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Dive into the research topics where N. Giglietto is active.

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Featured researches published by N. Giglietto.


Astroparticle Physics | 2009

On possible interpretations of the high energy electron–positron spectrum measured by the Fermi Large Area Telescope

D. Grasso; Stefano Profumo; A. W. Strong; L. Baldini; R. Bellazzini; Elliott D. Bloom; J. Bregeon; G. Di Bernardo; Daniele Gaggero; N. Giglietto; T. Kamae; L. Latronico; F. Longo; M. N. Mazziotta; A. A. Moiseev; A. Morselli; J. F. Ormes; M. Pesce-Rollins; M. Pohl; M. Razzano; C. Sgrò; G. Spandre; T. E. Stephens

The Fermi-LAT experiment recently reported high precision measurements of the spectrum of cosmic-ray electrons-plus-positrons (CRE) between 20 GeV and 1 TeV. The spectrum shows no prominent spectral features, and is significantly harder than that inferred from several previous experiments. Here we discuss several interpretations of the Fermi results based either on a single large scale Galactic CRE component or by invoking additional electron–positron primary sources, e.g. nearby pulsars or particle dark matter annihilation. We show that while the reported Fermi-LAT data alone can be interpreted in terms of a single component scenario, when combined with other complementary experimental results, specifically the CRE spectrum measured by H.E.S.S. and especially the positron fraction reported by PAMELA between 1 and 100 GeV, that class of models fails to provide a consistent interpretation. Rather, we find that several combinations of parameters, involving both the pulsar and dark matter scenarios, allow a consistent description of those results. We also briefly discuss the possibility of discriminating between the pulsar and dark matter interpretations by looking for a possible anisotropy in the CRE flux.


Astronomy and Astrophysics | 2012

Simultaneous Planck, Swift, and Fermi observations of X-ray and γ-ray selected blazars

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.


The Astrophysical Journal | 2009

Prospects for GRB Science with the Fermi Large Area Telescope

David L. Band; Magnus Axelsson; L. Baldini; G. Barbiellini; Matthew G. Baring; D. Bastieri; M. Battelino; R. Bellazzini; E. Bissaldi; G. Bogaert; Jerry T. Bonnell; J. Chiang; J. Cohen-Tanugi; V. Connaughton; S. Cutini; F. de Palma; B. L. Dingus; E. Do Couto E Silva; G. Fishman; A. Galli; N. Gehrels; N. Giglietto; Jonathan Granot; S. Guiriec; R. Hughes; T. Kamae; Nu. Komin; F. Kuehn; M. Kuss; F. Longo

The Large Area Telescope (LAT) instrument on the Fermi mission will reveal the rich spectral and temporal gamma-ray burst (GRB) phenomena in the >100 MeV band. The synergy with Fermis Gamma-ray Burst Monitor detectors will link these observations to those in the well explored 10-1000 keV range; the addition of the >100 MeV band observations will resolve theoretical uncertainties about burst emission in both the prompt and afterglow phases. Trigger algorithms will be applied to the LAT data both onboard the spacecraft and on the ground. The sensitivity of these triggers will differ because of the available computing resources onboard and on the ground. Here we present the LATs burst detection methodologies and the instruments GRB capabilities.


Astroparticle Physics | 2012

A model-independent analysis of the Fermi Large Area Telescope gamma-ray data from the Milky Way dwarf galaxies and halo to constrain dark matter scenarios

M. N. Mazziotta; F. Loparco; F. de Palma; N. Giglietto

We implemented a novel technique to perform the collective spectral analysis of sets of multiple gamma-ray point sources using the data collected by the Large Area Telescope onboard the Fermi satellite. The energy spectra of the sources are reconstructed starting from the photon counts and without assuming any spectral model for both the sources and the background. In case of faint sources, upper limits on their fluxes are evaluated with a Bayesian approach. This analysis technique is very useful when several sources with similar spectral features are studied, such as sources of gamma rays from annihilation of dark matter particles. We present the results obtained by applying this analysis to a sample of dwarf spheroidal galaxies and to the Milky Way dark matter halo. The analysis of dwarf spheroidal galaxies yields upper limits on the product of the dark matter pair annihilation cross section and the relative velocity of annihilating particles that are well below those predicted by the canonical thermal relic scenario in a mass range from a few GeV to a few tens of GeV for some annihilation channels.


The Astrophysical Journal | 2017

Fermi-LAT Observations of High-energy Behind-the-limb Solar Flares

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

Preliminary results of the LAT Calibration Unit beam tests

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...


Proceedings of SPIE | 2016

Experimental verification of the HERD prototype at CERN SPS

Yongwei Dong; Zheng Quan; Junjing Wang; Ming Xu; Sebastiano Albergo; Filippo Ambroglini; G. Ambrosi; P. Azzarello; Yonglin Bai; Tianwei Bao; L. Baldini; R. Battiston; Paolo Bernardini; Zhen Chen; Raffaello D'Alessandro; M. Duranti; Domenico D'Urso; P. Fusco; Jiarui Gao; Xiaohui Gao; F. Gargano; N. Giglietto; Bingliang Hu; Ran Li; Yong Li; Xin Liu; F. Loparco; Junguang Lu; G. Marsella; Mario Nicola Mazziotta

The High Energy cosmic-Radiation Detection (HERD) facility is one of several space astronomy payloads of the cosmic light house program onboard Chinas Space Station, which is planned for operation starting around 2020 for about 10 years. Beam test with a HERD prototype, to verify the HERD specifications and the reading out method of wavelength shifting fiber and image intensified CCD, was taken at CERN SPS in November, 2015. The prototype is composed of an array of 5*5*10 LYSO crystals, which is 1/40th of the scale of HERD calorimeter. Experimental results on the performances of the calorimeter are discussed.


arXiv: High Energy Astrophysical Phenomena | 2017

Solar gamma rays and modulation of cosmic rays in the inner heliosphere

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

The quiet sun in gamma rays: modeling of the CR electrons in the Inner heliosphere

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.


Proceedings of 35th International Cosmic Ray Conference — PoS(ICRC2017) | 2017

A novel 3-D calorimeter for the high energy cosmic-radiation detection (HERD) facility onboard China's future space station

Yongwei Dong; Ming Xu; Zhigang Wang; Oscar Adriani; Sebastiano Albergo; G. Ambrosi; Philippe Azzarello; Yonglin Bai; Tianwei Bao; Paolo Bernardini; Bruna Bertucci; Xiaojun Bi; Massimo Bongi; Sergio Bottai; Weiwei Cao; Junying Chai; Zhen Chen; Raffaello D’Alessandro; Margherita Di Santo; M. Duranti; Kun Fang; H. Feng; Valerio Formato; P. Fusco; Jiarui Gao; F. Gargano; N. Giglietto; Peng Hu; Ran Li; Yong Li

The High Energy cosmic-Radiation Detection (HERD) facility is a flagship and landmark scientific experiment onboard Chinas Space Station, planned for operation starting around 2025 for about 10 years. The main instrument of HERD is a 3-D calorimeter (CALO) sensitive to incident gamma-rays and particles from five sides. With this design, the effective geometric factor of HERD is more than one order of magnitude larger than that of previous missions. CALO is made of about 7,500 cubes of LYSO crystals, corresponding to about 55 radiation lengths and 3 nuclear interaction lengths, respectively. The crystal signals are transferred by wavelength shifting fibers and read out by ISCMOS devices. Energy deposition in each crystal is then derived by summing up about 400 CMOS pixels and with necessary correction for light saturation. Both a low range ISCMOS and a high range one are required to meet the requirement of a large dynamic range of at least 10 million. The prototype of CALO has been tested successfully in November 2015 at CERN, which leads to an improved design of CALO.

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Dive into the N. Giglietto's collaboration.

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F. Gargano

Istituto Nazionale di Fisica Nucleare

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P. Fusco

Istituto Nazionale di Fisica Nucleare

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C. Favuzzi

Istituto Nazionale di Fisica Nucleare

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F. Loparco

Istituto Nazionale di Fisica Nucleare

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B. Marangelli

Instituto Politécnico Nacional

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A. Morselli

University of Rome Tor Vergata

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F. Giordano

Instituto Politécnico Nacional

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M. Brigida

Instituto Politécnico Nacional

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Francesco Saverio Cafagna

Istituto Nazionale di Fisica Nucleare

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