yunjin Kim; Takao Kitaguchi; Jason E. Koglin; Kristin K. Madsen; Peter H. Mao; Hiromasa Miyasaka; Kaya Mori; Matteo Perri; Michael J. Pivovaroff; S. Puccetti; V. Rana; Niels Jørgen Stenfeldt Westergaard; Jason Willis; Andreas Zoglauer; Hongjun An; Matteo Bachetti; Eric C. Bellm; Varun Bhalerao; Nicolai F. Brejnholt
The Nuclear Spectroscopic Telescope Array (NuSTAR) is a National Aeronautics and Space Administration (NASA) Small Explorer mission that carried the first focusing hard X-ray (6-79 keV) telescope into orbit. It was launched on a Pegasus rocket into a low-inclination Earth orbit on June 13, 2012, from Reagan Test Site, Kwajalein Atoll. NuSTAR will carry out a two-year primary science mission. The NuSTAR observatory is composed of the X-ray instrument and the spacecraft. The NuSTAR spacecraft is three-axis stabilized with a single articulating solar array based on Orbital Sciences Corporations LEOStar-2 design. The NuSTAR science instrument consists of two co-aligned grazing incidence optics focusing on to two shielded solid state CdZnTe pixel detectors. The instrument was launched in a compact, stowed configuration, and after launch, a 10-meter mast was deployed to achieve a focal length of 10.15 m. The NuSTAR instrument provides sub-arcminute imaging with excellent spectral resolution over a 12-arcminute field of view. The NuSTAR observatory will be operated out of the Mission Operations Center (MOC) at UC Berkeley. Most science targets will be viewed for a week or more. The science data will be transferred from the UC Berkeley MOC to a Science Operations Center (SOC) located at the California Institute of Technology (Caltech). In this paper, we will describe the mission architecture, the technical challenges during the development phase, and the post-launch activities.
Monthly Notices of the Royal Astronomical Society | 2009
P. A. Evans; A. P. Beardmore; Kim L. Page; J. P. Osborne; Paul T. O'Brien; R. Willingale; Rhaana L. C. Starling; D. N. Burrows; Olivier Godet; L. Vetere; Judith Lea Racusin; Mike R. Goad; K. Wiersema; L. Angelini; Milvia Capalbi; Guido Chincarini; Neil Gehrels; J. A. Kennea; Raffaella Margutti; D. C. Morris; C. J. Mountford; C. Pagani; Matteo Perri; Patrizia Romano; Nial R. Tanvir
We present a homogeneous X-ray analysis of all 318 gamma-ray bursts detected by the X-ray telescope (XRT) on the Swift satellite up to 2008 July 23; this represents the largest sample of X-ray GRB data published to date. In Sections 2-3, we detail the methods which the Swift-XRT team has developed to produce the enhanced positions, light curves, hardness ratios and spectra presented in this paper. Software using these methods continues to create such products for all new GRBs observed by the Swift-XRT. We also detail web-based tools allowing users to create these products for any object observed by the XRT, not just GRBs. In Sections 4-6, we present the results of our analysis of GRBs, including probability distribution functions of the temporal and spectral properties of the sample. We demonstrate evidence for a consistent underlying behaviour which can produce a range of light-curve morphologies, and attempt to interpret this behaviour in the framework of external forward shock emission. We find several difficulties, in particular that reconciliation of our data with the forward shock model requires energy injection to continue for days to weeks.
Science | 2005
David N. Burrows; Patrizia Romano; A. Falcone; Shiho Kobayashi; Bing Zhang; A. Moretti; Paul T. O'Brien; Michael R. Goad; Sergio Campana; Kim L. Page; Lorella Angelini; S. D. Barthelmy; Andrew P. Beardmore; Milvia Capalbi; Guido Chincarini; J. R. Cummings; G. Cusumano; Derek B. Fox; Paolo Giommi; J. E. Hill; J. A. Kennea; Hans A. Krimm; Vanessa Mangano; Francis E. Marshall; P. Meszaros; David C. Morris; John A. Nousek; Julian P. Osborne; Claudio Pagani; Matteo Perri
Gamma-ray burst (GRB) afterglows have provided important clues to the nature of these massive explosive events, providing direct information on the nearby environment and indirect information on the central engine that powers the burst. We report the discovery of two bright x-ray flares in GRB afterglows, including a giant flare comparable in total energy to the burst itself, each peaking minutes after the burst. These strong, rapid x-ray flares imply that the central engines of the bursts have long periods of activity, with strong internal shocks continuing for hundreds of seconds after the gamma-ray emission has ended.
Nature | 2005
Neil Gehrels; Craig L. Sarazin; Paul T. O'Brien; Bing Zhang; Loius M. Barbier; S. D. Barthelmy; Alexander J. Blustin; David N. Burrows; J. Cannizzo; J. R. Cummings; Michael R. Goad; Stephen T. Holland; C. P. Hurkett; J. A. Kennea; Andrew J. Levan; Craig B. Markwardt; K. O. Mason; P. Meszaros; M. J. Page; David M. Palmer; E. Rol; Takanori Sakamoto; R. Willingale; Lorella Angelini; Andrew P. Beardmore; Patricia T. Boyd; Alice A. Breeveld; Sergio Campana; Margaret Chester; Guido Chincarini
Gamma-ray bursts (GRBs) come in two classes: long (> 2 s), soft-spectrum bursts and short, hard events. Most progress has been made on understanding the long GRBs, which are typically observed at high redshift (z ≈ 1) and found in subluminous star-forming host galaxies. They are likely to be produced in core-collapse explosions of massive stars. In contrast, no short GRB had been accurately (< 10″) and rapidly (minutes) located. Here we report the detection of the X-ray afterglow from—and the localization of—the short burst GRB 050509B. Its position on the sky is near a luminous, non-star-forming elliptical galaxy at a redshift of 0.225, which is the location one would expect if the origin of this GRB is through the merger of neutron-star or black-hole binaries. The X-ray afterglow was weak and faded below the detection limit within a few hours; no optical afterglow was detected to stringent limits, explaining the past difficulty in localizing short GRBs.
The Astrophysical Journal | 2006
P. T. O’Brien; R. Willingale; Julian P. Osborne; Mike R. Goad; Kim L. Page; S. Vaughan; E. Rol; A. P. Beardmore; Olivier Godet; C. P. Hurkett; Alan A. Wells; Bing Zhang; Shiho Kobayashi; David N. Burrows; John A. Nousek; J. A. Kennea; A. Falcone; Dirk Grupe; Neil Gehrels; S. D. Barthelmy; John K. Cannizzo; J. R. Cummings; J. E. Hill; Hans A. Krimm; Guido Chincarini; Gianpiero Tagliaferri; Sergio Campana; A. Moretti; P. Giommi; Matteo Perri
We present observations of the early X-ray emission for a sample of 40 gamma-ray bursts (GRBs) obtained using the Swift satellite, for which the narrow-field instruments were pointed at the burst within 10 minutes of the trigger. Using data from the Burst Alert Telescope and the X-Ray Telescope, we show that the X-ray light curve can be well described by an exponential that relaxes into a power law, often with flares superimposed. The transition time between the exponential and the power law provides a physically defined timescale for the burst duration. In most bursts, the power law breaks to a shallower decay within the first hour, and a late emission hump is observed, which can last for many hours. In other GRBs the hump is weak or absent. The observed variety in the shape of the early X-ray light curve can be explained as a combination of three components: prompt emission from the central engine, afterglow, and the late hump. In this scenario, afterglow emission begins during or soon after the burst, and the observed shape of the X-ray light curve depends on the relative strengths of the emission due to the central engine and that of the afterglow. There is a strong correlation such that those GRBs with stronger afterglow components have brighter early optical emission. The late emission hump can have a total fluence equivalent to that of the prompt phase. GRBs with the strongest late humps have weak or no X-ray flares.
Nature | 2011
David N. Burrows; J. A. Kennea; G. Ghisellini; Vanessa Mangano; Bing Zhang; Kim L. Page; M. Eracleous; Patrizia Romano; T. Sakamoto; A. Falcone; J. P. Osborne; Sergio Campana; A. P. Beardmore; Alice A. Breeveld; M. M. Chester; R. Corbet; S. Covino; J. R. Cummings; Paolo D'Avanzo; Valerio D'Elia; P. Esposito; P. A. Evans; Dino Fugazza; Jonathan Mark Gelbord; Kazuo Hiroi; S. T. Holland; Kuiyun Huang; Myungshin Im; G. L. Israel; Young-Beom Jeon
Supermassive black holes have powerful gravitational fields with strong gradients that can destroy stars that get too close, producing a bright flare in ultraviolet and X-ray spectral regions from stellar debris that forms an accretion disk around the black hole. The aftermath of this process may have been seen several times over the past two decades in the form of sparsely sampled, slowly fading emission from distant galaxies, but the onset of the stellar disruption event has not hitherto been observed. Here we report observations of a bright X-ray flare from the extragalactic transient Swift J164449.3+573451. This source increased in brightness in the X-ray band by a factor of at least 10,000 since 1990 and by a factor of at least 100 since early 2010. We conclude that we have captured the onset of relativistic jet activity from a supermassive black hole. A companion paper comes to similar conclusions on the basis of radio observations. This event is probably due to the tidal disruption of a star falling into a supermassive black hole, but the detailed behaviour differs from current theoretical models of such events.D. N. Burrows , J. A. Kennea , G. Ghisellini , V. Mangano , B. Zhang , K. L. Page , M. Eracleous , P. Romano , T. Sakamoto , A. D. Falcone , J. P. Osborne , S. Campana , A. P. Beardmore , A. A. Breeveld , M. M. Chester , R. Corbet , S. Covino , J. R. Cummings , P. D’Avanzo , V. D’Elia , P. Esposito , P. A. Evans , D. Fugazza, J. M. Gelbord , K. Hiroi , S. T. Holland , K. Y. Huang , M. Im, G. Israel , Y. Jeon , Y.-B. Jeon , N. Kawai , H. A. Krimm , P. Mészáros , H. Negoro , N. Omodei , W.K. Park , J. S. Perkins , M. Sugizaki , H.-I. Sung , G. Tagliaferri , E. Troja , Y. Ueda, Y. Urata, R. Usui , L. A. Antonelli , S. D. Barthelmy , G. Cusumano , P. Giommi , F. E. Marshall , A. Melandri , M. Perri , J. L. Racusin , B. Sbarufatti , M. H. Siegel , & N. Gehrels 21
Nature | 2011
D. N. Burrows; J. A. Kennea; G. Ghisellini; Vanessa Mangano; Bin-Bin Zhang; Kim L. Page; M. Eracleous; Patrizia Romano; T. Sakamoto; A. Falcone; J. P. Osborne; S. Campana; A. P. Beardmore; Alice A. Breeveld; M. M. Chester; R. Corbet; S. Covino; J. R. Cummings; Paolo D'Avanzo; Valerio D'Elia; P. Esposito; P. A. Evans; Dino Fugazza; Jonathan Mark Gelbord; Kazuo Hiroi; S. T. Holland; Kuiyun Huang; Myungshin Im; G. L. Israel; Young-Beom Jeon
Supermassive black holes have powerful gravitational fields with strong gradients that can destroy stars that get too close, producing a bright flare in ultraviolet and X-ray spectral regions from stellar debris that forms an accretion disk around the black hole. The aftermath of this process may have been seen several times over the past two decades in the form of sparsely sampled, slowly fading emission from distant galaxies, but the onset of the stellar disruption event has not hitherto been observed. Here we report observations of a bright X-ray flare from the extragalactic transient Swift J164449.3+573451. This source increased in brightness in the X-ray band by a factor of at least 10,000 since 1990 and by a factor of at least 100 since early 2010. We conclude that we have captured the onset of relativistic jet activity from a supermassive black hole. A companion paper comes to similar conclusions on the basis of radio observations. This event is probably due to the tidal disruption of a star falling into a supermassive black hole, but the detailed behaviour differs from current theoretical models of such events.D. N. Burrows , J. A. Kennea , G. Ghisellini , V. Mangano , B. Zhang , K. L. Page , M. Eracleous , P. Romano , T. Sakamoto , A. D. Falcone , J. P. Osborne , S. Campana , A. P. Beardmore , A. A. Breeveld , M. M. Chester , R. Corbet , S. Covino , J. R. Cummings , P. D’Avanzo , V. D’Elia , P. Esposito , P. A. Evans , D. Fugazza, J. M. Gelbord , K. Hiroi , S. T. Holland , K. Y. Huang , M. Im, G. Israel , Y. Jeon , Y.-B. Jeon , N. Kawai , H. A. Krimm , P. Mészáros , H. Negoro , N. Omodei , W.K. Park , J. S. Perkins , M. Sugizaki , H.-I. Sung , G. Tagliaferri , E. Troja , Y. Ueda, Y. Urata, R. Usui , L. A. Antonelli , S. D. Barthelmy , G. Cusumano , P. Giommi , F. E. Marshall , A. Melandri , M. Perri , J. L. Racusin , B. Sbarufatti , M. H. Siegel , & N. Gehrels 21
Astronomy and Astrophysics | 2009
E. Massaro; P. Giommi; Cristina Leto; P. Marchegiani; A. Maselli; Matteo Perri; S. Piranomonte; S. Sclavi
We present a new catalogue of blazars based on multi-frequency surveys and on an extensive review of the literature. Blazars are classified as BL Lacertae objects, as flat spectrum radio quas ars or as blazars of uncertain/transitional type. Each object is identified by a root name, coded as BZB, BZQ and BZU for these three subclasses respectively, and by its coordinates. This catalogue i s being built as a tool useful for the identification of the extragala ctic sources that will be detected by present and future experiments for X and gamma-ray astronomy, like Swift, AGILE, Fermi-GLAST and Simbol-X. An electronic version is available from the ASI Science Data Center web site at http://www.asdc.asi.it/bzcat.
Nature | 2009
Nial R. Tanvir; Derek B. Fox; Andrew J. Levan; Edo Berger; K. Wiersema; J. P. U. Fynbo; A. Cucchiara; T. Krühler; N. Gehrels; J. S. Bloom; J. Greiner; P. A. Evans; E. Rol; F. E. Olivares; J. Hjorth; P. Jakobsson; J. Farihi; R. Willingale; Rhaana L. C. Starling; S. B. Cenko; Daniel A. Perley; Justyn R. Maund; J. Duke; R. A. M. J. Wijers; Andrew J. Adamson; A. Allan; M. N. Bremer; D. N. Burrows; A. J. Castro-Tirado; B. Cavanagh
Long-duration gamma-ray bursts (GRBs) are thought to result from the explosions of certain massive stars, and some are bright enough that they should be observable out to redshifts of z > 20 using current technology. Hitherto, the highest redshift measured for any object was z = 6.96, for a Lyman-alpha emitting galaxy. Here we report that GRB 090423 lies at a redshift of z approximately 8.2, implying that massive stars were being produced and dying as GRBs approximately 630 Myr after the Big Bang. The burst also pinpoints the location of its host galaxy.It is thought that the first generations of massive stars in the Universe were an important, and quite possibly dominant, source of the ultra-violet radiation that reionized the hydrogen gas in the intergalactic medium (IGM); a state in which it has remained to the present day. Measurements of cosmic microwave background anisotropies suggest that this phase-change largely took place in the redshift range z=10.8 +/- 1.4, while observations of quasars and Lyman-alpha galaxies have shown that the process was essentially completed by z=6. However, the detailed history of reionization, and characteristics of the stars and proto-galaxies that drove it, remain unknown. Further progress in understanding requires direct observations of the sources of ultra-violet radiation in the era of reionization, and mapping the evolution of the neutral hydrogen fraction through time. The detection of galaxies at such redshifts is highly challenging, due to their intrinsic faintness and high luminosity distance, whilst bright quasars appear to be rare beyond z~7. Here we report the discovery of a gamma-ray burst, GRB 090423, at redshift z=8.26 -0.08 +0.07. This is well beyond the redshift of the most distant spectroscopically confirmed galaxy (z=6.96) and quasar (z=6.43). It establishes that massive stars were being produced, and dying as GRBs, ~625 million years after the Big Bang. In addition, the accurate position of the burst pinpoints the location of the most distant galaxy known to date. Larger samples of GRBs beyond z~7 will constrain the evolving rate of star formation in the early universe, while rapid spectroscopy of their afterglows will allow direct exploration of the progress of reionization with cosmic time.Long-duration γ-ray bursts (GRBs) are thought to result from the explosions of certain massive stars, and some are bright enough that they should be observable out to redshifts of z > 20 using current technology. Hitherto, the highest redshift measured for any object was z = 6.96, for a Lyman-α emitting galaxy. Here we report that GRB 090423 lies at a redshift of z ≈ 8.2, implying that massive stars were being produced and dying as GRBs ∼630 Myr after the Big Bang. The burst also pinpoints the location of its host galaxy.
Nature | 2005
Gianpiero Tagliaferri; Mike R. Goad; Guido Chincarini; A. Moretti; Sergio Campana; David N. Burrows; Matteo Perri; S. D. Barthelmy; N. Gehrels; Hans A. Krimm; Takanori Sakamoto; Pawan Kumar; P. Meszaros; Shiho Kobayashi; Bing Zhang; L. Angelini; P. L. Banat; A. P. Beardmore; Milvia Capalbi; S. Covino; G. Cusumano; P. Giommi; Olivier Godet; J. E. Hill; J. A. Kennea; Vanessa Mangano; David C. Morris; John A. Nousek; Paul T. O'Brien; Julian P. Osborne
‘Long’ γ-ray bursts (GRBs) are commonly accepted to originate in the explosion of particularly massive stars, which give rise to highly relativistic jets. Inhomogeneities in the expanding flow result in internal shock waves that are believed to produce the γ-rays we see. As the jet travels further outward into the surrounding circumstellar medium, ‘external’ shocks create the afterglow emission seen in the X-ray, optical and radio bands. Here we report observations of the early phases of the X-ray emission of five GRBs. Their X-ray light curves are characterised by a surprisingly rapid fall-off for the first few hundred seconds, followed by a less rapid decline lasting several hours. This steep decline, together with detailed spectral properties of two particular bursts, shows that violent shock interactions take place in the early jet outflows.