6–8 Jul 2011
Sala Convegni della Cassa di Risparmio di Firenze
Europe/Rome timezone

Session

DAY 1

6 Jul 2011, 08:30
Sala Convegni della Cassa di Risparmio di Firenze

Sala Convegni della Cassa di Risparmio di Firenze

Via Folco Portinari 5 Firenze, Italy

Presentation materials

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  1. Prof. Pier Andrea Mando` (Università di Firenze and INFN)
    06/07/2011, 09:10
    Talk
  2. Dr Daniel Esperante Pereira (Universidade de Santiago de Compostela, Spain)
    06/07/2011, 09:30
    Talk
    The LHCb experiment is one of the four big experiments at the Large Hadron Collider (LHC) and it is designed to perform high-precision measurements of CP violation and search for New Physics. It is constructed as a forward single-arm spectrometer covering the polar angle 15-300 mrad. The Silicon Tracker (ST) of LHCb is a silicon micro-strip detector designed to perform a precise measurement of...
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  3. Dr Derek Strom (University of Illinois at Chicago)
    06/07/2011, 09:50
    Talk
    The CMS tracker is the largest silicon detector ever built, covering 200 square meters and providing an average of 14 high-precision measurements per track. The use of tracker data for reconstruction of charged particles and primary and secondary vertices requires fine-grained monitoring and calibration procedures as well as accurate alignment. Results from timing and threshold optimization,...
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  4. Dominic Hirschbuehl (Wuppertal)
    06/07/2011, 10:10
    Tracking Systems
    Talk
    The ATLAS Pixel Detector is the innermost detector of the ATLAS experiment at the Large Hadron Collider at CERN, providing high-resolution measurements of charged particle tracks in the high radiation environment close to the collision region. This capability is vital for the identification and measurement of proper decay times of long-lived particles such as b-hadrons, and thus vital for the...
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  5. Mr Matthew Chan (Massachusetts Institute of Technology)
    06/07/2011, 10:30
    Tracking Systems
    Talk
    The CMS tracker is the largest silicon detector ever built, covering 200 square meters and providing an average of 14 high-precision measurements per track. Data from proton-proton collisions at a center-of-mass energy of 7 TeV are used to measure the performance of the detector and the reconstruction algorithms. The resolution and efficiency of the track, vertex, and beam line reconstruction...
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  6. Giacomo Contin (TS)
    06/07/2011, 11:20
    Talk
    The Inner Tracking System (ITS) of the ALICE experiment is made out of six layers of silicon detectors exploiting three different technologies (pixel, drift and strip). It covers the central pseudorapidity range of |η| < 0.9 and its distance from the beam line ranges from r = 3.9 cm for the innermost pixel layer up to r = 43 cm for the outermost strip layer. The main tasks of the ITS are to...
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  7. Dr Attilio Andreazza (Università di Milano and INFN)
    06/07/2011, 11:40
    Tracking Systems
    Talk
    The ATLAS Pixel Detector is the innermost detector of the ATLAS experiment at the Large Hadron Collider at CERN. It consists of 1744 silicon sensors equipped with approximately 80 M electronic channels, providing typically three measurement points with high resolution for particles emerging from the beam-interaction region, thus allowing to measure particle tracks and secondary vertices with...
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  8. Junji Tojo (KEK)
    06/07/2011, 12:00
    Talk
    The SemiConductor Tracker (SCT), comprising of silicon micro-strip detectors is one of the key precision tracking devices in the ATLAS Inner Detector. ATLAS is one of the experiments at CERN LHC. The completed SCT is in very good shapes with 99.3% of the SCT’s 4088 modules (a total of 6.3 million strips) are operational. The noise occupancy and hit efficiency exceed the design...
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  9. Ernesto Migliore (University of Torino and INFN)
    06/07/2011, 12:20
    Talk
    The CMS Silicon Tracker consists of 16’588 modules covering an area of more than 200m2. To achieve an optimal track-parameter resolution, the position and orientation of the modules must be determined with a precision of a few microns and an accurate representation of the distribution of material in the tracker is needed. Results of the alignment of the tracker are presented, based on the...
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  10. Dr Salvador Marti`-Garcia (IFIC-València (UVEG-CSIC))
    06/07/2011, 12:40
    Tracking Systems
    Talk
    The ATLAS experiment at the LHC is equipped with a charged particle tracking system, the Inner Detector, built on three subdetectors, which provide high precision measurements made from a fine detector granularity. The Pixel and microstrip (SCT) subdetectors, which use the silicon technology, are complemented with the Transition Radiation Tracker. Since the LHC startup in 2009, the ATLAS...
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  11. Dr Luca Baldini (INFN -Pisa)
    06/07/2011, 15:00
    Talk
    The Large Area Telescope (LAT) is the main instrument onboard the Fermi Gamma-ray Space Telescope, an orbital observatory launched in low-Earth orbit on June 11 2008 to survey the high-energy gamma-ray sky. The LAT tracker/converter serves the twofold purpose of converting the incoming gamma-ray into an electron-positron pair and tracking the latter in order to measure the original photon...
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  12. Mr Matteo Duranti (Università di Perugia and INFN)
    06/07/2011, 15:20
    Tracking Systems
    Talk
    The Alpha Magnetic Spectrometer (AMS-02) is a high-energy physics experiment operating in space on the International Space Station since the 16th of May. Thanks to a large acceptance and a data taking period of, at least, 10 years, AMS-02 will measure over 1010 charged particles in the rigidity range 500 MV - 2 TV. AMS-02 is able to measure the energy spectrum of the cosmic ray components...
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  13. Prof. Piero Spillantini (INFN e Univerità di Firenze)
    06/07/2011, 15:40
    Tracking Systems
    Talk
    GAMMA-400 is a space mission included in the Russian Federal Space Program and supported by the Russian Federal Space Agency. The main characteristics of the mission are a high elliptical orbit (initial parameters: perigee 500 km, apogee 300 000 km), a total mass for the scientific payload of 2600 kg, and a power budget for the instrument of 2 kW. The experiment is intended to improve the...
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  14. Dr Valeria Sipala (INFN Catania and Dip. Fisica Univ Catania, Italy)
    06/07/2011, 16:00
    Talk
    Proton Computed Tomography (pCT) is a medical imaging method based on the use of proton beams with kinetic energy of the order of 250 MeV, aimed at directly measuring the stopping power distribution of tissues (presently calculated from X-rays attenuation coefficients) to improve the accuracy of treatment planning in hadron therapy. A pCT system should be able to measure tissue electron...
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  15. Dr Domenico Lo Presti (University of Catania)
    06/07/2011, 16:20
    Talk
    In this paper we describe a new detection system both for tracking and measurement of the residual range, designed and developed with the aim of achieving real-time imaging, large detection areas with high space and time resolutions. The tracker has been designed and tested as a prototype, with a large area of 20 x 20 sqcm, consisting in two ribbons of scintillating fibers positioned in the...
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  16. Cinzia Talamonti (INFN Firenze, Dipartimento di Fisiopatologia Clinica Univ. Firenze and Azienda Ospedaliera Universitaria Careggi Firenze,Italy)
    06/07/2011, 16:40
    Talk
    We present first results of a project devoted to the development of a large-area modular detector for intensity modulated radiotherapy based on high – quality polycrystalline diamond produced by Chemical Vapour Deposition. The work is performed in the framework of the DIAPIX project of INFN CSN5. The proposed modular system is based on an electronic-grade quality polycrystalline diamond...
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  17. Prof. Emanuele Antoniucci, Prof. Giovanni Vitangeli
    06/07/2011, 17:30
    Organ and Trumpet Concert
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  18. 06/07/2011, 18:30
Building timetable...