PPT-Calorimeter Electronics Status

Author : mitsue-stanley | Published Date : 2019-11-08

Calorimeter Electronics Status HCal Modules 16 EmCal Sector 0 Steve Boose BNL 11719 Calorimeter Electronics 1 CalElect Status EMCal Sector 0 All electronics boards

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Calorimeter Electronics Status: Transcript


Calorimeter Electronics Status HCal Modules 16 EmCal Sector 0 Steve Boose BNL 11719 Calorimeter Electronics 1 CalElect Status EMCal Sector 0 All electronics boards in hand Cables production waiting preliminary assembly of Sector 0 to verify routing and cable lengthsorientation. 7 311 332 285 Internet Advertising 261 277 301 357 Email Advertising 253 249 293 359 Direct Mail 224 226 235 204 Magazines 197 184 225 268 Cable 189 205 222 200 Newspaper 189 186 222 170 Radio 175 188 181 134 Social Media Facebook Twitter etc 142 164 Jackson Choate. ATLAS Calorimeters. The Science Behind It…. High-energy electrons and photons lose energy primarily through Bremsstrahlung and pair production, respectively.. Bremsstrahlung and pair production produce more electrons and photons at lower energies. Peilong Wang, Southern Methodist University. For PHYS 5380 Fall 2014. Outline. Physics requirements for the ATLAS . LAr. Calorimeter. Structure of the ATLAS . LAr. Calorimeters. Electromagnetic Calorimeters. Jin Huang. Los Alamos National Lab. Calorimeter defines the inner-R edge of large-angle acceptance. The proposal assumed a 2.5 degree polar angle gap (14.5-17). Calorimeter Group Communications. Jin Huang. τ. Reconstruction . In High Luminosity LHC(HL-LHC. ). With a High Granularity Endcap Calorimeter. A. . Izadi. Rad (Sharif University of Technology, Iran), P. . Tereziu. (Faculty of Natural Sciences, University of Tirana). during Fall . GMp. run. February 24. th. 2016. Alexandre . Camsonne. DVCS setup. Stand has range from 10 to 16 degrees. Z position from 1.5 m to 5.5 m. Carrier about 2 m x 1m. 208 channels of RG 213 signal going in HRS. TileCal. ) at the LHC is used to measure the hadrons produced with polar angles >21. 0 . and the energy deposition of ~20MeV to ~1.3TeV in the detector cells. The total readout channels are ~10K and the required readout dynamic range is 16-bit. The front-end readout electronics of the ATLAS . Roger Rusack – The University of Minnesota. 3/19/14. rusack@physics.umn.edu. 1. Contributing Institutions. 3/19/14. 2. Athens, Beijing, CERN, . Demokritos. , Imperial College, . Iowa, LLR, Minnesota, SINP (Kolkata) & UC Santa Barbara. Nisha Kondrath. Assistant Professor. Dept. of Electrical and Computer Engineering. University of Minnesota Duluth. Background. Education. Doctor of Philosophy in Engineering. Wright State University, Dayton, OH, 2010. Vincent . Sulkosky. Longwood University. for the E12-07-108 . Collaboration. Hall A . DVCS Collaboration . Meeting. December 19-20, . 2013. 1. Outline . . The . GMp. Experiment: . Goals and Physics Motivation. cal. /g·°C) to consume the drink?.  . a. Calculate . the energy expended (in . Cal. ) to consume a 12-oz beer (about 355 mL) if the beer is initially at 4.0°C. Assume the drink is mostly water and its density is 1.01 g/. Electron is just a particle that can't be defined, but it has charge & tendency to flow. This nature of electron has made a separate section of study called electronics engineering .. Electronics is about study, designing & implementation of different components/circuits for various human necessities. . Ulrich Heintz. Brown . University. for the CMS HCAL group. 3/20/2014. Ulrich Heintz - ACES 2014. 1. CMS hadron calorimeters. 3/20/2014. Ulrich Heintz - ACES 2014. 2. HB/HE (barrel/. endcap. ). brass/scintillator. P. . Antilogus. , P. . Bailly. , . P. Barrillon. , S. . Baumont. , M. . Dhellot. , J. . Jeglot. , C. . Juramy. -Gilles, . H. . Lebbolo. , D. Martin, M. . Moniez. , S. Russo, . D. . Terront. , V. . Tocut.

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