The LUX Experiment Trigger and Data Acquisition Systems. Eryk Druszkiewicz April 15 th 2013
|
|
- Randall Kelly
- 6 years ago
- Views:
Transcription
1 The LUX Experiment Trigger and Data Acquisition Systems Eryk Druszkiewicz April 15 th 2013
2 Principle of operation Two-phase operation: Initial interaction produces scintillation light and free electrons (the number of free electrons differs for nuclear and electron interactions). Scintillation light is detected immediately in the PMTs (S1 signal). The free electrons drift through the Xenon and escape from the liquid. They are amplified in the gas region and produce a second pulse in the PMTs (S2 signal). The time difference between the S1 and S2 signals provide information about the vertical position of the interaction. 2
3 LUX DAQ & Trigger Overview Specially shaped signals for: The Struck digitizers Digital trigger CAEN discriminators Jeremy Chapman (Brown) Pre-Amp Post-Amp Trigger channel summing UC Davis Harvard 3
4 LUX DAQ Based on the Struck SIS3301: 100 MHz sampling with 14-bit resolution Customized firmware allowing for Pulse Only Digitization (POD) 1.5 khz acquisition rate with zero dead time and >99% zero suppression 95% single photoelectrons > 5σ of baseline noise > 200 kev ee dynamic range with dark matter search gains 4
5 LUX DAQ Sample Event 1.5 kev ee event 5
6 LUX Trigger Overview DDC-8DSP Trigger Builder (TB) 64 MHz sampling at 14-bit resolution Processing Mbytes/second Trigger decision reached within a few microseconds (mostly due to integration length of the filters) Four lane LVDS links over HDMI between DDCs and TB Major operation modes: S1, S2, S1&S2 We have full control over the firmware! (developed by E.D.) 6
7 Digital filter for S1 and S2 detection Primary goals: Response proportional to the area of the pulse Remove the baseline S1 filter specification: Integration width = ~ ns Dynamic range = 800 phe (linear), 2000 phe (non-linear) S2 filter specification: Integration width = ~ ns Dynamic range = phe (linear), phe (non-linear) 7
8 Trigger example Generated event S1 found S2 found 2 μs Trigger 3.1 μs Necessary to exclude the possibility of the pulse being an S2-type. Coincidence window (2 μs) + time to transfer trigger data to the TB and make the final trigger decision. 8
9 Fiducialization of events Key points of the maximum based trigger: The top PMTs provide X,Y localization We find the group of PMTs that saw the maximum signal We generate a trigger if the group belongs to the fiducial volume Top PMT trigger grouping The efficiency is energy independent. 9
10 System monitoring The DDC-8DSPs perform constant channel sweeps in the background without affecting the trigger performance. Loose cable Monitoring data is incorporated into the Slow-Control of the experiment and allows for setting automated alarms and notifications. 10
11 Ease of reconfiguration Configuration via GUIs The operation and control of the DAQ acquisitions and the trigger is closely tied with the use of a centralized MySql database. This leaves less room for operator error and also gives a precise record of all activities and usage of the system. Configuration via XML files 11
12 Final remarks Both DAQ and Trigger have been extensively tested over the last year. We suppress % of electronics noise baseline. Diagnostic tools that have been developed to monitor the data flow and the performance of the system have proven to be priceless. Being in full control of the trigger firmware has been critical for the success of the project. Main supported trigger modes: S1, S2, S1+S2, VETO large S1 signals, VETO large S2 signals, maximum signal detection and also generating gating signals for the acquisition. The flexibility of the Trigger has been important in improving data collection efficiency under a wide range of conditions. Thank you. Questions? 12
arxiv: v1 [physics.ins-det] 26 Nov 2015
Preprint typeset in JINST style - HYPER VERSION arxiv:1511.08385v1 [physics.ins-det] 26 Nov 2015 The Data Acquisition System for LZ Eryk Druszkiewicz a, for the LZ Collaboration a Department of Physics
More informationDigital trigger system for the RED-100 detector based on the unit in VME standard
Journal of Physics: Conference Series PAPER OPEN ACCESS Digital trigger system for the RED-100 detector based on the unit in VME standard To cite this article: D Yu Akimov et al 2016 J. Phys.: Conf. Ser.
More informationTraditional analog QDC chain and Digital Pulse Processing [1]
Giuliano Mini Viareggio April 22, 2010 Introduction The aim of this paper is to compare the energy resolution of two gamma ray spectroscopy setups based on two different acquisition chains; the first chain
More informationDarkSide-50. Alessandro Razeto LNGS 26/3/14
DarkSide-50 Alessandro Razeto LNGS 26/3/14 CRH Radon-free clean assembly room 5 mbq/m3 in >100 m3 μ veto a d passive shield 1000 ton water Cherenkov neutron veto 30 ton borated liquid scintillator TPC
More informationevent physics experiments
Comparison between large area PMTs at cryogenic temperature for neutrino and rare Andrea Falcone University of Pavia INFN Pavia event physics experiments Rare event physics experiment Various detectors
More informationINDEX. Firmware for DPP (Digital Pulse Processing) DPP-PSD Digital Pulse Processing for Pulse Shape Discrimination
Firmware for DPP (Digital Pulse Processing) Thanks to the powerful FPGAs available nowadays, it is possible to implement Digital Pulse Processing (DPP) algorithms directly on the acquisition boards and
More informationTesting the Electronics for the MicroBooNE Light Collection System
Testing the Electronics for the MicroBooNE Light Collection System Kathleen V. Tatem Nevis Labs, Columbia University & Fermi National Accelerator Laboratory August 3, 2012 Abstract This paper discusses
More informationPreliminary simulation study of the front-end electronics for the central detector PMTs
Angra Neutrino Project AngraNote 1-27 (Draft) Preliminary simulation study of the front-end electronics for the central detector PMTs A. F. Barbosa Centro Brasileiro de Pesquisas Fsicas - CBPF, e-mail:
More informationarxiv: v2 [physics.ins-det] 17 Oct 2015
arxiv:55.9v2 [physics.ins-det] 7 Oct 25 Performance of VUV-sensitive MPPC for Liquid Argon Scintillation Light T.Igarashi, S.Naka, M.Tanaka, T.Washimi, K.Yorita Waseda University, Tokyo, Japan E-mail:
More informationDigital coincidence acquisition applied to portable β liquid scintillation counting device
Nuclear Science and Techniques 24 (2013) 030401 Digital coincidence acquisition applied to portable β liquid scintillation counting device REN Zhongguo 1,2 HU Bitao 1 ZHAO Zhiping 2 LI Dongcang 1,* 1 School
More informationarxiv: v2 [astro-ph.im] 2 Jul 2012
Preprint typeset in JINST style - HYPER VERSION Tests of PMT Signal Read-out of Liquid Argon Scintillation with a New Fast Waveform Digitizer arxiv:1203.1371v2 [astro-ph.im] 2 Jul 2012 R. Acciarri a, N.
More informationDAQ & Electronics for the CW Beam at Jefferson Lab
DAQ & Electronics for the CW Beam at Jefferson Lab Benjamin Raydo EIC Detector Workshop @ Jefferson Lab June 4-5, 2010 High Event and Data Rates Goals for EIC Trigger Trigger must be able to handle high
More informationGAMMA-GAMMA CORRELATION Latest Revision: August 21, 2007
C1-1 GAMMA-GAMMA CORRELATION Latest Revision: August 21, 2007 QUESTION TO BE INVESTIGATED: decay event? What is the angular correlation between two gamma rays emitted by a single INTRODUCTION & THEORY:
More informationDirect Dark Matter Search with XMASS --- modulation analysis ---
Direct Dark Matter Search with XMASS --- modulation analysis --- ICRR, University of Tokyo K. Kobayashi On behalf of the XMASS collaboration September 8 th, 2015 TAUP 2015, Torino, Italy XMASS experiment
More informationGamma Ray Spectroscopy with NaI(Tl) and HPGe Detectors
Nuclear Physics #1 Gamma Ray Spectroscopy with NaI(Tl) and HPGe Detectors Introduction: In this experiment you will use both scintillation and semiconductor detectors to study γ- ray energy spectra. The
More informationDarkSide-50 and DarkSide-20k experiments: computing model and evolution of infrastructure
DarkSide-50 and DarkSide-20k experiments: computing model and evolution of infrastructure Simone Sanfilippo Università degli Studi Roma 3 INFN - Sezione Roma 3 on behalf of the DarkSide Collaboration May
More informationMuLan Experiment Progress Report
BV 37 PSI February 16 2006 p. 1 MuLan Experiment Progress Report PSI Experiment R 99-07 Françoise Mulhauser, University of Illinois at Urbana Champaign (USA) The MuLan Collaboration: BERKELEY BOSTON ILLINOIS
More informationDigital Signal Processing Electronics for Nuclear Physics Applications
Digital Signal Processing Electronics for Nuclear Physics Applications Small Business Innovation Research Department Of Energy Grant DE-FG02-03ER83778 Wojtek Skulski SkuTek Instrumentation and University
More informationFinal Report Data Acquisition Box
Final Report Data Acquisition Box By Gene Bender DeSmet Jesuit High School July 25, 2003 Contents Overview...2 A Hybrid LBNL Cosmic Ray Detector...2 The Detectors...6 Changing PMT Voltage...7 Comparator
More informationarxiv: v1 [physics.ins-det] 7 Jul 2017
Prepared for submission to JINST Update of the trigger system of the PandaX-II experiment arxiv:1707.02134v1 [physics.ins-det] 7 Jul 2017 Qinyu Wu, a Xun Chen, a Xiangdong Ji, a,b,c,d Jianglai Liu, a Siao
More informationDigital Signal Processing for HPGe Detectors
Digital Signal Processing for HPGe Detectors David Radford ORNL Physics Division July 28, 2012 HPGe Detectors Hyper-Pure Ge (HPGe) detectors are the gold standard for gamma-ray spectroscopy Unsurpassed
More informationNIM. ADCs (Peak Sensing) Analog Pulse Processors Amplifiers (Fast) Amplifiers (Spectroscopy) Attenuators Coincidence/Logic/Trigger Units
The NIM-Nuclear Instrumentation Module standard is a very popular form factor widely used in experimental Particle and Nuclear Physics setups. Defined the first time by the U.S. Atomic Energy Commission
More informationCAEN. Electronic Instrumentation. CAEN Silicon Photomultiplier Kit
CAEN Tools for Discovery Electronic Instrumentation CAEN Silicon Photomultiplier Kit CAEN realized a modular development kit dedicated to Silicon Photomultipliers, representing the state-of-the art in
More informationData Acquisition System for the Angra Project
Angra Neutrino Project AngraNote 012-2009 (Draft) Data Acquisition System for the Angra Project H. P. Lima Jr, A. F. Barbosa, R. G. Gama Centro Brasileiro de Pesquisas Físicas - CBPF L. F. G. Gonzalez
More informationMSCF-16- PMT V
MSCF-16- PMT V4.0-1.0 16 fold Spectroscopy Amplifier with CFDs and Multiplicity Trigger mesytec MSCF-16-PMT is an integrating shaping / timing filter amplifier with constant fraction discriminator and
More informationMASE: Multiplexed Analog Shaped Electronics
MASE: Multiplexed Analog Shaped Electronics C. Metelko, A. Alexander, J. Poehlman, S. Hudan, R.T. desouza Outline 1. Needs 2. Problems with existing Technology 3. Design Specifications 4. Overview of the
More informationHighly Segmented Detector Arrays for. Studying Resonant Decay of Unstable Nuclei. Outline
Highly Segmented Detector Arrays for Studying Resonant Decay of Unstable Nuclei MASE: Multiplexed Analog Shaper Electronics C. Metelko, S. Hudan, R.T. desouza Outline 1. Resonant Decay 2. Detectors 3.
More informationDevelopment of LYSO detector modules for a charge-particle EDM polarimeter
Mitglied der Helmholtz-Gemeinschaft Development of LYSO detector modules for a charge-particle EDM polarimeter on behalf of the JEDI collaboration Dito Shergelashvili, PhD student @ SMART EDM_Lab, TSU,
More informationPMT Calibration in the XENON 1T Demonstrator. Abstract
PMT Calibration in the XENON 1T Demonstrator Sarah Vickery Nevis Laboratories, Columbia University, Irvington, NY 10533 USA (Dated: August 2, 2013) Abstract XENON Dark Matter Project searches for the dark
More informationStatus of Primex Beam Position Monitor July 29 th, 2010
Status of Primex Beam Position Monitor July 29 th, 2010 Anthony Tatum University of North Carolina at Wilmington The Beam Position Monitor (BPM) is used to determine the vertical and horizontal position
More informationThe Trigger System of the MEG Experiment
The Trigger System of the MEG Experiment On behalf of D. Nicolò F. Morsani S. Galeotti M. Grassi Marco Grassi INFN - Pisa Lecce - 23 Sep. 2003 1 COBRA magnet Background Rate Evaluation Drift Chambers Target
More informationSilicon Photomultiplier Evaluation Kit. Quick Start Guide. Eval Kit SiPM. KETEK GmbH. Hofer Str Munich Germany.
KETEK GmbH Hofer Str. 3 81737 Munich Germany www.ketek.net info@ketek.net phone +49 89 673 467 70 fax +49 89 673 467 77 Silicon Photomultiplier Evaluation Kit Quick Start Guide Eval Kit Table of Contents
More informationP. Branchini (INFN Roma 3) Involved Group: INFN-LNF G. Felici, INFN-NA A. Aloisio, INFN-Roma1 V. Bocci, INFN-Roma3
P. Branchini (INFN Roma 3) Involved Group: INFN-LNF G. Felici, INFN-NA A. Aloisio, INFN-Roma1 V. Bocci, INFN-Roma3 Let s remember the specs in SuperB Baseline: re-implement BaBar L1 trigger with some improvements
More informationLevel-1 Calorimeter Trigger Calibration
December 2004 Level-1 Calorimeter Trigger Calibration Birmingham, Heidelberg, Mainz, Queen Mary, RAL, Stockholm Alan Watson, University of Birmingham Norman Gee, Rutherford Appleton Lab Outline Reminder
More informationGoal of the project. TPC operation. Raw data. Calibration
Goal of the project The main goal of this project was to realise the reconstruction of α tracks in an optically read out GEM (Gas Electron Multiplier) based Time Projection Chamber (TPC). Secondary goal
More informationA small dual-phase xenon TPC with APD and PMT readout for the study of liquid xenon scintillation
A small dual-phase xenon TPC with APD and PMT readout for the study of liquid xenon scintillation Institute of Physics & PRISMA Cluster of Excellence, Johannes Gutenberg University, Mainz, Germany E-mail:
More informationEUDET Pixel Telescope Copies
EUDET Pixel Telescope Copies Ingrid-Maria Gregor, DESY December 18, 2010 Abstract A high resolution beam telescope ( 3µm) based on monolithic active pixel sensors was developed within the EUDET collaboration.
More informationPARISROC, a Photomultiplier Array Integrated Read Out Chip
PARISROC, a Photomultiplier Array Integrated Read Out Chip S. Conforti Di Lorenzo a, J.E. Campagne b, F. Dulucq a, C. de La Taille a, G. Martin-Chassard a, M. El Berni a, W. Wei c a OMEGA/LAL/IN2P3, centre
More informationAIDA-2020 Advanced European Infrastructures for Detectors at Accelerators. Deliverable Report. CERN pixel beam telescope for the PS
AIDA-2020-D15.1 AIDA-2020 Advanced European Infrastructures for Detectors at Accelerators Deliverable Report CERN pixel beam telescope for the PS Dreyling-Eschweiler, J (DESY) et al 25 March 2017 The AIDA-2020
More informationMulti-channel front-end board for SiPM readout
Preprint typeset in JINST style - HYPER VERSION Multi-channel front-end board for SiPM readout arxiv:1606.02290v1 [physics.ins-det] 7 Jun 2016 M. Auger, A. Ereditato, D. Goeldi, I. Kreslo, D. Lorca, M.
More informationThe MUSE experiment. Technical Overview. Guy Ron (for the MUSE collaboration) Hebrew University of Jerusalem
The MUSE experiment Technical Overview Guy Ron (for the MUSE collaboration) Hebrew University of Jerusalem MUSE is not your garden variety scattering experiment Low beam flux Large angle, non-magnetic
More informationElectronic Instrumentation for Radiation Detection Systems
Electronic Instrumentation for Radiation Detection Systems January 23, 2018 Joshua W. Cates, Ph.D. and Craig S. Levin, Ph.D. Course Outline Lecture Overview Brief Review of Radiation Detectors Detector
More informationRP220 Trigger update & issues after the new baseline
RP220 Trigger update & issues after the new baseline By P. Le Dû pledu@cea.fr Cracow - P. Le Dû 1 New layout features Consequence of the meeting with RP420 in Paris last September Add 2 vertical detection
More informationMSCF-16 F (Data sheet V51_02)
(Data sheet V51_02) 16 fold Spectroscopy Amplifier with CFDs and Multiplicity Trigger mesytec is a shaping / timing filter amplifier with constant fraction discriminator and multiplicity trigger and provides
More informationDetecting and Suppressing Background Signal
Detecting and Suppressing Background Signal Valerie Gray St. Norbert College Advisors: Dr. Michael Wiescher Freimann Professor Nuclear Physics University of Notre Dame Dr. Ed Stech Associate Professional
More informationSpring 2018 Group Update
Spring 2018 Group Update Jonathan Nikoleyczik Todays update starts on slide 57 1 Current tasks Gamma-X events from calibration sources Phase 1 optical maps Simulate LZ calibrations and see how they are
More informationRadionuclide Imaging MII 3073 RADIONUCLIDE IMAGING SYSTEM
Radionuclide Imaging MII 3073 RADIONUCLIDE IMAGING SYSTEM Preamplifiers and amplifiers The current from PMT must be further amplified before it can be processed and counted (the number of electrons yielded
More informationCHAPTER 8 PHOTOMULTIPLIER TUBE MODULES
CHAPTER 8 PHOTOMULTIPLIER TUBE MODULES This chapter describes the structure, usage, and characteristics of photomultiplier tube () modules. These modules consist of a photomultiplier tube, a voltage-divider
More informationInstructions for gg Coincidence with 22 Na. Overview of the Experiment
Overview of the Experiment Instructions for gg Coincidence with 22 Na 22 Na is a radioactive element that decays by converting a proton into a neutron: about 90% of the time through β + decay and about
More informationPARTICLE DETECTORS (V): ELECTRONICS
Monday, April 13, 2015 1 PARTICLE DETECTORS (V): ELECTRONICS Zhenyu Ye April 13, 2015 Monday, April 13, 2015 2 References Techniques for Nuclear and Particle Physics Experiments by Leo, Chapter 15-17 Particle
More informationTime-of-flight PET with SiPM sensors on monolithic scintillation crystals Vinke, Ruud
University of Groningen Time-of-flight PET with SiPM sensors on monolithic scintillation crystals Vinke, Ruud IMPORTANT NOTE: You are advised to consult the publisher's version (publisher's PDF) if you
More informationNIM INDEX. Attenuators. ADCs (Peak Sensing) Discriminators. Translators Analog Pulse Processors Amplifiers (Fast) Amplifiers (Spectroscopy)
NIM The NIM-Nuclear Instrumentation Module standard is a very popular form factor widely used in experimental Particle and Nuclear Physics setups. Defined the first time by the U.S. Atomic Energy Commission
More informationMicromegas for muography, the Annecy station and detectors
Micromegas for muography, the Annecy station and detectors M. Chefdeville, C. Drancourt, C. Goy, J. Jacquemier, Y. Karyotakis, G. Vouters 21/12/2015, Arche meeting, AUTH Overview The station Technical
More informationMoller DAQ with the FADC250 B 2. Figure M1 CR SR CL SL FADC SD_FP. VME64x FLEX_I/O ROC CR: CALORIMETER RIGHT [1-4] SR: SCINTILLATOR RIGHT [1-4]
Moller DAQ with the F5 CR: CALORIMETER RIGHT [1-] CR SR CL SL F SR: SCINTILLATOR RIGHT [1-] CL: CALORIMETER LEFT [1-] SL: SCINTILLATOR LEFT [1-] A b a SD_FP A: [ HELICITY, HELICITY_FLIP ] (NIM or ECL)
More informationRadiation Test Report Paul Scherer Institute Proton Irradiation Facility
the Large Hadron Collider project CERN CH-2 Geneva 23 Switzerland CERN Div./Group RadWG EDMS Document No. xxxxx Radiation Test Report Paul Scherer Institute Proton Irradiation Facility Responsibility Tested
More informationThe detector system of the EPOS system
The detector system of the EPOS system 1. The detector arrangement 2. The lifetime system 3. Digital Doppler measurement 4. AMOC Martin-Luther-Universität RK Halle R Detector system 3 experiments: lifetime
More informationA Prototype Amplifier-Discriminator Chip for the GLAST Silicon-Strip Tracker
A Prototype Amplifier-Discriminator Chip for the GLAST Silicon-Strip Tracker Robert P. Johnson Pavel Poplevin Hartmut Sadrozinski Ned Spencer Santa Cruz Institute for Particle Physics The GLAST Project
More informationFRS setup. FRS web page. Standard FRS detectors. Detectors needed for simulations
FRS setup FRS web page Standard FRS detectors Detectors needed for simulations FRS web page The FRS web page for technical information is : http://www-w2k.gsi.de/frs/technical.asp. This web page is important
More informationCosmic Ray Detector Hardware
Cosmic Ray Detector Hardware How it detects cosmic rays, what it measures and how to use it Matthew Jones Purdue University 2012 QuarkNet Summer Workshop 1 What are Cosmic Rays? Mostly muons down here
More informationnanomca-sp datasheet I. FEATURES
datasheet nanomca-sp 80 MHz HIGH PERFORMANCE, LOW POWER DIGITAL MCA WITH BUILT IN PREAMPLIFIER Model Numbers: SP0534A/B to SP0539A/B Standard Models: SP0536B and SP0536A I. FEATURES Built-in preamplifier
More informationReal-Time Pulse-Shape Discrimination and Beta-Gamma Coincidence Detection in Field- Programmable Gate Array
Real-Time Pulse-Shape Discrimination and Beta-Gamma Coincidence Detection in Field- Programmable Gate Array A. T. Farsoni, B. Alemayehu, A. Alhawsawi, E. M. Becker Department of Nuclear Engineering and
More informationLIFETIME OF THE MUON
Muon Decay 1 LIFETIME OF THE MUON Introduction Muons are unstable particles; otherwise, they are rather like electrons but with much higher masses, approximately 105 MeV. Radioactive nuclear decays do
More informationExperiment 10. The Speed of Light c Introduction Apparatus
Experiment 10 The Speed of Light c 10.1 Introduction In this experiment you will measure the speed of light, c. This is one of the most fundamental constants in physics, and at the same time the fastest
More informationA Fast Waveform-Digitizing ASICbased DAQ for a Position & Time Sensing Large-Area Photo-Detector System
A Fast Waveform-Digitizing ASICbased DAQ for a Position & Time Sensing Large-Area Photo-Detector System Eric Oberla on behalf of the LAPPD collaboration PHOTODET 2012 12-June-2012 Outline LAPPD overview:
More informationReal Time Pulse Pile-up Recovery in a High Throughput Digital Pulse Processor
Real Time Pulse Pile-up Recovery in a High Throughput Digital Pulse Processor Paul A. B. Scoullar a, Chris C. McLean a and Rob J. Evans b a Southern Innovation, Melbourne, Australia b Department of Electrical
More informationCOMPENDIUM OF FRONT-END ELECTRONICS
COMPENDIUM OF FRONT-END ELECTRONICS F. MESSI Division of Nuclear Physics, Lund University and European Spallation Source ERIC Lund, Sweden Email: francesco.messi@nuclear.lu.se Abstract Our world is changing
More informationCAEN Tools for Discovery
Viareggio 5 September 211 Introduction In recent years CAEN has developed a complete family of digitizers that consists of several models differing in sampling frequency, resolution, form factor and other
More informationMSCF-16-LN (Data sheet V5.0_01)
(Data sheet V5.0_01) 16 fold Spectroscopy Amplifier with active BLR, CFDs, and Multiplicity Trigger mesytec MSCF-16-LN is an ultra low noise spectroscopy amplifier with active baseline restorer. It provides
More information50 MHz Voltage-to-Frequency Converter
Journal of Physics: Conference Series OPEN ACCESS 50 MHz Voltage-to-Frequency Converter To cite this article: T Madden and J Baldwin 2014 J. Phys.: Conf. Ser. 493 012008 View the article online for updates
More informationnanodpp datasheet I. FEATURES
datasheet nanodpp I. FEATURES Ultra small size high-performance Digital Pulse Processor (DPP). 16k channels utilizing smart spectrum-size technology -- all spectra are recorded and stored as 16k spectra
More informationCAEN. Electronic Instrumentation DPP-PSD. Rev July Digital Pulse Processing for Pulse Shape Discrimination. User Manual UM2580
Tools for Discovery n Rev 4-21 July 2014 User Manual UM2580 DPP-PSD Digital Pulse Processing for Pulse Shape Discrimination Rev 8 - September 29th, 2016 Purpose of this Manual This User Manual contains
More informationOctal ASD Certification Tests at Michigan
Octal ASD Certification Tests at Michigan J. Chapman, Tiesheng Dai, & Tuan Bui August 30, 2002 - CERN Goals of Michigan Test Confirm actual deadtime vrs setting. Hits/event vrs trigger rate (I/O traffic
More informationSoftware Requirements Specification for LLRF Applications at FLASH Version 1.0 Prepared by Zheqiao Geng MSK, DESY Nov. 06, 2009
Software Specification for LLRF Applications at FLASH Version 1.0 Prepared by Zheqiao Geng MSK, DESY Nov. 06, 2009 Copyright 2009 by Zheqiao Geng. Any change of this document should be agreed by the development
More informationData Compression and Analysis Methods for High- Throughput Radiation Detector Systems
1 Data Compression and Analysis Methods for High- Throughput Radiation Detector Systems John Mattingly Associate Professor, Nuclear Engineering North Carolina State University 2 Introduction The capabilities
More informationChapter 7: From Digital-to-Analog and Back Again
Chapter 7: From Digital-to-Analog and Back Again Overview Often the information you want to capture in an experiment originates in the laboratory as an analog voltage or a current. Sometimes you want to
More informationGFT Channel Digital Delay Generator
Features 20 independent delay Channels 100 ps resolution 25 ps rms jitter 10 second range Output pulse up to 6 V/50 Ω Independent trigger for every channel Four triggers Three are repetitive from three
More informationThe LZ Program. Bob Jacobsen UCLA Dark Matter 2012 For the LZ Collaboration
The LZ Program Bob Jacobsen UCLA Dark Matter 2012 For the LZ Collaboration 1 The LUX Collabora.on Brown Richard Gaitskell Simon Fiorucci Research Associate Monica Pangilinan Jeremy Chapman Carlos Hernandez
More informationAn ASIC dedicated to the RPCs front-end. of the dimuon arm trigger in the ALICE experiment.
An ASIC dedicated to the RPCs front-end of the dimuon arm trigger in the ALICE experiment. L. Royer, G. Bohner, J. Lecoq for the ALICE collaboration Laboratoire de Physique Corpusculaire de Clermont-Ferrand
More informationnanomca datasheet I. FEATURES
datasheet nanomca I. FEATURES Finger-sized, high performance digital MCA. 16k channels utilizing smart spectrum-size technology -- all spectra are recorded and stored as 16k spectra with instant, distortion-free
More informationnanomca 80 MHz HIGH PERFORMANCE, LOW POWER DIGITAL MCA Model Numbers: NM0530 and NM0530Z
datasheet nanomca 80 MHz HIGH PERFORMANCE, LOW POWER DIGITAL MCA Model Numbers: NM0530 and NM0530Z I. FEATURES Finger-sized, high performance digital MCA. 16k channels utilizing smart spectrum-size technology
More informationOn the initiation of lightning in thunderclouds (Instrumentation, Supplementary information)
On the initiation of lightning in thunderclouds (Instrumentation, Supplementary information) Ashot Chilingarian 1,2, Suren Chilingaryan 1, Tigran Karapetyan 1, Lev Kozliner 1, Yeghia Khanikyants 1, Gagik
More informationTechnical Information Manual
Technical Information Manual Revision n. 5 25 November 2002 MOD. N840-N841 8-16 CHANNEL LEADING EDGE DISCRIMINATOR NPO: 00103/00:840-1.MUTx/05 CAEN will repair or replace any product within the guarantee
More informationThe electronics and data acquisition systems of a CsI(Tl) scintillating crystal detector for low energy neutrino experiment
Nuclear Instruments and Methods in Physics Research A 465 (2001) 550 565 The electronics and data acquisition systems of a CsI(Tl) scintillating crystal detector for low energy neutrino experiment W.P.
More informationTechnical Information Manual
Technical Information Manual Revision n. 0 21 April 1999 MOD. N 145 QUAD SCALER AND PRESET COUNTER/TIMER User's Manual (MUT) Mod. N145 Quad Scaler and Preset Counter/Timer Quad Scaler 20/04/1999 0 and
More informationModels 296 and 295 combine sophisticated
Established 1981 Advanced Test Equipment Rentals www.atecorp.com 800-404-ATEC (2832) Models 296 and 295 50 MS/s Synthesized Multichannel Arbitrary Waveform Generators Up to 4 Independent Channels 10 Standard
More information2520 Pulsed Laser Diode Test System
Complete pulse test of laser diode bars and chips with dual photocurrent measurement channels 0 Pulsed Laser Diode Test System Simplifies laser diode L-I-V testing prior to packaging or active temperature
More informationPixel hybrid photon detectors
Pixel hybrid photon detectors for the LHCb-RICH system Ken Wyllie On behalf of the LHCb-RICH group CERN, Geneva, Switzerland 1 Outline of the talk Introduction The LHCb detector The RICH 2 counter Overall
More informationJohn Kelley and Jim Braun UW-Madison September 26, 2005 IceCube Collaboration Meeting London
John Kelley and Jim Braun UW-Madison September 26, 2005 IceCube Collaboration Meeting London Overview Status of DOM-Cal Review of capabilities Recent improvements Transit time calibration Tutorial on use
More informationCommissioning Status and Results of ATLAS Level1 Endcap Muon Trigger System. Yasuyuki Okumura. Nagoya TWEPP 2008
Commissioning Status and Results of ATLAS Level1 Endcap Muon Trigger System Yasuyuki Okumura Nagoya University @ TWEPP 2008 ATLAS Trigger DAQ System Trigger in LHC-ATLAS Experiment 3-Level Trigger System
More informationA Novel Design of a High-Resolution Hodoscope for the Hall D Tagger Based on Scintillating Fibers
A Novel Design of a High-Resolution Hodoscope for the Hall D Tagger Based on Scintillating Fibers APS Division of Nuclear Physics Meeting October 25, 2008 GlueX Photon Spectrum Bremsstrahlung in diamond
More informationCAMAC products. CAEN Short Form Catalog Function Model Description Page
products Function Model Description Page Controller C111C Ethernet Crate Controller 44 Discriminator C808 16 Channel Constant Fraction Discriminator 44 Discriminator C894 16 Channel Leading Edge Discriminator
More informationActivities in Electronics Lab Associates are: Mrs. Arti Gupta, K.S.Golda, S.Muralithar & Dr.R.K.Bhowmik
Activities in Electronics Lab. 2006 Associates are: Mrs. Arti Gupta, K.S.Golda, S.Muralithar & Dr.R.K.Bhowmik Nuclear Electronics (INGA, NAND) Pulse Shape Discriminator Electronics for NAND National Array
More informationMeasuring Voltage and Time Quantities of a Signal Through a Virtual Oscilloscope
AASCIT Journal of Physics 2017; 3(2): 5-12 http://www.aascit.org/journal/physics ISSN: 2381-1358 (Print); ISSN: 2381-1366 (Online) Measuring Voltage and Time Quantities of a Signal Through a G. Tektas
More informationM Hewitson, K Koetter, H Ward. May 20, 2003
A report on DAQ timing for GEO 6 M Hewitson, K Koetter, H Ward May, Introduction The following document describes tests done to try and validate the timing accuracy of GEO s DAQ system. Tests were done
More informationStudy of the ALICE Time of Flight Readout System - AFRO
Study of the ALICE Time of Flight Readout System - AFRO Abstract The ALICE Time of Flight Detector system comprises about 176.000 channels and covers an area of more than 100 m 2. The timing resolution
More informationUse of a Hybrid Photo Detector (HPD) in the MAGIC micro power LIDAR system
Use of a Hybrid Photo Detector (HPD) in the MAGIC micro power LIDAR system Christian Fruck cfruck@ph.tum.de Max-Planck-Institut für Physik LIGHT 11 - Ringberg 03.11.2011 1 / 18 Overview MAGIC uses the
More informationDigitization of PMT signals with FADCs: comparison of simulation and measurement
Digitization of PMT signals with FADCs: comparison of simulation and measurement Arno Gadola General, 10. 12.05.2010 Outline Summary of previous presentations Impact of sampling rate Verification of simulation
More informationGAMMA-RAD5 User Manual
GAMMA-RAD5 User Manual 1 Introduction... 2 1.1 Gamma-Rad5 Description... 2 1.2 DP5 Family... 2 1.3 Options and Variations... 3 2 Specifications... 4 2.1 Spectroscopic Performance... 4 2.2 Processing, physical,
More informationCalorimeter Monitoring at DØ
Calorimeter Monitoring at DØ Calorimeter Monitoring at DØ Robert Kehoe ATLAS Calibration Mtg. December 1, 2004 Southern Methodist University Department of Physics Detector and Electronics Monitoring Levels
More informationSilicon Photomultiplier
Silicon Photomultiplier Operation, Performance & Possible Applications Slawomir Piatek Technical Consultant, Hamamatsu Corp. Introduction Very high intrinsic gain together with minimal excess noise make
More information