S. Rainò
Instituto Politécnico Nacional
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Astronomy and Astrophysics | 2012
P. Giommi; G. Polenta; A. Lähteenmäki; D. J. Thompson; Milvia Capalbi; S. Cutini; D. Gasparrini; J. González-Nuevo; J. León-Tavares; M. López-Caniego; M. N. Mazziotta; C. Monte; Matteo Perri; S. Rainò; G. Tosti; A. Tramacere; Francesco Verrecchia; Hugh D. Aller; M. F. Aller; E. Angelakis; D. Bastieri; A. Berdyugin; A. Bonaldi; L. Bonavera; C. Burigana; D. N. Burrows; S. Buson; E. Cavazzuti; Guido Chincarini; S. Colafrancesco
We present simultaneous Planck, Swift, Fermi, and ground-based data for 105 blazars belonging to three samples with flux limits in the soft X-ray, hard X-ray, and -ray bands, and we compare our results to those of a companion paper presenting simultaneous Planck and multi-frequency observations of 104 radio-loud northern active galactic nuclei selected at radio frequencies. While we confirm several previous results, our unique data set has allowed us to demonstrate that the selection method strongly influences the results, producing biases that cannot be ignored. Almost all the BL Lac objects have been detected by Fermi Large Area Telescope (LAT), whereas 30 to 40% of the flat-spectrum radio quasars (FSRQs) in the radio, soft X-ray, and hard X-ray selected samples are still below the -ray detection limit even after integrating 27 months of Fermi-LAT data. The radio to sub-millimetre spectral slope of blazars is quite flat, withh i 0 up to about 70 GHz, above which it steepens toh i 0:65. BL Lacs have significantly flatter spectra than FSRQs at higher frequencies. The distribution of the rest-frame synchrotron peak frequency ( S ) in the spectral energy distribution (SED) of FSRQs is the same in all the blazar samples withh S i = 10 13:1 0:1 Hz, while the mean inverse-Compton peak frequency,h IC i, ranges from 10 21 to 10 22 Hz. The distributions of S and of IC of BL Lacs are much broader and are shifted to higher energies than those of FSRQs; their shapes strongly depend on the selection method. The Compton dominance of blazars ranges from less than 0.2 to nearly 100, with only FSRQs reaching values larger than about 3. Its distribution is broad and depends strongly on the selection method, with -ray selected blazars peaking at 7 or more, and radio-selected blazars at values close to 1, thus implying that the common assumption that the blazar power budget is largely dominated by high-energy emission is a selection e ect. A comparison of our multi-frequency data with theoretical predictions shows that simple homogeneous SSC models cannot explain the simultaneous SEDs of most of the -ray detected blazars in all samples. The SED of the blazars that were not detected by Fermi-LAT may instead be consistent with SSC emission. Our data challenge the correlation between bolometric luminosity and S predicted by the blazar sequence.
Physical Review D | 2017
S. Abdollahi; M. Ackermann; M. Ajello; W. B. Atwood; L. Baldini; G. Barbiellini; D. Bastieri; R. Bellazzini; E. D. Bloom; R. Bonino; T. Brandt; J. Bregeon; P. Bruel; R. Buehler; R. A. Cameron; R. Caputo; M. Caragiulo; Daniel Castro; E. Cavazzuti; C. Cecchi; A. Chekhtman; S. Ciprini; J. Cohen-Tanugi; F. Costanza; A. Cuoco; S. Cutini; F. D'Ammando; F. de Palma; R. Desiante; S. W. Digel
We present a measurement of the cosmic-ray electron+positron spectrum between 7 GeV and 2 TeV performed with almost seven years of data collected with the Fermi Large Area Telescope. We find that the spectrum is well fit by a broken power law with a break energy at about 50 GeV. Above 50 GeV, the spectrum is well described by a single power law with a spectral index of 3.07 ± 0.02 (stat+syst) ± 0.04 (energy measurement). An exponential cutoff lower than 1.8 TeV is excluded at 95% CL. PACS numbers: 98.70.Sa, 96.50.sb, 95.85.Ry, 95.55.Vj
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.
1st Gamma-ray Large Area Space Telescope Symposium, GLAST, 5 February 2007 through 8 February 2007, Stanford, CA, United States | 2007
L. Baldini; G. Barbiellini; R. Bellazzini; J.R. Bogart; G. Bogaert; E. Bonamente; J. Bregeon; A. Brez; M. Brigida; A. W. Borgland; P. Bruel; G. A. Caliandro; C. Cecchi; F. P. Ceglie; E. Charles; A. Chekhtman; R. Claus; J. Cohen-Tanugi; E. Do Couto E Silva; R. Dubois; J. Conrad; D. Dumora; C. Favuzzi; Z. Fewtrell; W. B. Focke; S. Funk; P. Fusco; F. Gargano; S. Germani; B. Giebels
The calibration strategy of the GLAST Large Area Telescope (LAT) combines analysis of cosmic ray data with accelerator particle beams measurements. An advanced Monte Carlo simulation of the LAT, based on the Geant4 package, was set up to reproduce the LAT response to such radiation and to benchmark the event reconstruction and the background rejection strategy before launch and during operation. To validate the LAT simulation, a massive campaign of beam tests was performed between July and November 2006, in parallel with the LAT integration and test, on the LAT Calibration Unit. This is a detector built with spare flight modules and flight‐like readout electronics, which was exposed to a large variety of beams, representing the whole spectrum of the signal that will be detected by the LAT, using the CERN and the GSI accelerator facilities. Beams of photons (0 – 2.5 GeV), electrons (1 – 300 GeV), hadrons (π and p, a few GeV – 100 GeV) and ions (C; Xe, 1.5 GeV/n) were shot through the CU to measure the phys...
Nuclear Physics B - Proceedings Supplements | 2002
R. Bellazzini; L. Andreanelli; F. Angelini; S. Allegretti; R. Bagagli; L. Baldini; G. Barbiellini; F. Belli; A. Brez; M. Ceccanti; C. Cecchi; M. Ceschia; J.Cohen Tanugi; A. De Angelis; C. Favuzzi; F. Gargano; R. Giannitrapani; Giglietto; F. Giordano; M. Kuss; L. Latronico; F. Longo; F. Loparco; P. Lubrano; Marco Maria Massai; M. N. Mazziotta; M. Minuti; A. Morselli; N. Omodei; A. Paccagnella
Abstract The Gamma-ray Large Area Space Telescope (GLAST) is an international and multi-agency space mission that will study the cosmos in the energy range 20 MeV – 1 TeV. GLAST is an imaging gamma-ray telescope more much capable than instruments flown previously. The main instrument on board of the spacecraft is the Large Area Telescope (LAT), a high energy pair conversion telescope consisting of three major subsystems: a precision silicon tracker/converter, a CsI electromagnetic calorimeter and a segmented anti-coincidence system. In this article, we present the status of the construction and tests of the silicon tracker.
arXiv: High Energy Astrophysical Phenomena | 2017
E. Orlando; N. Giglietto; I. V. Moskalenko; S. Rainò; Andrew W. Strong
The first evidence of the gamma-ray emission from the quiescent Sun was found in the archival EGRET data that was later confirmed by Fermi-LAT observations with high significance. This emission is produced by Galactic cosmic rays (CRs) penetrating the inner heliosphere and inter- acting with the solar atmosphere and optical photons. The solar emission is characterized by two spatially and spectrally distinct components: (i) disk emission due to the CR cascades in the solar atmosphere, and (ii) spatially extended inverse Compton (IC) emission due to the CR electrons scattering off of solar photons. The intensity of both components associated with Galactic CRs anti-correlate with the level of the solar activity being the brightest during solar minimum. In this paper we discuss updates of the models of the IC component of the emission based on CR measurements made at different levels of solar activity, and we make predictions for e- ASTROGAM and AMEGO, proposed low-energy gamma-ray missions.
Proceedings of 7th International Fermi Symposium — PoS(IFS2017) | 2017
Elena Orlando; N. Giglietto; I. V. Moskalenko; S. Rainò; Andrew W. Strong
The Sun in its quiescent state is a known gamma-ray source. The solar emission is produced by Cosmic Rays (CRs) penetrating the inner heliosphere and interacting with the solar atmosphere and optical photons. It is characterized by two spatially and spectrally distinct components: (i) the disk emission due to hadronic CR cascades in the solar atmosphere, and (ii) the spatially extended inverse Compton (IC) emission due to CR electrons scattering on the solar photons. The intensity of both components anti-correlates with the solar activity being the brightest during solar minima. Observations of the two components at various solar activities allow to gain information on CRs very close to the Sun and on CR propagation in the heliosphere. After the first observation of its gamma-ray emission in the EGRET archival data, Fermi-LAT is separating the two emission components with higher significance, allowing to precisely study the CR in the inner heliosphere. We present updates of the models of the IC emission based on recent CR measurements for various levels of solar activity, and we make predictions for e-ASTROGAM and AMEGO, proposed MeV-GeV gamma-ray missions.
Archive | 2007
M. Brigida; C. Favuzzi; P. Fusco; F. Gargano; N. Giglietto; F. Giordano; F. Loparco; B. Marangelli; M. N. Mazziotta; N. Mirizzi; S. Rainò; P. Spinelli
A test sequence that involves functional verification and mechanical thermal properties of the GLAST LAT Tracker has been done, first on Engineering model prototypes, and it will continue on flight hardware. The results of vibration and thermal vacuum tests on the Engineering Model Tower of the GLAST LAT Tracker are presented. The performance expected for silicon detectors as a function of operating temperatures in the mission environment have also been investigated and described.
Prepared for 9th ICATPP Conference on Astroparticle, Particle, Space Physics, Detectors and Medical Physics Applications, Villa Erba, Como, Italy, 17-21 Oct 2005 | 2006
M. Brigida; A. Caliandro; C. Favuzzi; P. Fusco; F. Gargano; N. Giglietto; F. Giordano; F. Loparco; B. Marangelli; M. N. Mazziotta; N. Mirizzi; S. Rainò; P. Spinelli; U Bari; Bari Infn
The GLAST Large Area Telescope (LAT) is a high energy gamma ray observatory, mounted on a satellite that will be own in 2007. The LAT tracker consists of an array of tower modules, equipped with planes of silicon strip detectors (SSDs) interleaved with tungsten converter layers. Photon detection is based on the pair conversion process; silicon strip detectors will reconstruct tracks of electrons and positrons. The instrument is actually being assembled. The first towers have been already tested and integrated at Stanford Linear Accelerator Center (SLAC). An overview of the integration stages of the main components of the tracker and a description of the pre-launch tests will be given. Experimental results on the performance of the tracker towers will be also discussed.
Prepared for 9th ICATPP Conference on Astroparticle, Particle, Space Physics, Detectors and Medical Physics Applications, Villa Erba, Como, Italy, 17-21 Oct 2005 | 2006
M. Brigida; A. Caliandro; C. Favuzzi; P. Fusco; F. Gargano; N. Giglietto; F. Giordano; F. Loparco; B. Marangelli; M. N. Mazziotta; N. Mirizzi; S. Rainò; P. Spinelli; U Bari; Bari Infn
The GLAST Large Area Telescope (LAT) is a gamma-ray telescope consisting of a silicon micro-strip detector tracker followed by a segmented CsI calorimeter and covered by a segmented scintillator anticoincidence system that will search for {gamma}-rays in the 20 MeV-300 GeV energy range. The results of the environmental tests performed on the flight modules (towers) of the Tracker are presented. The aim of the environmental tests is to verify the performance of the silicon detectors in the expected mission environment. The tower modules are subjected to dynamic tests that simulate the launch environment and thermal vacuum test that reproduce the thermal gradients expected on orbit. The tower performance is continuously monitored during the whole test sequence. The environmental test activity, the results of the tests and the silicon tracker performance are presented.