At the core of the AGILE scientific instrument, designed to operate on a satellite, there is the Gamma Ray Imaging Detector (GRID) consisting of a Silicon Tracker (ST), a Cesium Iodide Mini-Calorimeter and an Anti-Coincidence system of plastic scintillator bars. The ST needs an on-ground calibration with a gamma-ray beam to validate the simulation used to calculate the energy response function and the effective area versus the energy and the direction of the gamma rays. A tagged gamma-ray beam line was designed at the Beam Test Facility (BTF) of the INFN Laboratori Nazionali of Frascati (LNF), based on an electron beam generating gamma-rays through bremsstrahlung in a position-sensitive target. The gamma-ray energy is deduced by difference with the post-bremsstrahlung electron energy [1,2]. The electron energy is measured by a spectrometer consisting of a dipole magnet and an array of position sensitive silicon strip detectors, the Photon Tagging System (PTS). The use of the combined BTF-FTS system as tagged photon beam requires understanding the efficiency of gamma-ray tagging, the probability of fake tagging, the energy resolution andthe relation of the PTS hit position versus the gamma-ray energy. This paper describes this study comparing data taken during the AGILE calibration occurred in 2005 with simulation. (C) 2012 Elsevier B.V. All rights reserved.

Characterization of a tagged gamma-ray beam line at the DA Phi NE Beam Test Facility / Cattaneo PW; Argan A; Boffelli F; Bulgarelli A; Buonomo B; Chen AW; DAmmando F; Foggetta L; Froysland T; Fuschino F; Galli M; Gianotti F; Giuliani A; Longo F; Marisaldi M; Mazzitelli G; Pellizzoni A; Prest M; Pucella G; Quintieri L; Rappoldi A; Tavani M; Trifoglio M; Trois A; Valente P; Vallazza E; Vercellone S; Zambra A; Barbiellini G; Caraveo P; Cocco V; Costa E; De Paris G; Del Monte E; Di Cocco G; Donnarumma I; Evangelista Y; Feroci M; Ferrari A; Fiorini M; Labanti C; Lapshov I; Lazzarotto F; Lipari P; Mastropietro M; Mereghetti S; Morelli E; Moretti E; Morselli A; Pacciani L; Perotti F; Piano G; Picozza P; Pilia M; Porrovecchio G; Rapisarda M; Rubini A; Sabatini S; Soffitta P; Striani E; Vittorini V; Zanello D; Colafrancesco S; Giommi P; Pittori C; Santolamazza P; Verrecchia F; Salotti L. - In: NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH. SECTION A, ACCELERATORS, SPECTROMETERS, DETECTORS AND ASSOCIATED EQUIPMENT. - ISSN 0168-9002. - STAMPA. - 674:(2012), pp. 55-66. [10.1016/j.nima.2012.01.049]

Characterization of a tagged gamma-ray beam line at the DA Phi NE Beam Test Facility

D'AMMANDO, FILIPPO;
2012

Abstract

At the core of the AGILE scientific instrument, designed to operate on a satellite, there is the Gamma Ray Imaging Detector (GRID) consisting of a Silicon Tracker (ST), a Cesium Iodide Mini-Calorimeter and an Anti-Coincidence system of plastic scintillator bars. The ST needs an on-ground calibration with a gamma-ray beam to validate the simulation used to calculate the energy response function and the effective area versus the energy and the direction of the gamma rays. A tagged gamma-ray beam line was designed at the Beam Test Facility (BTF) of the INFN Laboratori Nazionali of Frascati (LNF), based on an electron beam generating gamma-rays through bremsstrahlung in a position-sensitive target. The gamma-ray energy is deduced by difference with the post-bremsstrahlung electron energy [1,2]. The electron energy is measured by a spectrometer consisting of a dipole magnet and an array of position sensitive silicon strip detectors, the Photon Tagging System (PTS). The use of the combined BTF-FTS system as tagged photon beam requires understanding the efficiency of gamma-ray tagging, the probability of fake tagging, the energy resolution andthe relation of the PTS hit position versus the gamma-ray energy. This paper describes this study comparing data taken during the AGILE calibration occurred in 2005 with simulation. (C) 2012 Elsevier B.V. All rights reserved.
2012
Characterization of a tagged gamma-ray beam line at the DA Phi NE Beam Test Facility / Cattaneo PW; Argan A; Boffelli F; Bulgarelli A; Buonomo B; Chen AW; DAmmando F; Foggetta L; Froysland T; Fuschino F; Galli M; Gianotti F; Giuliani A; Longo F; Marisaldi M; Mazzitelli G; Pellizzoni A; Prest M; Pucella G; Quintieri L; Rappoldi A; Tavani M; Trifoglio M; Trois A; Valente P; Vallazza E; Vercellone S; Zambra A; Barbiellini G; Caraveo P; Cocco V; Costa E; De Paris G; Del Monte E; Di Cocco G; Donnarumma I; Evangelista Y; Feroci M; Ferrari A; Fiorini M; Labanti C; Lapshov I; Lazzarotto F; Lipari P; Mastropietro M; Mereghetti S; Morelli E; Moretti E; Morselli A; Pacciani L; Perotti F; Piano G; Picozza P; Pilia M; Porrovecchio G; Rapisarda M; Rubini A; Sabatini S; Soffitta P; Striani E; Vittorini V; Zanello D; Colafrancesco S; Giommi P; Pittori C; Santolamazza P; Verrecchia F; Salotti L. - In: NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH. SECTION A, ACCELERATORS, SPECTROMETERS, DETECTORS AND ASSOCIATED EQUIPMENT. - ISSN 0168-9002. - STAMPA. - 674:(2012), pp. 55-66. [10.1016/j.nima.2012.01.049]
Cattaneo PW; Argan A; Boffelli F; Bulgarelli A; Buonomo B; Chen AW; DAmmando F; Foggetta L; Froysland T; Fuschino F; Galli M; Gianotti F; Giuliani A; Longo F; Marisaldi M; Mazzitelli G; Pellizzoni A; Prest M; Pucella G; Quintieri L; Rappoldi A; Tavani M; Trifoglio M; Trois A; Valente P; Vallazza E; Vercellone S; Zambra A; Barbiellini G; Caraveo P; Cocco V; Costa E; De Paris G; Del Monte E; Di Cocco G; Donnarumma I; Evangelista Y; Feroci M; Ferrari A; Fiorini M; Labanti C; Lapshov I; Lazzarotto F; Lipari P; Mastropietro M; Mereghetti S; Morelli E; Moretti E; Morselli A; Pacciani L; Perotti F; Piano G; Picozza P; Pilia M; Porrovecchio G; Rapisarda M; Rubini A; Sabatini S; Soffitta P; Striani E; Vittorini V; Zanello D; Colafrancesco S; Giommi P; Pittori C; Santolamazza P; Verrecchia F; Salotti L
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11585/595688
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