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Featured researches published by M. Mariotti.


Monthly Notices of the Royal Astronomical Society | 2010

Constraining blazar distances with combined Fermi and TeV data: an empirical approach

E. Prandini; G. Bonnoli; L. Maraschi; M. Mariotti; F. Tavecchio

We discuss a method to constrain the distance of blazars with unknown redshift using combined observations in the GeV and TeV regimes. We assume that the Very High Energies (VHE) spectrum corrected for the absorption through the interaction with the extragalactic background light cannot be harder than the spectrum in the Fermi/Large Area Telescope (LAT) band. Starting from the observed VHE spectral data we derive the EBL-corrected spectra as a function of the redshift z and fit them with power laws to be compared with power-law fits to the LAT data. We apply the method to all TeV blazars detected by LAT with known distance and derive an empirical law describing the relation between the upper limits and the true redshifts that can be used to estimate the distance of unknown redshift blazars. Using different EBL models leads to systematic changes in the derived upper limits. Finally, we use this relation to infer the distance of the unknown redshift blazar PKS 1424+240.


arXiv: High Energy Astrophysical Phenomena | 2009

Discovery of very high energy gamma-rays from the flat spectrum radio quasar 3C 279 with the MAGIC telescope

M. Errando; R. Bock; D. Kranich; E. Lorenz; P. Majumdar; M. Mariotti; D. Mazin; E. Prandini; F. Tavecchio; M. Teshima; Robert Wagner

3C 279 is one of the best studied flat spectrum radio quasars located at a comparatively large redshift of z = 0.536. Observations in the very high energy band of such distant sources were impossible until recently due to the expected steep energy spectrum and the strong gamma‐ray attenuation by the extragalactic background light photon field, which conspire to make the source visible only with a low energy threshold. Here the detection of a significant gamma ray signal from 3C 279 at very high energies (E>75 GeV) during a flare in early 2006 is reported. Implications of its energy spectrum on the current understanding of the extragalactic background light and very high energy gamma‐ray emission mechanism models are discussed.


Proceedings of SPIE | 2008

Glass mirrors by cold slumping to cover 100 m2 of the MAGIC II Cherenkov telescope reflecting surface

Giovanni Pareschi; E. Giro; Robert Banham; S. Basso; D. Bastieri; R. Canestrari; G. Ceppatelli; Oberto Citterio; M. Doro; Mauro Ghigo; F. Marioni; M. Mariotti; M. Salvati; F. Sanvito; Dervis Vernani

We report on the production and implementation of 100 square panels 1 m x 1 m, based on the innovative approach of cold slumping of thin glass sheets. The more than 100 segments will cover around one half of the 240 m-square reflecting surface of the MAGIC II, a clone of the atmospheric Cherenkov telescope MAGIC I (with a single-dish 17 m diameter mirror) which is already operating since late 2003 at La Palma. The MAGIC II telescope will be completed by the end of 2008 and will operate in stereoscopic mode with MAGIC I. While the central part of the of the reflector is composed of by diamond milled Aluminum of 1m2 area panels (following a design similar to that already used for MAGIC I), the outer coronas will be made of sandwiched glass segments. The glass panel production foresees the following steps: a) a thin glass sheet (1-2mm) is elastically deformed so as to retain the shape imparted by a master with convex profile - the radius of curvature is large, the sheet can be pressed against the master using vacuum suction -; b) on the deformed glass sheet a honeycomb structure that provides the needed rigidity is glued ; c) then a second glass sheet is glued on the top in order to obtain a sandwich; d) after on the concave side a reflecting coating (Aluminum) and a thin protective coating (Quartz) are deposited. The typical weight of each panel is about 12 kg and its resolution is better than 1 mrad at a level of diameter that contains the 90% of the energy reflected by the mirror; the areal cost of glass panels is ~2 k per 1m2. The technology based on cold slumping is a good candidate for the production of the primary mirrors of the telescopes forming the Cherenkov Telescope Array (CTA), the future large TeV observatory currently being studied in Europe. Details on the realization of MAGIC II new mirrors based on cold slumping glass will be presented.


Proceedings of SPIE | 2008

Development of cold-slumping glass mirrors for imaging Cherenkov telescopes

Dervis Vernani; Robert Banham; Oberto Citterio; F. Sanvito; Giuseppe Valsecchi; Giovanni Pareschi; Mauro Ghigo; E. Giro; M. Doro; M. Mariotti

The development of lightweight glass mirrors manufactured via cold-slumping technique for Imaging Atmospheric Cherenkov Telescope is presented. The mirror elements have a sandwich-like structure where the reflecting and backing facets are composed by glass sheets with an interposed honeycomb aluminum core. The reflecting coating is deposited in high vacuum by means of physical vapor deposition and consists of aluminum with an additional protective layer of SiO2. The mirror fabrication and environmental qualification by accelerated ageing, thermal cycling and coating adhesion are presented together with the optical performances measured as angular resolution and reflectivity obtained on spherical, 1 squared meter mirror prototypes.


Proceedings of SPIE | 2013

Status of the technologies for the production of the Cherenkov telescope array (CTA) mirrors

Giovanni Pareschi; T. Armstrong; H. Baba; J. Bähr; A. Bonardi; G. Bonnoli; P. Brun; R. Canestrari; P. M. Chadwick; M. Chikawa; P. H. Carton; V. de Souza; J. Dipold; M. Doro; D. Durand; M. Dyrda; A. Förster; M. Garczarczyk; E. Giro; J. F. Glicenstein; Y. Hanabata; M. Hayashida; M. Hrabovski; C. Jeanney; M. Kagaya; Hideaki Katagiri; L. Lessio; D. Mandat; M. Mariotti; C. Medina

The Cherenkov Telescope Array (CTA) is the next generation very high-energy gamma-ray observatory, with at least 10 times higher sensitivity than current instruments. CTA will comprise several tens of Imaging Atmospheric Cherenkov Telescopes (IACTs) operated in array-mode and divided into three size classes: large, medium and small telescopes. The total reflective surface could be up to 10,000 m2 requiring unprecedented technological efforts. The properties of the reflector directly influence the telescope performance and thus constitute a fundamental ingredient to improve and maintain the sensitivity. The R&D status of lightweight, reliable and cost-effective mirror facets for the CTA telescope reflectors for the different classes of telescopes is reviewed in this paper.


nuclear science symposium and medical imaging conference | 1991

The CDF silicon vertex detector: an overview and test results

W. Carithers; R. Ely; C. Haber; S. Holland; S. Kleinfelder; T. Merrick; O. Schneider; W. C. Wester; M. Wong; H. Carter; B. Flaugher; B. Gonzales; M. Hrycyk; C. Nelson; S. Segler; T. Shaw; S. Tkaczyk; K. Turner; T.R. Wesson; B. A. Barnett; C. Boswell; J. Skarha; F. D. Snider; A. Spies; J. Tseng; S. Vejcik; D. Amidei; P. F. Derwent; M. Gold; J. A. J. Matthews

The final design and construction of a 46080 channel silicon microstrip vertex detector (SVX) for the Collider Detector Facility (CDF) experiment at the Tevatron collider are described. The system performance of the front end electronics employing a custom VLSI readout chip and the mechanical support and cooling systems for the 0.7 m/sup 2/ silicon detector are discussed. The authors present performance results from initial testing of individual components through final testing of the full system of detectors, readout, cooling, and data acquisition. Preliminary results from cosmic ray triggered data are also described.<<ETX>>


nuclear science symposium and medical imaging conference | 1991

Construction of the CDF silicon vertex detector

J. Skarha; B. Barnett; C. Boswell; F.D. Snider; A. Spies; J. Tseng; S. Vejcik; H. Carter; B. Flaugher; B. Gonzales; M. Hrycyk; C. Nelson; S. Segler; T. Shaw; S. Tkaczyk; K. Turner; T.R. Wesson; W. Carithers; R. Ely; C. Haber; S. Holland; Stuart Kleinfelder; T. Merrick; O. Schneider; W. C. Wester; M. Wong; D. Amidei; Paul F. Derwent; M. Gold; J. A. J. Matthews

Technical details and methods used in constructing the Collision Detector Facility (CDF) silicon vertex detector are presented. Attention is given to the foam-carbon fiber composite structure used to support the silicon microstrip detectors and the procedure for achievement of 5- mu m detector alignment. The construction of the beryllium barrel structure, which houses the detector assemblies, is also described. In addition, the 10- mu m placement accuracy of the detectors in the barrel structure is discussed, and the detector cooling and mounting systems are described. The construction of the CDF silicon vertex detector has been completed. The silicon strip detectors are located to an accuracy of 10 mu m and >98-5% of the silicon strips are fully functional.<<ETX>>


arXiv: Instrumentation and Methods for Astrophysics | 2016

INFN Camera demonstrator for the Cherenkov Telescope Array

G. Ambrosi; M. Ambrosio; C. Aramo; B. Bertucci; E. Bissaldi; M. Bitossi; S. Brasolin; G. Busetto; R. Carosi; S. Catalanotti; M. A. Ciocci; R. Consoletti; P. Da Vela; F. Dazzi; A. De Angelis; B. De Lotto; F. de Palma; R. Desiante; T. Di Girolamo; C. Di Giulio; M. Doro; D. D'Urso; G. Ferraro; F. Ferrarotto; F. Gargano; N. Giglietto; F. Giordano; G. Giraudo; M. Iacovacci; M. Ionica

The Cherenkov Telescope Array is a world-wide project for a new generation of ground-based Cherenkov telescopes of the Imaging class with the aim of exploring the highest energy region of the electromagnetic spectrum. With two planned arrays, one for each hemisphere, it will guarantee a good sky coverage in the energy range from a few tens of GeV to hundreds of TeV, with improved angular resolution and a sensitivity in the TeV energy region better by one order of magnitude than the currently operating arrays. In order to cover this wide energy range, three different telescope types are envisaged, with different mirror sizes and focal plane features. In particular, for the highest energies a possible design is a dual-mirror Schwarzschild-Couder optical scheme, with a compact focal plane. A silicon photomultiplier (SiPM) based camera is being proposed as a solution to match the dimensions of the pixel (angular size of ~ 0.17 degrees). INFN is developing a camera demonstrator made by 9 Photo Sensor Modules (PSMs, 64 pixels each, with total coverage 1/4 of the focal plane) equipped with FBK (Fondazione Bruno Kessler, Italy) Near UltraViolet High Fill factor SiPMs and Front-End Electronics (FEE) based on a Target 7 ASIC, a 16 channels fast sampler (up to 2GS/s) with deep buffer, self-trigger and on-demand digitization capabilities specifically developed for this purpose. The pixel dimensions of


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2017

Studies on a silicon-photomultiplier-based camera for Imaging Atmospheric Cherenkov Telescopes

C. Arcaro; D. Corti; A. De Angelis; M. Doro; C. Manea; M. Mariotti; R. Rando; Ignasi Reichardt; D. Tescaro

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Proceedings of the 26th International Conference on High Energy Physics | 2008

Operation of the CDF silicon vertex detector with colliding beams at Fermilab

F. Bedeschi; V. Bolognesi; S. Dell’Agnello; S. Galeotti; G. Grieco; M. Mariotti; A. Menzione; G. Punzi; F. Raffaelli; L. Ristori; F. Tartarelli; N. Turini; H. Wenzel; F. Zetti; M. W. Bailey; A. F. Garfinkel; M. Kruse; N. M. Shaw; W. Carithers; R. Ely; C. Haber; S. Holland; S. Kleinfelder; T. Merrick; O. Schneider; W. C. Wester; M. Wong; W. M. Yao; H. Carter; B. Flaugher

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A. De Angelis

Istituto Nazionale di Fisica Nucleare

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