PPT-Eleonora Presani shower Reconstruction in the ANTARES detector

Shower reconstruction general idea Expected time for each hit So I need at least 3 hits to compute the shower parameters t 0 dzo The goal is to minimize the difference between the measured hit time and the expected hit time. Cardinal Shower Enclosures is a full service domestic manufacturer of shower enclosures, offering an extremely wide selection of models, finishes and glass options, from patterned to cast glass. Cardinal Shower Enclosures offers several trim levels of sliding door enclosures, from the basic Cardinal Builder series up to the luxurious Heavy Euro and Apollo series. Framed sliders have metal all the way around the glass while frameless sliders have clips holding the top of the glass. Lecture 12 / Homework 4. Breadth-First Search. Given source vertex S:. Find min. #edges to reach every vertex from S. (Assume source is vertex 0). 0. 1. 1. 2. 2. 3. Sequential . pseudocode. :. let Q be a queue. of Plastic Scintillator. Oct. 2, 2009. IP-BSM Group. 1. Schematic . Drawing . of. new Gamma Detector. 2. sandwich type calorimeter. SUS and plastic scintillation plate. wavelength-shifting fiber (WLSF) for light transmission. Hadronic. Final State Reconstruction in Collider Experiments. (Part II). Peter Loch. University of Arizona. Tucson, Arizona. USA. Principles of . Calorimetry. Detector needs for multi-purpose collider experiments. C.W. James, . ECAP, University of Erlangen,. on behalf of the ANTARES collaboration.. Cosmic . rays and neutrinos. What produces this spectrum?. Standard model: acceleration at relativistic astrophysical shocks. t. elescope . Simone . Biagi. on behalf of the ANTARES collaboration. INFN, . Laboratori. . Nazionali. del . Sud. RICH 2016 – Bled 8 Sept 2016. ANTARES: the largest Northern neutrino telescope. Scientific goals. Adam Para. January . 23. , . 2009. Goals and Purposes. Study the spatial (and temporal) distribution of energy deposition inside hadronic showers in BGO (and other crystals). To optimize the dimensions of the test beam hadron calorimeter prototype. LHCf. 　. Hiroaki MENJO . (KMI, Nagoya University, Japan). On behalf of the LHCf collaboration. Mini-workshop ”UHECR . and hadron interaction in the LHC . era” . @ ICRR, 12 Oct. 2011. Introduction . REAM. 1. λ. CW+1. λ . AC. @. 1.25Gbps). 2xCu. 50/50. DOM. APD. 2 Lasers. tunable. PIN. VOA. C1. LiNbO3 . Junction Box. λ. 4. LiNbO3 . λ. 4. λ. 4. λ. 5. λ. 5. SPM. Antares. DWDM . crate. λ. 5. M.Frank. 1. , F.Gaede. 2,. S.Lu. 2. , . N.Nikiforou. 1. , M.Petric. 1. , A.Sailer. 1. 1. CERN, . 2. DESY. 17 September 2015. N.Nikiforou. , ROOT Users' Workshop 2015. 1. Motivation and goals. 17 September 2015. The Beijing Electron Positron Collider II BEPCII the upgrade of BEPC is a multi-bunch ee- collider that is scheduled to provide collisions in 2007 The BESIII 1 is a general-purpose detector being buil IceCube. Justin Vandenbroucke, June 9, 2021. IceCube. Bootcamp, WIPAC, UW–Madison. Outline. Neutrino interactions and cross sections. Muon lifetime. Charged particles losing energy in matter. Ionization. By: . Ayan. . Batyrkhanov. For Horizon-t group. 1. Horizon-T Group. R. .. U. . . Beisembaev. , . E. .. A. . . Beisembaeva. , . O. .. D. . . Dalkarov. , . V. .. A. . . Ryabov. , . S. .. B. . . Shaulov.