Development of Data Acquisition Systems for Gamma Vertex Imaging System for Proton Dose Verification

Similar documents
Proton tracking for medical imaging and dosimetry

Information about the T9 beam line and experimental facilities

SPADIC: CBM TRD Readout ASIC

Electronics GRETINA Project

Electron-Muon Ranger (EMR)

Results from first tests of TRD prototypes for CBM. DPG Frühjahrstagung Münster 2011 Pascal Dillenseger Institut für Kernphysik Frankfurt am Main

Status and perspective of emission imaging techniques for ion beam therapy in Lyon

Experimental study of beam hardening artefacts in photon counting breast computed tomography

Neutron Detection Setups proposed for

Radiation Strip Thickness Measurement Systems

An option for the SHiP Muon Detector: Scintillator bars with WLS fibers and SiPMs readout

Track Trigger and Modules For the HLT

The accurate calibration of all detectors is crucial for the subsequent data

Radiation Detection and Measurement

GRETA. I-Yang Lee. For the GRETA Steering Committee. Workshop on the Experimental Equipment for RIA March 18-22, 2003, Oak Ridge, Tennessee

Mars Atmosphere and Volatile EvolutioN (MAVEN) Mission

CMS Tracker module / hybrid tests and DAQ development for the HL-LHC

How To Make Hard Xray Pixel Detectors For Hard X-Ray Astrophysics

Short overview of TEUFEL-project

Electron-Muon Ranger (EMR)

Development of on line monitor detectors used for clinical routine in proton and ion therapy

A Polarimetry concept for the EDM experiment at COSY

Activitity (of a radioisotope): The number of nuclei in a sample undergoing radioactive decay in each second. It is commonly expressed in curies

ACCELERATORS AND MEDICAL PHYSICS 2

ISTITUTO NAZIONALE DI FISICA NUCLEARE

Status of CBM-XYTER Development

Gamma Rays OBJECT: READINGS: APPARATUS: BACKGROUND:

Solid State Detectors = Semi-Conductor based Detectors

MICE detectors and first results. M. Bonesini Sezione INFN Milano Bicocca

Atomic and Nuclear Physics Laboratory (Physics 4780)

The data acquisition system of the XMASS experiment

Feasibility Study of Neutron Dose for Real Time Image Guided. Proton Therapy: A Monte Carlo Study

Monte Carlo Simulations in Proton Dosimetry with Geant4

MODELING AND IMPLEMENTATION OF THE MECHANICAL SYSTEM AND CONTROL OF A CT WITH LOW ENERGY PROTON BEAM

Dose enhancement near metal electrodes in diamond X- ray detectors. A. Lohstroh*, and D. Alamoudi

Single Electron Detection with the Large Volume Spherical Proportional Counter Ilias Savvidis

Gamma and X-Ray Detection

Precision Tracking Test Beams at the DESY-II Synchrotron. Simon Spannagel DPG 2014 T88.7 Mainz,

PLAS: Analog memory ASIC Conceptual design & development status

Testing thermo-acoustic sound generation in water with proton and laser beams

Cyclotron Centre in Poland and 2D thermoluminescence dosimetry

Indirect X-ray photon counting image sensor with 27T pixels and 15 electrons RMS accurate threshold

Comparisons between 2003 CMS ECAL TB data and a Geant 4 MC

The Timing Counter of the MEG experiment: calibration and performances

CHAPTER 7 SCINTILLATION COUNTING

T(CR)3IC Testbed for Coherent Radio Cherenkov Radiation from Cosmic-Ray Induced Cascades

Electronics, Data Acquisition and Trigger - Introduction -

GAMMA-RAY SPECTRA REFERENCES

Silicon Drift Detector Product Brochure Update 2013

(Amplifying) Photo Detectors: Avalanche Photodiodes Silicon Photomultiplier

ENERGY LOSS OF ALPHA PARTICLES IN GASES

Development of the electromagnetic calorimeter waveform digitizers for the Fermilab Muon g-2 experiment

Nuclear Weapons and Material Security (WMS) Team Program Review WMS2013

X- and Gamma Ray Imaging Systems based on CdTe-CMOS Detector Technology

Electron-Muon Ranger (EMR)

Fiber Optics. Integrated Photo Detector Receiver for Plastic Fiber Plastic Connector Housing SFH551/1-1 SFH551/1-1V

Electron Muon Ranger (EMR) Software Development

AMPLIFIED HIGH SPEED FIBER PHOTODETECTOR USER S GUIDE

Silicon Sensors for CMS Tracker at High-Luminosity Environment - Challenges in particle detection -

ATLAS Tile Calorimeter Readout Electronics Upgrade Program for the High Luminosity LHC

Use of the VALIDATOR Dosimetry System for Quality Assurance and Quality Control of Blood Irradiators

Large Hadron Collider am CERN

CELL CYCLE BASICS. G0/1 = 1X S Phase G2/M = 2X DYE FLUORESCENCE

A receiver TDC chip set for accurate pulsed time-of-flight laser ranging

IMPROVEMENT OF JET ENERGY RESOLUTION FOR SEGMENTED HCAL USING LAYER WEIGHTING TECHNIQUE

The Mainz LXe TPC MC simulations for a Compton scattering experiment

Characterisation of the Timepix Chip for the LHCb VELO Upgrade

CMS Tracking Performance Results from early LHC Running

ORTEC AN34 Experiment 7 High-Resolution Gamma-Ray Spectroscopy

Evaluation Tools for the Performance of a NESTOR Test Detector

Pixie Viewer Online Help

Optical Link ASICs for LHC Upgrades

The Muon Veto DAQ. Florian Ritter. Kepler Center for Astro and Particle Physics. Eberhard Karls Universität Tübingen

3D SCANNERTM. 3D Scanning Comes Full Circle. s u n. Your Most Valuable QA and Dosimetry Tools A / B / C. The 3D SCANNER Advantage

Performance Comparison of Four Commercial GE Discovery PET/CT Scanners: A Monte Carlo Study Using GATE

Design and performance of the ABCD chip for the binary readout of silicon strip detectors in the ATLAS Semiconductor Tracker

Reconfigurable System-on-Chip Design

A PC-BASED TIME INTERVAL COUNTER WITH 200 PS RESOLUTION

Passive Whole Body Monitoring Nuclear Power Industry Application Introduction to the Argos -5AB Zeus (Gamma Option) and the GEM

AN INVESTIGATION INTO THE USEFULNESS OF THE ISOCS MATHEMATICAL EFFICIENCY CALIBRATION FOR LARGE RECTANGULAR 3 x5 x16 NAI DETECTORS

A.Besson, IPHC-Strasbourg

Performance of Silicon N-in-P Pixel Detectors Irradiated up to neq /cm2 for Future ATLAS Upgrades

Calibration and performance test of the Very Front End electronics for the CMS electromagnetic calorimeter

Use of 3D Printers in Proton Therapy

Tutorial 4.6 Gamma Spectrum Analysis

Remote RadEye Product Family

The Alice Silicon Pixel Detector Readout System Moving towards system integration. (For the ALICE collaboration)

Febex Data Acquisition System

Tracking systems in HEP:

Development and Experimental Performance Evaluation of a Dose-Rate meter for Pulsed Beam.

Algorithms for digital γ-ray spectroscopy

GLAST Geant4 Simulation

Encoders for Linear Motors in the Electronics Industry

Gamma-ray Large Area Space Telescope (GLAST) Large Area Telescope (LAT) Calorimeter AFEE Board Parts Radiation Test Plan

Thinking ahead. Focused on life. REALIZED: GROUNDBREAKING RESOLUTION OF 80 µm VOXEL

Flex Circuits for the ATLAS Pixel Detector

Cronos -1 Gamma Object / Tool Monitors

10 is a soft polymer clay that can easily be moulded by hands (S1-Left). The simplest option is to create

G64 Area Gamma Monitor

Transcription:

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

Gamma vertex imaging C. H. Kim, J. H. Park, H. Seo, and H. R. Lee, Med. Phys. vol. 39, no. 10, pp. 1001-1006, 2012. 2

Performance estimation with Geant4 simulation Simulation condition Primary particles: 1.2 10 9 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

Proton beam 4

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

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: 3.125 mm) - Detector thickness: 1 st DSSD (145 μm), 2 nd DSSD (300 μm) - Bias voltage: 20 V (145 μm), 30 V (300 μm) 6

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

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

Development of multiplexing system Circuit design Multiplexing system Board layout 9

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

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. : 28% @ 400 nm - Gain: 2 10 4 @ 750 V Voltage divider Preamplifier (AMP-1000 Preamplifier) - Pulse fall time: ~ 50 µs - Maximum signal height: ±10 V Amplifier (in-house shaper, 250 ns) 11

Developed prototype imaging system Beryllium converter 1 st DSSD Electronic readout system for DSSD 2 nd DSSD Plastic scintillation detector 12

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

Test results 14

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

Performance test: V rms of DSSD First DSSD (145 μm) P-side V rms (V) V rms (kev) 0.153 3.35 0.160 4.53 0.145 3.58 0.152 3.60 0.143 3.15 0.151 3.80 0.157 3.42 0.152 2.98 0.149 3.47 0.156 3.59 0.138 3.45 0.147 4.19 0.142 3.51 0.148 2.62 0.142 3.16 0.149 3.53 N-side V rms (V) V rms (kev) 0.162 5.16 0.148 3.90 0.154 3.77 0.153 3.45 0.148 3.82 0.153 4.00 0.157 3.99 0.146 4.14 0.158 4.27 0.144 3.93 0.159 4.00 0.148 3.88 0.149 4.30 0.156 3.66 0.151 3.48 0.168 5.05 Second DSSD (300 μm) P-side V rms (V) V rms (kev) 0.128 5.05 0.124 5.58 0.113 5.98 0.119 3.97 0.121 4.55 0.115 3.98 0.123 4.64 0.122 3.79 0.117 5.10 0.118 4.53 0.116 4.48 0.121 4.36 0.118 3.63 0.111 4.16 0.115 3.68 0.115 4.43 N-side V rms (V) V rms (kev) 0.160 4.61 0.151 6.97 0.149 5.79 0.157 6.45 0.158 5.24 0.150 6.78 0.159 6.52 0.153 5.85 0.158 4.93 0.155 6.27 0.157 5.66 0.148 6.43 0.158 4.34 0.151 5.45 0.151 5.34 0.161 5.17 3.50 ± 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: 50.68 kev - Second DSSD: 104.85 kev 16

Energy calibration using Compton edges Y(channel) = 0.84 X(energy) + 2.3 Adj. R-square = 0.998 17

Test results for beta source 18

2D image for beta point source 90 Sr (Beta, 0.546 and 2.284 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

2D image for beta point source 90 Sr (Beta, 0.546 and 2.284 MeV) Position: 16.9 mm, -21.1 mm Original position (17.0 mm, -22.0 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

2D image for beta point source 90 Sr (Beta, 0.546 and 2.284 MeV) Position: 0.5 mm, -17.8 mm Original position (0.0 mm, -18.0 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

Test results for gamma source 22

2D image for gamma point source 60 Co (gamma, 1.173 and 1.332 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

2D image for gamma point source 60 Co (gamma, 1.173 and 1.332 MeV) Position: -17.9 mm, -16.5 mm Original position (-18.0 mm, -17.0 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

2D image for gamma point source 60 Co (gamma, 1.173 and 1.332 MeV) Position: -2.4 mm, -13.6 mm Original position (-2.5 mm, -14.0 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

Test results for high energy gamma source 26

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): 221.5 µci Measurement time: 30 min Energy threshold: 1.5 MeV 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): 221.5 µci Measurement time: 30 min Energy threshold: 1.5 MeV 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): 221.5 µci Measurement time: 30 min Energy threshold: 1.5 MeV 29

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

Thank you for your attention