PPT-Selex ES Detector Developments

SDW 2013 Peter Knowles Established Array Capability ACRT growth for photoconductors visible to 20µm LPE growth on CZT for homojunctions and APDs visible to 10µm MOVPE growth on 3 GaAs substrates for heterostructures 2 to 14µm. 山下智弘. JST CREST/. 神戸大学. Borrowing especially from presentations of M. . Asai. (SLAC). Geant4 Tutorial @ Japan 2007. 17-19 Oct, 2007 @ RCNS, based on Geant4 9.0.p01. 1. Outline. Introduction. Matthew Mendonca. Woodside High . School. Mentor. : Dr. . Doug Higinbotham and Lawrence . Selvy. Abstract. The particles that make up the nucleus of an atom are so infinitesimally small that it takes a detector of large magnitude in order to predict where protons and neutrons are located. This certain device requires the construction and utilization of one-meter-long rectangular plastic bars called scintillators. Attached to the left and right ends of each bar are Photomultiplier Tubes (PMTs) and bases with outlets for high voltage and signal wires. In experiments, there is a thick wall of lead positioned in front of the detector which excludes nearly all charged particles and permits primarily neutrons to enter and react with the nuclei inside the bars. When charged particles do pass through the scintillators, photons are released and bounce around until they reach a light guide and are collected by the PMTs. Within these there is liberation of electrons which in turn provide an analog signal to the electronics. A data acquisition system (DAQ) comprised of ADCs (Analog-to-Digital Converters) and TDCs (Time-to-Digital Converters) then store the data into files for later replay and analysis. By doing so, we can better measure the type of particle detected, it’s trajectory, and the amount of energy that it deposits. To ensure that these complex apparatuses are working at an acceptable level, scientists manipulate the constant flux (100 particles/m. B.Satyanarayana, Tata Institute of Fundamental Research, Mumbai. Lecture – I. Saturday, July 2, 2011. B.Satyanarayana, TIFR, Mumbai Resistive Plate Chambers & INO’s ICAL detector SERCEHEP11, VECC, Kolkata. Choice of assembly procedure. Screwing versus . glueing. Pro’s and con’s . MMM Würzburg, 30/01/2014. P. Ponsot/J. Wotschack. 1. Glueing. or screwing ?. The purpose of this presentation is to introduce the discussion on the first choice that we have to make in order to arrive at an agreed assembly procedure. Lab Methods Day. June 25, 2013. Taylor . Myers. 2. Carbon Monoxide Concentration. % of CO, by volume, in the air. Digital readout. Analog output 0/2/4 to 20 mA. Carbon Dioxide Concentration. % of . CO2, . Further developments of detectors with resistive electrodes:. R. Oliveira. 1. , V. Peskov. 1,2. , F. Pietropaolo. 3. , P. Picchi. 4. 1. CERN, Geneva, Switzerland. 2. NAM, Mexico. 3. INFN Padova, Ialy. M. Sullivan. Mini-workshop on the MEIC design. Nov 2, 2012. Introduction. Accelerator Parameters. Previous Synchrotron . R. adiation estimates. Other SR issues. Other detector backgrounds. Points of Interest. 2012/3/2. Y.Sugimoto. Background. Request for more space from DESY team. Several installation works in parallel. Depends on total allowed construction perio. d . Design of common cryogenic system. ILD, . CIV 101-. 03. March 25, 2016. Class . 26. The Rise of the Modern Sovereign State. Eventually, we get Europe out of this mess.. For the time being, they just fight with each other, often. .. Featured MONARCHS who ran the states and “took care of” their people.. Philip Anderson. National Sales Manager. System Sensor Canada. A hospital is like a city. Living areas. Machinery, high technology. Food prep/service. Retail, public spaces. Open spaces, parking. Wide range of application challenges. side. Wago. 2002-1201 . Wago. 2002-3203 . Door open. 800x600x200 mm. 0.93x60 cm. 10 cm. 4.9 cm. 4.9 cm. GSM cable. Gas pipes. ~25cm. ~25cm. NSYS3D8620. Inputs. Outputs. 600. 8. 00. 200. 60cm. 90 ˚ turn. 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 . 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). Previous work [1] studied the use of PTP and Synchronous Ethernet (. SyncE. ) for synchronization of detector data from multiple Pixie-Net modules, an earlier and smaller version of the digitizing and pulse processing electronics described here. The time resolution for coincident events reached ~10ns FWHM with PTP synchronization and 200-800ps FWHM with .