Development of Data Acquisition Systems for Gamma Vertex Imaging System for Proton Dose Verification
|
|
- Colin Austin
- 7 years ago
- Views:
Transcription
1 Development of Data Acquisition Systems for Gamma Vertex Imaging System for Proton Dose Verification Han Rim Lee 1, Jong Hoon Park 1, Young-su Kim 1, Won Gyun Jung 2, Chan Hyeong Kim 1 1 Department of Nuclear Engineering, Hanyang University 2 Heavy-ion Clinical Research Division, Korean Institute of Radiological & Medical Sciences 53 rd Annual Conference of the Particle Therapy Co-Operative Group
2 Gamma vertex imaging C. H. Kim, J. H. Park, H. Seo, and H. R. Lee, Med. Phys. vol. 39, no. 10, pp ,
3 Performance estimation with Geant4 simulation Simulation condition Primary particles: Phantom: soft tissue (30 cm 30 cm 40 cm) Incident position(d): 5 cm Energy window: 4-10 MeV Proton energy: 80, 150, 200 MeV Geant4 simulation Proton beam 3
4 Proton beam 4
5 Research objectives Develop the prototype gamma vertex imaging (GVI) system - Electronic read-out system for hodoscope - Electronic read-out system for calorimeter - DAQ and image reconstruction system Test the performance of the prototype system - Energy resolution and V rms of hodoscopes - Energy calibration of calorimeter - 2D image for beta source - 2D image for gamma source - 2D image for 4.4 MeV gamma of Am-Be source 5
6 Hodoscope (double-sided silicon strip detector) Hodoscope Hodoscope e e e Calorimeter Source Electron converter Double-sided silicon strip detector (DSSD) Specification of DSSD - Detector type: W1-type (Micron Semiconductor Ltd., UK) - Active area: 5 5 cm 2 - Strip number: 16 for each side (strip pitch: mm) - Detector thickness: 1 st DSSD (145 μm), 2 nd DSSD (300 μm) - Bias voltage: 20 V (145 μm), 30 V (300 μm) 6
7 Electronic read-out system for hodoscope (DSSD) DSSD signal (16 ch) CSP Slow amplifier Multiplexer Energy DAC Position Fast amplifier LED CR-110 (Cremat Inc., MA) for p-side ev-5094 (ev products, PA) for n-side Primary encoder In-house system 7
8 Development of shaping amplifier Shaping Amplifier Amplify and shape the signals in the form of Gaussian CR differentiator + active filter (2nd-order Sallen-key low pass filter) Shaping time= 100 (for trigger), 250 (for energy) ns, Gain= 10 Circuit design Shaping amplifier Board layout 8
9 Development of multiplexing system Circuit design Multiplexing system Board layout 9
10 Developed electronic read-out system Amplification Shaping amplifier CR-110(P-side) Multiplexing system (P-side) ev-5094(n-side) Multiplexing system (N-side) 10
11 Electronic read-out system for calorimeter (plastic scintillation detector) 1 st DSSD 2 nd DSSD e e e Calorimeter Source Electron converter SCIONIX(NL) Scintillator: EJ200 (thickness: 2cm, Eljen technology) Photomultiplier (9102, ET Enterprises Ltd) - Quantum eff. : 400 nm - Gain: V Voltage divider Preamplifier (AMP-1000 Preamplifier) - Pulse fall time: ~ 50 µs - Maximum signal height: ±10 V Amplifier (in-house shaper, 250 ns) 11
12 Developed prototype imaging system Beryllium converter 1 st DSSD Electronic readout system for DSSD 2 nd DSSD Plastic scintillation detector 12
13 DAQ and image reconstruction system PXI based data acquisition system Data analysis and image reconstruction system 1. Digitizer control and data acquisition 2. Determination of energy and time Controller (PXIe-8133) - Inter Core I7-820QM quad-core processor (1.73 GHz) Chassis (PXIe-1082) Digitizer (PXI-5105) - Input number: 8 channel - Sampling rate: 60 MS/s per channel - Input range: ±25 mv - ±15 V - Resolution: 12-bit 3. Check time and energy window 4. Image reconstruction 13
14 Test results 14
15 Performance test: energy resolution of hodoscopes 241 Am (59.5 kev) 57 Co (122 kev) First DSSD (145 μm) P-side Energy resolution of hodoscopes (DSSD) - First DSSD P-side: 28.8% ± 0.20%p (59.5 kev), 13.3% ± 0.12%p (122 kev) - First DSSD N-side: 30.8% ± 0.27%p (59.5 kev), 14.0% ± 0.22%p (122 kev) - Second DSSD P-side: 20.6% ± 0.15%p (59.5 kev), 8.9% ± 0.08%p (122 kev) - Second DSSD N-side: 25.2% ± 0.22%p (59.5 kev), 11.0% ± 0.17%p (122 kev) 15
16 Performance test: V rms of DSSD First DSSD (145 μm) P-side V rms (V) V rms (kev) N-side V rms (V) V rms (kev) Second DSSD (300 μm) P-side V rms (V) V rms (kev) N-side V rms (V) V rms (kev) ± 0.44 kev 4.05 ± 0.48 kev 4.49 ± 0.17 kev 5.73 ± 0.20 kev Minimum energy deposition of Compton electron to DSSD - First DSSD: kev - Second DSSD: kev 16
17 Energy calibration using Compton edges Y(channel) = 0.84 X(energy) Adj. R-square =
18 Test results for beta source 18
19 2D image for beta point source 90 Sr (Beta, and MeV) Position: 1.8 mm, -3.5 mm Original position (2.0 mm, -3.5 mm) FWHM: 17.8 mm Converter: none Source to 1 st DSSD distance: 26.5 mm Source activity: 0.9 µci Measurement time: 30 min Energy threshold: 1 MeV 19
20 2D image for beta point source 90 Sr (Beta, and MeV) Position: 16.9 mm, mm Original position (17.0 mm, mm) FWHM: 19.4 mm Converter: none Source to 1 st DSSD distance: 26.5 mm Source activity: 0.9 µci Measurement time: 30 min Energy threshold: 1 MeV 20
21 2D image for beta point source 90 Sr (Beta, and MeV) Position: 0.5 mm, mm Original position (0.0 mm, mm) FWHM: 18.6 mm Converter: none Source to 1 st DSSD distance: 26.5 mm Source activity: 0.9 µci Measurement time: 30 min Energy threshold: 1 MeV 21
22 Test results for gamma source 22
23 2D image for gamma point source 60 Co (gamma, and MeV) Position: -0.9 mm, -1.4 mm Original position (-1.0 mm, -1.5 mm) FWHM: 34.7 mm Converter: Be 1.08 mm Source to 1 st DSSD distance: 30 mm Source activity: 4.2 µci Measurement time: 30 min Energy threshold: 0.1 MeV 23
24 2D image for gamma point source 60 Co (gamma, and MeV) Position: mm, mm Original position (-18.0 mm, mm) FWHM: 35.1 mm Converter: Be 1.08 mm Source to 1 st DSSD distance: 30 mm Source activity: 4.2 µci Measurement time: 30 min Energy threshold: 0.1 MeV 24
25 2D image for gamma point source 60 Co (gamma, and MeV) Position: -2.4 mm, mm Original position (-2.5 mm, mm) FWHM: 33.8 mm Converter: Be 1.08 mm Source to 1 st DSSD distance: 30 mm Source activity: 4.2 µci Measurement time: 30 min Energy threshold: 0.1 MeV 25
26 Test results for high energy gamma source 26
27 2D image for high energy gammas Am-Be source (Gamma, 4.44 MeV) Converter: Be 1.08 mm Source to 1 st DSSD distance: 45 mm Source cup: 2.54 cm(outer diameter), 3.81 (length) Source activity (4.44 MeV): µci Measurement time: 30 min Energy threshold: 1.5 MeV 27
28 2D image for high energy gammas Am-Be source (Gamma, 4.44 MeV) Converter: Be 1.08 mm Source to 1 st DSSD distance: 45 mm Source cup: 2.54 cm(outer diameter), 3.81 (length) Source activity (4.44 MeV): µci Measurement time: 30 min Energy threshold: 1.5 MeV 28
29 2D image for high energy gammas Am-Be source (Gamma, 4.44 MeV) Converter: Be 1.08 mm Source to 1 st DSSD distance: 45 mm Source cup: 2.54 cm(outer diameter), 3.81 (length) Source activity (4.44 MeV): µci Measurement time: 30 min Energy threshold: 1.5 MeV 29
30 Conclusion In the present study, the prototype gamma vertex imaging (GVI) system was constructed and tested. The developed prototype imaging system shows satisfactory results for electron and gamma sources. The experiments using the therapeutic proton beams will be performed in a near future. 30
31 Thank you for your attention
Proton tracking for medical imaging and dosimetry
Proton tracking for medical imaging and dosimetry J.Taylor, P.Allport, G.Casse For the PRaVDA Consortium 1 Background and motivation - What is the PRaVDA experiment? - Why are we using Monte Carlo? GEANT4
More informationInformation about the T9 beam line and experimental facilities
Information about the T9 beam line and experimental facilities The incoming proton beam from the PS accelerator impinges on the North target and thus produces the particles for the T9 beam line. The collisions
More informationSPADIC: CBM TRD Readout ASIC
SPADIC: CBM TRD Readout ASIC Tim Armbruster tim.armbruster@ziti.uni-heidelberg.de HIC for FAIR, Darmstadt Schaltungstechnik Schaltungstechnik und und February 2011 Visit http://spadic.uni-hd.de 1. Introduction
More informationElectronics GRETINA Project
Electronics GRETINA Project Requirement Document Sergio Zimmermann July 24, 2004 ANL Electronics Workshop, Schedule 1 Outline Doc Data Base Justification Document types Functional requirements List of
More informationElectron-Muon Ranger (EMR)
Electron-Muon Ranger (EMR) Digitization and Reconstruction François Drielsma Ruslan Asfandiyarov University of Geneva On Behalf of the EMR Group 38 th MICE Collaboration Meeting February 23, 2014 Electron-Muon
More informationResults from first tests of TRD prototypes for CBM. DPG Frühjahrstagung Münster 2011 Pascal Dillenseger Institut für Kernphysik Frankfurt am Main
Results from first tests of TRD prototypes for CBM DPG Frühjahrstagung Münster 2011 Pascal Dillenseger Institut für Kernphysik Contents Overview of the CBM experiment CBM-TRD General TRD requirements The
More informationStatus and perspective of emission imaging techniques for ion beam therapy in Lyon
14th International Conference on Nuclear Reaction Mechanisms, Varenna 18th June 2015 Status and perspective of emission imaging techniques for ion beam therapy in Lyon on behalf of the CAS-PHABIO group
More informationExperimental study of beam hardening artefacts in photon counting breast computed tomography
Experimental study of beam hardening artefacts in photon counting breast computed tomography M.G. Bisogni a, A. Del Guerra a,n. Lanconelli b, A. Lauria c, G. Mettivier c, M.C. Montesi c, D. Panetta a,
More informationNeutron Detection Setups proposed for
Neutron Detection Setups proposed for DESPEC D. Cano-Ott on behalf of the WG members CIEMAT, IFIC, LNL, FYL, UPC, UU, UW Motivation GOAL: to measure neutron emission probabilities and energies for neutron
More informationRadiation Strip Thickness Measurement Systems
Radiation Strip Thickness Measurement Systems During the past years we have increased our sales of radiometric Vollmer strip thickness measurement systems, i.e. X-ray or isotope gauges, dramatically. Now,
More informationAn option for the SHiP Muon Detector: Scintillator bars with WLS fibers and SiPMs readout
An option for the SHiP Muon Detector: Scintillator bars with WLS fibers and SiPMs readout M. Anelli, W. Baldini, P. Ciambrone, M. Dallavalle, F. Fabbri, G. Lanfranchi, A. Montanari INFN-LNF, INFN-Ferrara,
More informationTrack Trigger and Modules For the HLT
CMS L1 Track Trigger for SLHC Anders Ryd for the CMS Track Trigger Task Force Vertex 2009 Sept. 13-18, 2009 L=1035 cm-2s-1 Outline: SLHC trigger challenge Tracking triggers Track trigger modules Simulation
More informationThe accurate calibration of all detectors is crucial for the subsequent data
Chapter 4 Calibration The accurate calibration of all detectors is crucial for the subsequent data analysis. The stability of the gain and offset for energy and time calibration of all detectors involved
More informationRadiation Detection and Measurement
Radiation Detection and Measurement June 2008 Tom Lewellen Tkldog@u.washington.edu Types of radiation relevant to Nuclear Medicine Particle Symbol Mass (MeV/c 2 ) Charge Electron e-,! - 0.511-1 Positron
More informationGRETA. I-Yang Lee. For the GRETA Steering Committee. Workshop on the Experimental Equipment for RIA March 18-22, 2003, Oak Ridge, Tennessee
GRETA I-Yang Lee For the GRETA Steering Committee Workshop on the Experimental Equipment for RIA March 18-22, 2003, Oak Ridge, Tennessee Gamma-ray Tracking Concepts Compton Suppressed Ge Veto Ν det = 100
More informationMars Atmosphere and Volatile EvolutioN (MAVEN) Mission
Mars Atmosphere and Volatile EvolutioN (MAVEN) Mission MAVEN Science Community Workshop December 2, 2012 Particles and Fields Package Solar Energetic Particle Instrument (SEP) Davin Larson and the SEP
More informationCMS Tracker module / hybrid tests and DAQ development for the HL-LHC
CMS Tracker module / hybrid tests and DAQ development for the HL-LHC S. Mersi, G. Auzinger georg.auzinger@cern.ch 1 Outline Reminder: the Ph2 CMS Tracker upgrade pt Modules: principle, elements, electronics
More informationHow To Make Hard Xray Pixel Detectors For Hard X-Ray Astrophysics
Development of Focal Plane Detectors for the Nuclear Spectroscopic Telescope Array (NuSTAR) Mission Vikram R. Rana a, Walter R. Cook III a, Fiona A. Harrison a, Peter H. Mao a, Hiromasa Miyasaka a a Space
More informationShort overview of TEUFEL-project
Short overview of TEUFEL-project ELAN-meeting may 2004 Frascati (I) Contents Overview of TEUFEL project at Twente Photo cathode research Recent experience Outlook Overview FEL Drive laser Photo cathode
More informationElectron-Muon Ranger (EMR)
Electron-Muon Ranger (EMR) Ruslan Asfandiyarov MICE Video Conference April 11, 2013 Construction Construction quarter of the detector completed (12 planes) every plane tested (LED / Camera / image analysis)
More informationDevelopment of on line monitor detectors used for clinical routine in proton and ion therapy
Development of on line monitor detectors used for clinical routine in proton and ion therapy A. Ansarinejad Torino, february 8 th, 2010 Overview Hadrontherapy CNAO Project Monitor system: Part1:preliminary
More informationA Polarimetry concept for the EDM experiment at COSY
A Polarimetry concept for the EDM experiment at COSY Paul Maanen JEDI Collaboration Physics Institute III B, RWTH Aachen University DPG Frühjahrstagung March 27, 2015 Outline Introduction Detector concept
More informationActivitity (of a radioisotope): The number of nuclei in a sample undergoing radioactive decay in each second. It is commonly expressed in curies
Activitity (of a radioisotope): The number of nuclei in a sample undergoing radioactive decay in each second. It is commonly expressed in curies (Ci), where 1 Ci = 3.7x10 10 disintegrations per second.
More informationACCELERATORS AND MEDICAL PHYSICS 2
ACCELERATORS AND MEDICAL PHYSICS 2 Ugo Amaldi University of Milano Bicocca and TERA Foundation EPFL 2-28.10.10 - U. Amaldi 1 The icone of radiation therapy Radiation beam in matter EPFL 2-28.10.10 - U.
More informationISTITUTO NAZIONALE DI FISICA NUCLEARE
ISTITUTO NAZIONALE DI FISICA NUCLEARE Sezione di Catania INFN/TC-11/02 February 28, 2011 PRELIMINARY TESTS OF A SCINTILLATOR-BASED MINI-STATION FOR EXTENSIVE AIR SHOWERS MEASUREMENTS S.Aiola 1, P. La Rocca
More informationStatus of CBM-XYTER Development
Status of CBM-XYTER Development Latest Results of the CSA/ADC Test-Chip Tim Armbruster tim.armbruster@ziti.uni-heidelberg.de Heidelberg University Schaltungstechnik Schaltungstechnik und und 14th CBM CM
More informationGamma Rays OBJECT: READINGS: APPARATUS: BACKGROUND:
Gamma Rays OBJECT: To understand the various interactions of gamma rays with matter. To calibrate a gamma ray scintillation spectrometer, using gamma rays of known energy, and use it to measure the energy
More informationSolid State Detectors = Semi-Conductor based Detectors
Solid State Detectors = Semi-Conductor based Detectors Materials and their properties Energy bands and electronic structure Charge transport and conductivity Boundaries: the p-n junction Charge collection
More informationMICE detectors and first results. M. Bonesini Sezione INFN Milano Bicocca
MICE detectors and first results M. Bonesini Sezione INFN Milano Bicocca I will speak of the installed beamline PID detectors (TOFes, CKOVs, KL) and only shortly of EMR (to be built)/ the trackers (tested
More informationAtomic and Nuclear Physics Laboratory (Physics 4780)
Gamma Ray Spectroscopy Week of September 27, 2010 Atomic and Nuclear Physics Laboratory (Physics 4780) The University of Toledo Instructor: Randy Ellingson Gamma Ray Production: Co 60 60 60 27Co28Ni *
More informationThe data acquisition system of the XMASS experiment
The data acquisition system of the XMASS experiment Katsuki Hiraide 1,2, for the XMASS Collaboration 1 Kamioka Observatory, Institute for Cosmic Ray Research, the University of Tokyo, Higashi-Mozumi, Kamioka,
More informationFeasibility Study of Neutron Dose for Real Time Image Guided. Proton Therapy: A Monte Carlo Study
Feasibility Study of Neutron Dose for Real Time Image Guided Proton Therapy: A Monte Carlo Study Jin Sung Kim, Jung Suk Shin, Daehyun Kim, EunHyuk Shin, Kwangzoo Chung, Sungkoo Cho, Sung Hwan Ahn, Sanggyu
More informationMonte Carlo Simulations in Proton Dosimetry with Geant4
Monte Carlo Simulations in Proton Dosimetry with Geant4 Zdenek Moravek, Ludwig Bogner Klinik und Poliklinik für Strahlentherapie Universität Regensburg Objectives of the Study what particles and how much
More informationMODELING AND IMPLEMENTATION OF THE MECHANICAL SYSTEM AND CONTROL OF A CT WITH LOW ENERGY PROTON BEAM
MODELING AND IMPLEMENTATION OF THE MECHANICAL SYSTEM AND CONTROL OF A CT WITH LOW ENERGY PROTON BEAM João Antônio Palma Setti, j.setti@pucpr.br Pontifícia Universidade Católica do Paraná / Rua Imaculada
More informationDose enhancement near metal electrodes in diamond X- ray detectors. A. Lohstroh*, and D. Alamoudi
Dose enhancement near metal electrodes in diamond X- ray detectors Acknowledgements Surrey University: P.J. Sellin M. Abd-El Rahman P. Veeramani H. Al-Barakaty F. Schirru Mechanical Workshop A. Lohstroh*,
More informationSingle Electron Detection with the Large Volume Spherical Proportional Counter Ilias Savvidis
Single Electron Detection with the Large Volume Spherical Proportional Counter Ilias Savvidis Collaboration S. Andriamonje, S. Aune, E. Bougamont, M. Chapelier, P. Colas, J. Derré, E. Ferrer, G. Gerbier,
More informationGamma and X-Ray Detection
Gamma and X-Ray Detection DETECTOR OVERVIEW The kinds of detectors commonly used can be categorized as: a. Gas-filled Detectors b. Scintillation Detectors c. Semiconductor Detectors The choice of a particular
More informationPrecision Tracking Test Beams at the DESY-II Synchrotron. Simon Spannagel DPG 2014 T88.7 Mainz, 26.3.2014
Precision Tracking Test Beams at the DESY-II Synchrotron. Simon Spannagel DPG 2014 T88.7 Mainz, 26.3.2014 Overview > Test Beams at DESY-II > Tracking with the DATURA Telescope Telescope Hardware Software
More informationPLAS: Analog memory ASIC Conceptual design & development status
PLAS: Analog memory ASIC Conceptual design & development status Ramón J. Aliaga Instituto de Física Corpuscular (IFIC) Consejo Superior de Investigaciones Científicas (CSIC) Universidad de Valencia Vicente
More informationTesting thermo-acoustic sound generation in water with proton and laser beams
International ARENA Workshop DESY, Zeuthen 17th 19th of May 25 Testing thermo-acoustic sound generation in water with proton and laser beams Kay Graf Universität Erlangen-Nürnberg Physikalisches Institut
More informationCyclotron Centre in Poland and 2D thermoluminescence dosimetry
Cyclotron Centre in Poland and 2D thermoluminescence dosimetry Jan Gajewski Institute of Nuclear Physics, Kraków, Poland Department of Radiation Dosimetry Nuclear Physics Institute Academy of Science of
More informationIndirect X-ray photon counting image sensor with 27T pixels and 15 electrons RMS accurate threshold
Indirect X-ray photon counting image sensor with 27T pixels and 15 electrons RMS accurate threshold B. Dierickx 1,2, B. Dupont 1,3, A. Defernez 1, N. Ahmed 1 1 Caeleste, Antwerp, Belgium 2 Vrije Universiteit
More informationComparisons between 2003 CMS ECAL TB data and a Geant 4 MC
Comparisons between 2003 CMS CAL TB data and a Geant 4 MC P. Meridiani LCG Validation Meeting 7 th July 2004 Outline CMS lectromagnetic calorimeter and 2003 TB h4sim http://cmsdoc.cern.ch/~h4sim/ (What
More informationThe Timing Counter of the MEG experiment: calibration and performances
The Timing Counter of the MEG experiment: calibration and performances INFN Pavia On behalf of MEG TC group 12th seminar on IPRD Siena 1 MEG: signal and background background signal µ e γ physical e +
More informationCHAPTER 7 SCINTILLATION COUNTING
CHAPTER 7 SCINTILLATION COUNTING Radiation of various types is widely utilized for non-destructive inspection and testing such as in medical diagnosis, industrial inspection, material analysis and other
More informationT(CR)3IC Testbed for Coherent Radio Cherenkov Radiation from Cosmic-Ray Induced Cascades
T(CR)3IC Testbed for Coherent Radio Cherenkov Radiation from Cosmic-Ray Induced Cascades R. Milinčić1, P. Gorham1, C. Hebert1, S. Matsuno1, P. Miočinović1, M. Rosen1, D. Saltzberg2, G. Varner1 1 University
More informationElectronics, Data Acquisition and Trigger - Introduction -
Physik-Institut Exerimental Methods in Particle Physics (HS 2015) Electronics, Data Acquisition and Trigger - Introduction - Lea Caminada lea.caminada@hysik.uzh.ch Lecture Program This week: Electronics
More informationGAMMA-RAY SPECTRA REFERENCES
GAMMA-RAY SPECTRA REFERENCES 1. K. Siegbahn, Alpha, Beta and Gamma-Ray Spectroscopy, Vol. I, particularly Chapts. 5, 8A. 2. Nucleonics Data Sheets, Nos. 1-45 (available from the Resource Centre) 3. H.E.
More informationSilicon Drift Detector Product Brochure Update 2013
Silicon Drift Detector Product Brochure Update 2013 Content Classic Silicon Drift Detector High Resolution Silicon Drift Detector Multielement Silicon Detector Extra Large Detector Series July 2013 About
More information(Amplifying) Photo Detectors: Avalanche Photodiodes Silicon Photomultiplier
(Amplifying) Photo Detectors: Avalanche Photodiodes Silicon Photomultiplier (no PiN and pinned Diodes) Peter Fischer P. Fischer, ziti, Uni Heidelberg, Seite 1 Overview Reminder: Classical Photomultiplier
More informationENERGY LOSS OF ALPHA PARTICLES IN GASES
Vilnius University Faculty of Physics Department of Solid State Electronics Laboratory of Applied Nuclear Physics Experiment No. ENERGY LOSS OF ALPHA PARTICLES IN GASES by Andrius Poškus (e-mail: andrius.poskus@ff.vu.lt)
More informationDevelopment of the electromagnetic calorimeter waveform digitizers for the Fermilab Muon g-2 experiment
Development of the electromagnetic calorimeter waveform digitizers for the Fermilab g-2 experiment 1 on behalf of the Fermilab E989 g-2 Collaboration European Physical Society Conference on High Energy
More informationNuclear Weapons and Material Security (WMS) Team Program Review WMS2013
Office of Research & Development Nuclear Weapons and Material Security (WMS) Team Program Review WMS2013 Array of Virtual Frisch-Grid CZT Detectors with Common Cathode Readout for Correcting Charge Trapping
More informationX- and Gamma Ray Imaging Systems based on CdTe-CMOS Detector Technology
X- and Gamma Ray Imaging Systems based on dte-mos Detector Technology Konstantinos Spartiotis, Ray Durrant, nssi Leppänen, Henrik Lohman, Olli Männistö, Tuomas Pantsar, Jouni Pyyhtiä, Tom Schulman, Oy
More informationElectron-Muon Ranger (EMR)
Electron-Muon Ranger (EMR) Status of EMR Project R.Asfandiyarov 1, P.Béné 1, R.Bloch 1, A.Blondel 1, D.Bolognini 3 F.Cadoux 1, S.Débieux 1, J-S.Graulich 1, C.Husi 1, D.Lietti 3, F.Masciocchi 1, L.Nicola
More informationFiber Optics. Integrated Photo Detector Receiver for Plastic Fiber Plastic Connector Housing SFH551/1-1 SFH551/1-1V
Fiber Optics Integrated Photo Detector Receiver for Plastic Fiber Plastic Connector Housing SFH551/1-1 Features Bipolar IC with open-collector output Digital output, TTL compatible Sensitive in visible
More informationElectron Muon Ranger (EMR) Software Development
Electron Muon Ranger (EMR) Software Development François Drielsma on behalf of the EMR Group University of Geneva June 25, 2014 François Drielsma on behalf of the EMR Group Electron (University Muon of
More informationAMPLIFIED HIGH SPEED FIBER PHOTODETECTOR USER S GUIDE
AMPLIFIED HIGH SPEED FIBER PHOTODETECTOR USER S GUIDE Thank you for purchasing your Amplified High Speed Fiber Photodetector. This user s guide will help answer any questions you may have regarding the
More informationSilicon Sensors for CMS Tracker at High-Luminosity Environment - Challenges in particle detection -
timo.peltola@helsinki.fi Finnish Society for Natural Philosophy, Helsinki, 17 February 2015 Silicon Sensors for CMS Tracker at High-Luminosity Environment - Challenges in particle detection - Timo Peltola
More informationATLAS Tile Calorimeter Readout Electronics Upgrade Program for the High Luminosity LHC
ATLAS Tile Calorimeter Readout Electronics Upgrade Program for the High Luminosity LHC Augusto Santiago Cerqueira On behalf of the ATLAS Tile Calorimeter Group Federal University of Juiz de Fora, Brazil
More informationUse of the VALIDATOR Dosimetry System for Quality Assurance and Quality Control of Blood Irradiators
Technical Note: 9 Use of the VALIDATOR Dosimetry System for Quality Assurance and Quality Control of Blood Irradiators 1- Introduction The VALIDATOR, model TN-ID-60, is a compact, and stand-alone dosimetry
More informationLarge Hadron Collider am CERN
The CMS Silicon Tracker Lutz Feld 1. Physikalisches Institut, RWTH Aachen GSI Darmstadt, 18. 4. 2007 Large Hadron Collider am CERN proton proton quarks & gluons circumference 27 km 1200 superconducting
More informationCELL CYCLE BASICS. G0/1 = 1X S Phase G2/M = 2X DYE FLUORESCENCE
CELL CYCLE BASICS Analysis of a population of cells replication state can be achieved by fluorescence labeling of the nuclei of cells in suspension and then analyzing the fluorescence properties of each
More informationA receiver TDC chip set for accurate pulsed time-of-flight laser ranging
A receiver TDC chip set for accurate pulsed time-of-flight laser ranging Juha Kostamovaara, Sami Kurtti, Jussi-Pekka Jansson University of Oulu, Department of Electrical Engineering, Electronics Laboratory,
More informationIMPROVEMENT OF JET ENERGY RESOLUTION FOR SEGMENTED HCAL USING LAYER WEIGHTING TECHNIQUE
IMPROVEMEN OF JE ENERGY RESOLUION FOR SEGMENED HCAL USING LAYER WEIGHING ECHNIQUE V. Andreev 1, I. Golutvin 2, A. Nikitenko 3,V.Palichik 2 1 Lebedev Physical Institute, Moscow, Russia 2 Joint Institute
More informationThe Mainz LXe TPC MC simulations for a Compton scattering experiment
The Mainz LXe TPC MC simulations for a Compton scattering experiment Pierre Sissol Johannes Gutenberg Universität Mainz 12 November 2012 1 / 24 Outline 1 Dark Matter 2 Principle of a dual-phase LXe TPC
More informationCharacterisation of the Timepix Chip for the LHCb VELO Upgrade
Particle and Astroparticle Physics Master Thesis Characterisation of the Timepix Chip for the LHCb VELO Upgrade Veerle Heijne Supervisor: Dr. Martin van Beuzekom Second reviewer: Dr. Auke-Pieter Colijn
More informationCMS Tracking Performance Results from early LHC Running
CMS Tracking Performance Results from early LHC Running CMS PAPER TRK-10-001 L. Spiegel, K. Stenson, M. Swartz 1 First Collisions Tracking Paper Provide description of tracker, tracking algorithm, and
More informationORTEC AN34 Experiment 7 High-Resolution Gamma-Ray Spectroscopy
Equipment Needed from ORTEC GEM10P4/CFG-PV4/DWR-30 Coaxial Detector System (Includes detector, cryostat, dewar, preamplifier, and 12-ft. cable pack); typical specifications: 10% relative efficiency, 1.75
More informationEvaluation Tools for the Performance of a NESTOR Test Detector
Evaluation Tools for the Performance of a NESTOR Test Detector G. Bourlis, A. Leisos, S. E. Tzamarias and A. Tsirigotis Particle and Astroparticle Physics Group School of Science and Technology Hellenic
More informationPixie Viewer Online Help
Getting Help for the Pixie Viewer There are several ways to get help for the Pixie Viewer. You can use IGOR's built-in help browser to access the Pixie Viewer specific help file by selecting Help -> Help
More informationOptical Link ASICs for LHC Upgrades
Optical Link ASICs for LHC Upgrades K.K. Gan, H.P. Kagan, R.D. Kass, J. Moore, S. Smith The Ohio State University July 30, 2009 K.K. Gan DPF2009 1 Outline Introduction VCSEL driver chip PIN receiver/decoder
More informationThe Muon Veto DAQ. Florian Ritter. Kepler Center for Astro and Particle Physics. Eberhard Karls Universität Tübingen
The Muon Veto DAQ Florian Ritter Kepler Center for Astro and Particle Physics Eberhard Karls Universität Tübingen Outline Muon Veto Facts I Summary and Outlook Muon Veto Facts plastic scintillator photomultiplier
More information3D SCANNERTM. 3D Scanning Comes Full Circle. s u n. Your Most Valuable QA and Dosimetry Tools A / B / C. The 3D SCANNER Advantage
3D SCANNERTM 3D Scanning Comes Full Circle Relative 3D Dosimetry offering the easiest setup, most objectivity, and best consistency available The 3D SCANNER Advantage Advanced Design Ring and diameter
More informationPerformance Comparison of Four Commercial GE Discovery PET/CT Scanners: A Monte Carlo Study Using GATE
Performance Comparison of Four Commercial GE Discovery PET/CT Scanners: A Monte Carlo Study Using Parham Geramifar 1,3,4, Mohammad Reza Ay 2,3,4, Mojtaba Shamsaie Zafarghandi 1, George Loudos 5, Arman
More informationDesign and performance of the ABCD chip for the binary readout of silicon strip detectors in the ATLAS Semiconductor Tracker
EEE TRANSACTONS ON NUCLEAR SCENCE, VOL. 47, NO. G, DECEMBER 2000 1843 Design and performance of the ABCD chip for the binary readout of silicon strip detectors in the ATLAS Semiconductor Tracker W. Dabrowski',
More informationReconfigurable System-on-Chip Design
Reconfigurable System-on-Chip Design MITCHELL MYJAK Senior Research Engineer Pacific Northwest National Laboratory PNNL-SA-93202 31 January 2013 1 About Me Biography BSEE, University of Portland, 2002
More informationA PC-BASED TIME INTERVAL COUNTER WITH 200 PS RESOLUTION
35'th Annual Precise Time and Time Interval (PTTI) Systems and Applications Meeting San Diego, December 2-4, 2003 A PC-BASED TIME INTERVAL COUNTER WITH 200 PS RESOLUTION Józef Kalisz and Ryszard Szplet
More informationPassive Whole Body Monitoring Nuclear Power Industry Application Introduction to the Argos -5AB Zeus (Gamma Option) and the GEM
Application Note Passive Whole Body Monitoring Nuclear Power Industry Application Introduction to the Argos -5AB Zeus (Gamma Option) and the GEM -5 Gamma Exit Monitor CANBERRA s personnel contamination
More informationAN INVESTIGATION INTO THE USEFULNESS OF THE ISOCS MATHEMATICAL EFFICIENCY CALIBRATION FOR LARGE RECTANGULAR 3 x5 x16 NAI DETECTORS
AN INVESTIGATION INTO THE USEFULNESS OF THE ISOCS MATHEMATICAL EFFICIENCY CALIBRATION FOR LARGE RECTANGULAR 3 x5 x16 NAI DETECTORS Frazier L. Bronson CHP Canberra Industries, Inc. 800 Research Parkway,
More informationA.Besson, IPHC-Strasbourg
DIGMAPS: a standalone tool to study digitization an overview of a digitizer strategy for CMOS/MAPS sensors A.Besson, IPHC-Strasbourg thanks to A.Geromitsos and J.Baudot Motivations for a CMOS sensor digitizer,
More informationPerformance of Silicon N-in-P Pixel Detectors Irradiated up to 5 1015 neq /cm2 for Future ATLAS Upgrades
Performance of Silicon N-in-P Pixel Detectors Irradiated up to 5 1 neq /cm for Future ATLAS Upgrades Philipp Weigell1 Ch. A. La Rosa3, A. Macchiolo1, R. Nisius1, H. Pernegger3, R.H. Richter Gallrapp3,
More informationCalibration and performance test of the Very Front End electronics for the CMS electromagnetic calorimeter
Calibration and performance test of the Very Front End electronics for the CMS electromagnetic calorimeter Jan Blaha IPN Lyon 10th Topical Seminar on Innovative Particle and Radiation Detectors (IPRD06)
More informationUse of 3D Printers in Proton Therapy
Use of 3D Printers in Proton Therapy Nicholas Remmes, PhD Mayo Clinic, Rochester, MN Department of Radiation Oncology Remmes.Nicholas@mayo.edu 2015 MFMER slide-1 Disclosures/Confessions My 3D Printing
More informationTutorial 4.6 Gamma Spectrum Analysis
Tutorial 4.6 Gamma Spectrum Analysis Slide 1. Gamma Spectrum Analysis In this module, we will apply the concepts that were discussed in Tutorial 4.1, Interactions of Radiation with Matter. Slide 2. Learning
More informationRemote RadEye Product Family
Remote RadEye Product Family Overview The Remote RadEye x-ray camera provides the ultimate flexibility in design and product options for your complex imaging applications. Our unique camera design separates
More informationThe Alice Silicon Pixel Detector Readout System Moving towards system integration. (For the ALICE collaboration)
The Alice Silicon Pixel Detector Readout System Moving towards system integration R.Dinapoli 1, 2, G.Anelli 2, M.Burns 2, M.Campbell 2, P.Chochula 2, A.Kluge 2, M.Morel 2, P. Nilsson 2, P.Riedler 2, G.Stefanini
More informationFebex Data Acquisition System
Febex Data Acquisition System (FPGA Hit Finder and Energy Filter for the FEBEX Pipelining ADC) Dr. Ivan Rusanov for CSEE, GSI - Darmstadt CSEE meeting, GSI 24.02.2014., Darmstadt The Febex Data AcquisitionSystem
More informationTracking systems in HEP:
Tracking systems in HEP: concept and performance of 3 experiments Davide Bolognini Universita' degli Studi dell'insubria Presentazione dottorato Anno I Outline Tracking systems in HEP CMS @ LHC...but not
More informationDevelopment and Experimental Performance Evaluation of a Dose-Rate meter for Pulsed Beam.
5 th International Workshop on Radiation Safety at Synchrotron Radiation Sources Development and Experimental Performance Evaluation of a Dose-Rate meter for Pulsed Beam. A. Vascotto 1, K. Casarin 1, S.
More informationAlgorithms for digital γ-ray spectroscopy
NUKLEONIKA 2013;58(2):333 338 ORIGINAL PAPER Algorithms for digital γ-ray spectroscopy Zbigniew Guik, Tomas Krakowski Abstract. The data processing in modern nuclear spectroscopy is dominated by digital
More informationGLAST Geant4 Simulation
GLAST Geant4 Simulation F.Longo D. Favretto R.Giannitrapani 1 Introduction Simulation effort GammaRayTel advanced example in the Geant4 3.0 release XML - Geant4 visitor Hit class 2 Simulation Effort Design
More informationEncoders for Linear Motors in the Electronics Industry
Technical Information Encoders for Linear Motors in the Electronics Industry The semiconductor industry and automation technology increasingly require more precise and faster machines in order to satisfy
More informationGamma-ray Large Area Space Telescope (GLAST) Large Area Telescope (LAT) Calorimeter AFEE Board Parts Radiation Test Plan
GLAST LAT DESIGN DESCRIPTION Document Title AFEE Board Parts Radiation Test Plan Document # Date Effective LAT-SS-01890-01 1 April 2003 Prepared by(s) Supersedes James Ampe None Subsystem/Office Calorimeter
More informationThinking ahead. Focused on life. REALIZED: GROUNDBREAKING RESOLUTION OF 80 µm VOXEL
Thinking ahead. Focused on life. REALIZED: GROUNDBREAKING RESOLUTION OF 80 µm VOXEL X-ray ZOOM RECONSTRUCTION Flat Panel Detector (FPD) Automatic Positioning Function For ø 40 x H 40 mm, ø 60 x H 60 mm,
More informationFlex Circuits for the ATLAS Pixel Detector
Flex Circuits for the ATLAS Pixel Detector P. Skubic University of Oklahoma Outline ATLAS pixel detector ATLAS prototype Flex hybrid designs Performance simulations Performance measurements Wire bonding
More informationCronos -1 Gamma Object / Tool Monitors
Features Counting chamber volume: 42.9 L (1.5 cu. ft.) Robust, ergonomic, easy-to-use and decontaminate Photon energy range from 50 kev to 2 MeV Four or optional six large surface area plastic scintillator
More information10 is a soft polymer clay that can easily be moulded by hands (S1-Left). The simplest option is to create
Electronic Supplementary Material (ESI) for Lab on a Chip. This journal is The Royal Society of Chemistry 2014 1 Angry pathogens, how to get rid of them: introducing microfluidics for 2 waterborne pathogen
More informationG64 Area Gamma Monitor
Features Solid state detector: range 0.1 µsv/h to 100 msv/h (10 µr/hr 10 R/hr) Pseudo-logarithmic ratemeter averaging for good statistics at low level and fast response at high levels Removable detector
More information