PPT-HPS – ECal Detector - TECHNICAL

Author : elitered | Published Date : 2020-08-27

PARAMETERS The experimental apparatus includes two main detectors a silicon vertex tracker SVT for precise momentum vertex determination and and an electromagnetic

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HPS – ECal Detector - TECHNICAL: Transcript


PARAMETERS The experimental apparatus includes two main detectors a silicon vertex tracker SVT for precise momentum vertex determination and and an electromagnetic calorimeter ECal to trigger on . Rémi . Cornat. Laboratoire Leprince-Ringuet. Ecole Polytechnique – . IN2P3/CNRS. On . behalf. of the . SiW. -ECAL ILD . project. *. w. ithin. CALICE coll.. 2. From this.... t. o this. . :. ECAL. nA. -- ~3 . mkA. HCAL, similar expected for ECAL), the magnitude of the LED difference does not depend on the PMT . position (Irina). . Jacques’ hypothesis: this can be rate effect, it is known to saturate at anode currents of 10-100 . Guido Haefeli, Lausanne PEBS meeting 10.Jan. 2011. 1. Overview. SPIROCA in . testbeam. 9.2010. (Jean-. Baptiste. ). Why change from . SPIROCA to VATA64?. VATA64 measurements. Plans for the electronics . 16/03/2011. 2. Integrator boards. NB. requires slight modification of CW bases: install 100 . nF. in series with 25 . Ω. . This does not affect the signal.. Recently, the integrators were upgraded: the 40 mezzanines were replaced with new ones.. Status . Patrick Robbe, LAL Orsay, 18 Sep 2011. Trigger Rates. With L=3.5x10. 32. , . m. =1.4, 1380 bunches. Hadron (. E. T. >. 3.5 . GeV. and SPD<600): . 395 kHz. Electron (. E. T. >. 2.5 . engineering. (these are slides which were updated after the meeting). 1. 2. Summary of ECAL . discussions (by C. . Grefe. ):. - In previous discussions it has been agreed that the inner radius of the ECAL should be ~1500mm. This fact alone results a significant cost reduction with respect to the ILD ECAL which starts at ~1800mm.. SLAC. Heavy Photon Search Collaboration Meeting. Thomas Jefferson National Accelerator Facility, May 26-27, 2011. 1. HPS Test Run Goals. Primary HPS Test Run Goals:. M. easure . Si sensor occupancies . 9 . Nov. 2018 (GMT . 313. ). To. 16:00 on . M. on 12 Nov. . 2018 (GMT . 316. ). AMS on ISS. Readout. Data Reduction. Detectors. POIC, MSFC. AMS CAN Bus. AMS. Laptop. Ku-band. S-band. Internet. AMSWire. Highlights. Inner silicon detector, 700,000 channels. Scintillating fiber tracker & . preshower. , . 100,000 channels. Uranium/liquid argon calorimeter, 50,000 channels. Muon. system (wire chambers and scintillator), 70,000 channels. Brian . Kross. – mechanical design and construction / gas systems. Seungjoon. Lee – advanced image recon algorithms / mechanical / detectors. John . McKisson. – software / data acquisition / electronics. Sergey . Boyarinov. Sep 25, 2017. N. otation. ECAL – old EC (electromagnetic calorimeter). PCAL – . preshower. calorimeter. DC – drift chamber. HTCC – high threshold . cherenkov. counter. FT – forward tagger. FCC week Washington. 23. -27 March . 2015. W. . Riegler. D. . Denisov. , H. . ten. Kate, L. . Lienssen. , F. . Lanni. , M. . Abbrescia. , R. Richter, Y. . Onel. , W. Smith, S. . C. hekanov. Exploration + Higgs as a tool for . Nabarun . Dev. 1. , Colin Jessop. 1. , Nancy Marinelli. 1. , Maurizio Pierini. 2. 08. /11/. 2017. 1 . University of Notre . Dame. 2. CERN. DQM-ML meeting. Outline. N.Dev, University of Notre Dame. DQM-ML Meeting, 08/11/17. DEELS 2016. DESY, 27-28 . June. 2016. Marie LABAT, Nicolas HUBERT. In-Air X-ray Detector. Image of the vertical beam profile. Hard X-rays crossing the crotch absorber behind dipoles magnets.. Design by ESRF (6 GeV) and applied at ANKA (2,5 GeV) and ALBA (3 GeV).

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