A dedicated tool for PET scanner simulations using FLUKA

Size: px
Start display at page:

Download "A dedicated tool for PET scanner simulations using FLUKA"

Transcription

1 A dedicated tool for PET scanner simulations using FLUKA P. G. Ortega FLUKA meeting June

2 Need for in-vivo treatment monitoring Particles: The good thing is that they stop... Tumour Normal tissue/organ at risk Wanted: In-vivo range verification In-vivo dosimetric verification Desirable: A procedure for the verification of the irradiation field position of the particle range simultaneous with the therapeutic irradiation and, in particular, a procedure for the quantification of the dose distribution in-situ, in-vivo and in real time. the bad thing is that we have to know where! 2

3 Need for in-vivo treatment monitoring Check for: Mispositioning Anatomical changes Patient & organ movement Treatment mistakes and accidents We need a way to obtain real-time information about the treatment by analyzing the secondary radiation exiting the patient Among the possible monitoring methods, Positron emission tomography (PET) is currently the only available technique for non-invasive monitoring of ion beam dose delivery, tested in several clinical pilot studies. 3

4 PET treatment monitoring Positron Emission Tomography (PET): Detection of induced β + -activity formed as by-product of irradiation with ion beams Careful! AA(rr) DD(rr) : Non trivial relation Measured activity compared with MC calculation From K. Parodi 4

5 Also possible for other ions C ions (212 MeV/n) Protons (110 MeV) 11C, 10C 15O, 14O 11C, 13N,... K. Parodi et al, IEEE TNS 2005 Projectile + target β+-activation Only target β+-activation By-product of irradiation (15O, 11C, 13N...with T1/2 ~ 2, 20 and 10 min) 5

6 Calculation model of β+ activation FLUKA Monte Carlo code describes β+ emitter distribution for CT-based calculations in patient using Planning CT (segmented into 27 material) and same CT-range calibration curve as TPS (Parodi et al MP 34, 2007, PMB 52, 2007) Experimental cross-sections for β+ emitter production Semi-empirical biological modeling (Parodi et al IJROBP 2007) Convolution with 3D Gaussian kernel (7-7.5 mm FWHM) 6

7 FLUKA code development for (p,d), (n,d) reactions Excitation functions 12 C(p,x) 11 C and 16 O(p,x) 15 O, relevant for PET : Now deuteron formation at low energies is treated directly and no longer through coalescence (Data: CSISRS, NNDC, blue Fluka2011.2, red Fluka2013.0) 7

8 Flair tools for medical applications Flair is the GUI for FLUKA It helps with the creation of the input, provides a Geometry Editor to visualize and modify the geometry, allows to run, compile user routines, process the output files... and includes tools for medical applications like DICOM to FLUKA voxel geometry conversor and PET geometry builder 8

9 DICOM to FLUKA voxel geometry tool Imports DICOM files and translate them into FLUKA voxels. the folder containing all the DICOM files should be introduced. Flair will read it through and show the information for each slice (complete header) Just select the slice you are interested in and hit the voxel tab! 9

10 DICOM to FLUKA voxel geometry tool Imports DICOM files and translate them into FLUKA voxels. It is necessary to provide a file with the material definition list and another file with the assignment of materials for each Hounsfield Unit. Usually different materials for HU divided in intervals from 1050 HHHH 3100 Association of given HU interval with material and additional density and stopping power correction factors (Editable!) Process DICOM files and generate VOXEL and scoring mesh 10

11 Flair tools for PET simulations Provided the basic parameters for the PET scanner the tool generates the geometry, thanks to the lattice capabilities of FLUKA. Two sections: - Definition of the module (array of scintillator crystals): number of crystals, dimensions, spatial separation. - Definition of the ring: Number of modules, radius, opening angle (for full or partial rings), scintillator material. 11

12 Flair tools for PET simulations Several templates from commercially available PET scanners are included in the tool The user is free to edit the parameters for his particular situation before including it in the final geometry. 12

13 Flair tools for PET simulations 13

14 Flair tools for PET simulations Taking advantage of DICOM to FLUKA voxel geometry tool Optimized geometry of the simulation ready in few steps! All the elements can be easily adapted to each situation. 14

15 Flair tools for PET simulations Dedicated scoring, prepared to store the data in Interfile 3.3 binary format, list mode or particle track information Ready to use with external reconstruction algorithms Possibility to choose scoring parameters: o Arc correction. The radial bin size is corrected for the circular shape of the detector. o Maximum Ring Difference (MRD). The difference between two rings events can be restricted to a maximum value. o Span. Extent of axial data combined. Reduces the size of the stored data. o Mashing factor. Reduction of the angular sampling. Reduces the size of the stored data. o Number of segments. Parameter related to MRD and span number. Defines the number of segments the cells in the Michelogram can be divided. 15

16 Simple proof-of-concept of dedicated tool Measurement of two NEMA-like phantoms as a proof-of-concept, using an Ecat EXACT HR+ scanner with the standard scoring settings: The black cylinders have 4 times more activity than the background (gray). White areas are cold. 16

17 Simple proof-of-concept of dedicated tool 10 9 isotopes simulated and reconstructed with STIR filtered back-projection 3D reprojection (FBP3DRP) algorithm, simple but enough for our purposes. Original phantom Big phantom Small phantom section reconstruction reconstruction Scoring parameters: Span=9, MRD=22, No mashing factor, with 5 segments Some artifacts are present, due to simple reconstruction algorithm, but good overall description of the phantom. 17

18 Conclusions Recent FLUKA code developments improve the description of deuteron formation in reactions important for PETrelated studies, like the generation and distribution of β+ emitters for hadron-therapy. A dedicated tool for DICOM to FLUKA voxel geometry conversor and a tool for PET scanner geometry building have been presented, integrated into Flair, the GUI for FLUKA. The use of these tools allows a complete simulation of clinical studies and PET monitoring in few steps. Image from K. Parodi et al. IJRBOP

19 Thanks for your attention! Work partially founded by: 19

ADVANCES IN FLUKA PET TOOLS

ADVANCES IN FLUKA PET TOOLS MCMA2017 ADVANCES IN FLUKA PET TOOLS Caterina Cuccagna Tera Foundation (CERN) and University of Geneva Ricardo Santos Augusto, Caterina Cuccagna, Wioletta Kozlowska,Pablo Garcia Ortega, Yassine Toufique,

More information

Voxels and Medical Applications. FLUKA Beginners course

Voxels and Medical Applications. FLUKA Beginners course Voxels and Medical Applications FLUKA Beginners course The FLUKA voxel geometry It is possible to describe a geometry in terms of voxels, i.e., tiny parallelepipeds (all of equal size) forming a 3-dimensional

More information

Detector simulations for in-beam PET with FLUKA. Francesco Pennazio Università di Torino and INFN, TORINO

Detector simulations for in-beam PET with FLUKA. Francesco Pennazio Università di Torino and INFN, TORINO Detector simulations for in-beam PET with FLUKA Francesco Pennazio Università di Torino and INFN, TORINO francesco.pennazio@unito.it Outline Why MC simulations in HadronTherapy monitoring? The role of

More information

A new PET prototype for proton therapy: comparison of data and Monte Carlo simulations

A new PET prototype for proton therapy: comparison of data and Monte Carlo simulations A new PET prototype for proton therapy: comparison of data and Monte Carlo simulations V. Rosso, G.Battistoni, N. Belcari, N. Camarlinghi, A. Ferrari, S. Ferretti, A. Kraan, A. Mairani, N. Marino, J. E.

More information

RADIOMICS: potential role in the clinics and challenges

RADIOMICS: potential role in the clinics and challenges 27 giugno 2018 Dipartimento di Fisica Università degli Studi di Milano RADIOMICS: potential role in the clinics and challenges Dr. Francesca Botta Medical Physicist Istituto Europeo di Oncologia (Milano)

More information

Image-based Monte Carlo calculations for dosimetry

Image-based Monte Carlo calculations for dosimetry Image-based Monte Carlo calculations for dosimetry Irène Buvat Imagerie et Modélisation en Neurobiologie et Cancérologie UMR 8165 CNRS Universités Paris 7 et Paris 11 Orsay, France buvat@imnc.in2p3.fr

More information

Michael Speiser, Ph.D.

Michael Speiser, Ph.D. IMPROVED CT-BASED VOXEL PHANTOM GENERATION FOR MCNP MONTE CARLO Michael Speiser, Ph.D. Department of Radiation Oncology UT Southwestern Medical Center Dallas, TX September 1 st, 2012 CMPWG Workshop Medical

More information

The OpenGATE Collaboration

The OpenGATE Collaboration The OpenGATE Collaboration GATE developments and future releases GATE Users meeting, IEEE MIC 2015, San Diego Sébastien JAN CEA - IMIV sebastien.jan@cea.fr Outline Theranostics modeling Radiobiology Optics

More information

In-vivo dose verification for particle therapy

In-vivo dose verification for particle therapy In-vivo dose verification for particle therapy D.R. Schaart, NCS Lustrum, 5-Oct-2012 HollandPTC 1 Protons vs. photons Photons Protons Dennis R. Schaart Delft University of Technology 2 Protons: the promise

More information

gpmc: GPU-Based Monte Carlo Dose Calculation for Proton Radiotherapy Xun Jia 8/7/2013

gpmc: GPU-Based Monte Carlo Dose Calculation for Proton Radiotherapy Xun Jia 8/7/2013 gpmc: GPU-Based Monte Carlo Dose Calculation for Proton Radiotherapy Xun Jia xunjia@ucsd.edu 8/7/2013 gpmc project Proton therapy dose calculation Pencil beam method Monte Carlo method gpmc project Started

More information

Validation of GEANT4 for Accurate Modeling of 111 In SPECT Acquisition

Validation of GEANT4 for Accurate Modeling of 111 In SPECT Acquisition Validation of GEANT4 for Accurate Modeling of 111 In SPECT Acquisition Bernd Schweizer, Andreas Goedicke Philips Technology Research Laboratories, Aachen, Germany bernd.schweizer@philips.com Abstract.

More information

Implementation and evaluation of a fully 3D OS-MLEM reconstruction algorithm accounting for the PSF of the PET imaging system

Implementation and evaluation of a fully 3D OS-MLEM reconstruction algorithm accounting for the PSF of the PET imaging system Implementation and evaluation of a fully 3D OS-MLEM reconstruction algorithm accounting for the PSF of the PET imaging system 3 rd October 2008 11 th Topical Seminar on Innovative Particle and Radiation

More information

A fast and accurate GPU-based proton transport Monte Carlo simulation for validating proton therapy treatment plans

A fast and accurate GPU-based proton transport Monte Carlo simulation for validating proton therapy treatment plans A fast and accurate GPU-based proton transport Monte Carlo simulation for validating proton therapy treatment plans H. Wan Chan Tseung 1 J. Ma C. Beltran PTCOG 2014 13 June, Shanghai 1 wanchantseung.hok@mayo.edu

More information

Performance Evaluation of radionuclide imaging systems

Performance Evaluation of radionuclide imaging systems Performance Evaluation of radionuclide imaging systems Nicolas A. Karakatsanis STIR Users meeting IEEE Nuclear Science Symposium and Medical Imaging Conference 2009 Orlando, FL, USA Geant4 Application

More information

Basics of treatment planning II

Basics of treatment planning II Basics of treatment planning II Sastry Vedam PhD DABR Introduction to Medical Physics III: Therapy Spring 2015 Dose calculation algorithms! Correction based! Model based 1 Dose calculation algorithms!

More information

DUAL-ENERGY CT IN PROTON THERAPY

DUAL-ENERGY CT IN PROTON THERAPY 10/31/17 DUAL-ENERGY CT IN PROTON THERAPY Isabel Almeida, MAASTRO Clinic 7th NCS Lustrum Symposium 1 10/31/17 http://zonptc.bouwwebcam.nl https://www.youtube.com/watch?v=3vvvf5bqn7g Range uncertainties

More information

Dosimetric Analysis Report

Dosimetric Analysis Report RT-safe 48, Artotinis str 116 33, Athens Greece +30 2107563691 info@rt-safe.com Dosimetric Analysis Report SAMPLE, for demonstration purposes only Date of report: ----------- Date of irradiation: -----------

More information

Proton dose calculation algorithms and configuration data

Proton dose calculation algorithms and configuration data Proton dose calculation algorithms and configuration data Barbara Schaffner PTCOG 46 Educational workshop in Wanjie, 20. May 2007 VARIAN Medical Systems Agenda Broad beam algorithms Concept of pencil beam

More information

Geant4 in Brachytherapy

Geant4 in Brachytherapy Geant4 in Brachytherapy 1. 2. 3. 4. 5. Brachytherapy: Brief Overview Clinical applications Basic research Ultrafast & biology applications Issues for the work group 1 Brachytherapy: Overview Brachy: Greek

More information

Dosimetry Simulations with the UF-B Series Phantoms using the PENTRAN-MP Code System

Dosimetry Simulations with the UF-B Series Phantoms using the PENTRAN-MP Code System Dosimetry Simulations with the UF-B Series Phantoms using the PENTRAN-MP Code System A. Al-Basheer, M. Ghita, G. Sjoden, W. Bolch, C. Lee, and the ALRADS Group Computational Medical Physics Team Nuclear

More information

CLINICAL ASPECTS OF COMPACT GANTRY DESIGNS

CLINICAL ASPECTS OF COMPACT GANTRY DESIGNS CLINICAL ASPECTS OF COMPACT GANTRY DESIGNS J. Heese, J. Wulff, A. Winnebeck, A. Huggins, M. Schillo VARIAN PARTICLE THERAPY JUERGEN HEESE New gantry developments Viewpoint from user and vendor perspective

More information

Introduction to Positron Emission Tomography

Introduction to Positron Emission Tomography Planar and SPECT Cameras Summary Introduction to Positron Emission Tomography, Ph.D. Nuclear Medicine Basic Science Lectures srbowen@uw.edu System components: Collimator Detector Electronics Collimator

More information

Measurement of fragmentation cross-section of 400 MeV/u 12 C beam on thin targets

Measurement of fragmentation cross-section of 400 MeV/u 12 C beam on thin targets Measurement of fragmentation cross-section of 400 MeV/u 12 C beam on thin targets Candidate: Abdul Haneefa Kummali Supervisor : Dr. Vincenzo Monaco PhD School - Department of Physics XXVII cycle 14-February-2014

More information

Basics of treatment planning II

Basics of treatment planning II Basics of treatment planning II Sastry Vedam PhD DABR Introduction to Medical Physics III: Therapy Spring 2015 Monte Carlo Methods 1 Monte Carlo! Most accurate at predicting dose distributions! Based on

More information

Diagnostic imaging techniques. Krasznai Zoltán. University of Debrecen Medical and Health Science Centre Department of Biophysics and Cell Biology

Diagnostic imaging techniques. Krasznai Zoltán. University of Debrecen Medical and Health Science Centre Department of Biophysics and Cell Biology Diagnostic imaging techniques Krasznai Zoltán University of Debrecen Medical and Health Science Centre Department of Biophysics and Cell Biology 1. Computer tomography (CT) 2. Gamma camera 3. Single Photon

More information

Design and performance characteristics of a Cone Beam CT system for Leksell Gamma Knife Icon

Design and performance characteristics of a Cone Beam CT system for Leksell Gamma Knife Icon Design and performance characteristics of a Cone Beam CT system for Leksell Gamma Knife Icon WHITE PAPER Introduction Introducing an image guidance system based on Cone Beam CT (CBCT) and a mask immobilization

More information

ADVANCING CANCER TREATMENT

ADVANCING CANCER TREATMENT The RayPlan treatment planning system makes proven, innovative RayStation technology accessible to clinics that need a cost-effective and streamlined solution. Fast, efficient and straightforward to use,

More information

Image Guided Multibeam Radiotherapy

Image Guided Multibeam Radiotherapy José Luis Freijo a* Image Guided Multibeam Radiotherapy a Comisión Nacional de Energía Atómica, Av. del Libertador 8250, 1429, Buenos Aires, Argentina. Abstract. This paper provides an outlook of the status

More information

ADVANCING CANCER TREATMENT

ADVANCING CANCER TREATMENT 3 ADVANCING CANCER TREATMENT SUPPORTING CLINICS WORLDWIDE RaySearch is advancing cancer treatment through pioneering software. We believe software has un limited potential, and that it is now the driving

More information

Monte Carlo methods in proton beam radiation therapy. Harald Paganetti

Monte Carlo methods in proton beam radiation therapy. Harald Paganetti Monte Carlo methods in proton beam radiation therapy Harald Paganetti Introduction: Proton Physics Electromagnetic energy loss of protons Distal distribution Dose [%] 120 100 80 60 40 p e p Ionization

More information

Introduction to Biomedical Imaging

Introduction to Biomedical Imaging Alejandro Frangi, PhD Computational Imaging Lab Department of Information & Communication Technology Pompeu Fabra University www.cilab.upf.edu X-ray Projection Imaging Computed Tomography Digital X-ray

More information

Goals of this presentation

Goals of this presentation Transferring HEP Innovative concepts of electronics, trigger and DAQ Architecture for future large experiments to state of the art applications in medical imaging. P. Le Dû p.ledu@ipnl.in2p3.fr DEC_2010

More information

ELECTRON DOSE KERNELS TO ACCOUNT FOR SECONDARY PARTICLE TRANSPORT IN DETERMINISTIC SIMULATIONS

ELECTRON DOSE KERNELS TO ACCOUNT FOR SECONDARY PARTICLE TRANSPORT IN DETERMINISTIC SIMULATIONS Computational Medical Physics Working Group Workshop II, Sep 30 Oct 3, 2007 University of Florida (UF), Gainesville, Florida USA on CD-ROM, American Nuclear Society, LaGrange Park, IL (2007) ELECTRON DOSE

More information

INTRODUCTION TO MEDICAL IMAGING- 3D LOCALIZATION LAB MANUAL 1. Modifications for P551 Fall 2013 Medical Physics Laboratory

INTRODUCTION TO MEDICAL IMAGING- 3D LOCALIZATION LAB MANUAL 1. Modifications for P551 Fall 2013 Medical Physics Laboratory INTRODUCTION TO MEDICAL IMAGING- 3D LOCALIZATION LAB MANUAL 1 Modifications for P551 Fall 2013 Medical Physics Laboratory Introduction Following the introductory lab 0, this lab exercise the student through

More information

COMPARISON OF DOSE CALCULATION ALGORITHMS FOR LEKSELL GAMMA KNIFE PERFEXION USING MONTE CARLO VOXEL PHANTOMS

COMPARISON OF DOSE CALCULATION ALGORITHMS FOR LEKSELL GAMMA KNIFE PERFEXION USING MONTE CARLO VOXEL PHANTOMS COMPARISON OF DOSE CALCULATION ALGORITHMS FOR LEKSELL GAMMA KNIFE PERFEXION USING MONTE CARLO VOXEL PHANTOMS Jan Pipek 1, Josef Novotný Jr. 1,2,3, Josef Novotný 1, Petra Kozubíková 1 1 Faculty of Nuclear

More information

TEPZZ Z754_7A_T EP A1 (19) (11) EP A1 (12) EUROPEAN PATENT APPLICATION. (51) Int Cl.: A61N 5/10 ( )

TEPZZ Z754_7A_T EP A1 (19) (11) EP A1 (12) EUROPEAN PATENT APPLICATION. (51) Int Cl.: A61N 5/10 ( ) (19) TEPZZ Z74_7A_T (11) EP 3 07 417 A1 (12) EUROPEAN PATENT APPLICATION (43) Date of publication: 0..16 Bulletin 16/ (1) Int Cl.: A61N / (06.01) (21) Application number: 16163147.8 (22) Date of filing:

More information

Validation of Proton Nozzle. Jae-ik Shin (KIRAMS) Sebyeong Lee (NCC)

Validation of Proton Nozzle. Jae-ik Shin (KIRAMS) Sebyeong Lee (NCC) Validation of Proton Nozzle Jae-ik Shin (KIRAMS) Sebyeong Lee (NCC) Outline 1. Proposal 2. Status Report of BeamNozzle example 3. Comparison between simulation and measurement 4. Summary Proposal Goal

More information

IMSURE QA SOFTWARE FAST, PRECISE QA SOFTWARE

IMSURE QA SOFTWARE FAST, PRECISE QA SOFTWARE QA SOFTWARE FAST, PRECISE Software for accurate and independent verification of monitor units, dose, and overall validity of standard, IMRT, VMAT, SRS and brachytherapy plans no film, no phantoms, no linac

More information

MCNP4C3-BASED SIMULATION OF A MEDICAL LINEAR ACCELERATOR

MCNP4C3-BASED SIMULATION OF A MEDICAL LINEAR ACCELERATOR Computational Medical Physics Working Group Workshop II, Sep 3 Oct 3, 7 University of Florida (UF), Gainesville, Florida USA on CD-ROM, American Nuclear Society, LaGrange Park, IL (7) MCNP4C3-BASED SIMULATION

More information

Corso di laurea in Fisica A.A Fisica Medica 5 SPECT, PET

Corso di laurea in Fisica A.A Fisica Medica 5 SPECT, PET Corso di laurea in Fisica A.A. 2007-2008 Fisica Medica 5 SPECT, PET Step 1: Inject Patient with Radioactive Drug Drug is labeled with positron (β + ) emitting radionuclide. Drug localizes

More information

PURE. ViSION Edition PET/CT. Patient Comfort Put First.

PURE. ViSION Edition PET/CT. Patient Comfort Put First. PURE ViSION Edition PET/CT Patient Comfort Put First. 2 System features that put patient comfort and safety first. Oncology patients deserve the highest levels of safety and comfort during scans. Our Celesteion

More information

Simulations in emission tomography using GATE

Simulations in emission tomography using GATE Simulations in emission tomography using GATE Irène Buvat buvat@imed.jussieu.fr Laboratory of Functional Imaging, U678 INSERM, Paris, France Outline Emission tomography and need for simulations GATE short

More information

Hidenobu Tachibana The Cancer Institute Hospital of JFCR, Radiology Dept. The Cancer Institute of JFCR, Physics Dept.

Hidenobu Tachibana The Cancer Institute Hospital of JFCR, Radiology Dept. The Cancer Institute of JFCR, Physics Dept. 2-D D Dose-CT Mapping in Geant4 Hidenobu Tachibana The Cancer Institute Hospital of JFCR, Radiology Dept. The Cancer Institute of JFCR, Physics Dept. Table of Contents Background & Purpose Materials Methods

More information

MapCHECK 2 & 3DVH. The Gold Standard for 2D Arrays

MapCHECK 2 & 3DVH. The Gold Standard for 2D Arrays MapCHECK 2 & 3DVH The Gold Standard for 2D Arrays Your Most Valuable QA and Dosimetry Tools THE GOLD STANDARD FOR 2D ARRAYS The MapCHECK 2 is the world s most selected independent 2D measurement array.

More information

Reconstruction in CT and relation to other imaging modalities

Reconstruction in CT and relation to other imaging modalities Reconstruction in CT and relation to other imaging modalities Jørgen Arendt Jensen November 1, 2017 Center for Fast Ultrasound Imaging, Build 349 Department of Electrical Engineering Center for Fast Ultrasound

More information

BME I5000: Biomedical Imaging

BME I5000: Biomedical Imaging 1 Lucas Parra, CCNY BME I5000: Biomedical Imaging Lecture 4 Computed Tomography Lucas C. Parra, parra@ccny.cuny.edu some slides inspired by lecture notes of Andreas H. Hilscher at Columbia University.

More information

Arion: a realistic projection simulator for optimizing laboratory and industrial micro-ct

Arion: a realistic projection simulator for optimizing laboratory and industrial micro-ct Arion: a realistic projection simulator for optimizing laboratory and industrial micro-ct J. DHAENE* 1, E. PAUWELS 1, T. DE SCHRYVER 1, A. DE MUYNCK 1, M. DIERICK 1, L. VAN HOOREBEKE 1 1 UGCT Dept. Physics

More information

Modern CT system generations Measurement of attenuation

Modern CT system generations Measurement of attenuation CT reconstruction repetition & hints Reconstruction in CT and hints to the assignments Jørgen Arendt Jensen October 4, 16 Center for Fast Ultrasound Imaging, Build 349 Department of Electrical Engineering

More information

Reconstruction in CT and hints to the assignments

Reconstruction in CT and hints to the assignments Reconstruction in CT and hints to the assignments Jørgen Arendt Jensen October 24, 2016 Center for Fast Ultrasound Imaging, Build 349 Department of Electrical Engineering Center for Fast Ultrasound Imaging

More information

Loma Linda University Medical Center Dept. of Radiation Medicine

Loma Linda University Medical Center Dept. of Radiation Medicine Loma Linda University Medical Center Dept. of Radiation Medicine and Northern Illinois University Dept. of Physics and Dept. of Computer Science Presented by George Coutrakon, PhD NIU Physics Dept. Collaborators

More information

MapCHECK 2 & 3DVH The Gold Standard for 2D Arrays

MapCHECK 2 & 3DVH The Gold Standard for 2D Arrays MapCHECK 2 & 3DVH The Gold Standard for 2D Arrays Your Most Valuable QA and Dosimetry Tools THE GOLD STANDARD FOR 2D ARRAYS The MapCHECK 2 is the world s most selected independent 2D measurement array.

More information

VXRE Reconstruction Software Manual

VXRE Reconstruction Software Manual VXRE Reconstruction Software Manual Version 1.7.8 3D INDUSTRIAL IMAGING 3D Industrial Imaging Co.,Ltd. Address :#413 Institute of Computer Technology, Seoul National University, Daehak-dong, Gwanak-gu,

More information

Radon Transform and Filtered Backprojection

Radon Transform and Filtered Backprojection Radon Transform and Filtered Backprojection Jørgen Arendt Jensen October 13, 2016 Center for Fast Ultrasound Imaging, Build 349 Department of Electrical Engineering Center for Fast Ultrasound Imaging Department

More information

Cherenkov Radiation. Doctoral Thesis. Rok Dolenec. Supervisor: Prof. Dr. Samo Korpar

Cherenkov Radiation. Doctoral Thesis. Rok Dolenec. Supervisor: Prof. Dr. Samo Korpar Doctoral Thesis Time-of-Flight Time-of-Flight Positron Positron Emission Emission Tomography Tomography Using Using Cherenkov Cherenkov Radiation Radiation Rok Dolenec Supervisor: Prof. Dr. Samo Korpar

More information

THE WIRELESS PHANTOM PERFORM ACCURATE PATIENT QA IN LESS TIME THAN EVER!

THE WIRELESS PHANTOM PERFORM ACCURATE PATIENT QA IN LESS TIME THAN EVER! THE WIRELESS PHANTOM PERFORM ACCURATE PATIENT QA IN LESS TIME THAN EVER! Confidence in complex treatments Modern radiation therapy uses complex plans with techniques such as IMRT, VMAT and Tomotherapy.

More information

CLASS HOURS: 4 CREDIT HOURS: 4 LABORATORY HOURS: 0

CLASS HOURS: 4 CREDIT HOURS: 4 LABORATORY HOURS: 0 Revised 10/10 COURSE SYLLABUS TM 220 COMPUTED TOMOGRAPHY PHYSICS CLASS HOURS: 4 CREDIT HOURS: 4 LABORATORY HOURS: 0 CATALOG COURSE DESCRIPTION: This course is one of a three course set in whole body Computed

More information

Mathematical methods and simulations tools useful in medical radiation physics

Mathematical methods and simulations tools useful in medical radiation physics Mathematical methods and simulations tools useful in medical radiation physics Michael Ljungberg, professor Department of Medical Radiation Physics Lund University SE-221 85 Lund, Sweden Major topic 1:

More information

Effects of the difference in tube voltage of the CT scanner on. dose calculation

Effects of the difference in tube voltage of the CT scanner on. dose calculation Effects of the difference in tube voltage of the CT scanner on dose calculation Dong Joo Rhee, Sung-woo Kim, Dong Hyeok Jeong Medical and Radiological Physics Laboratory, Dongnam Institute of Radiological

More information

MEDICAL IMAGING 2nd Part Computed Tomography

MEDICAL IMAGING 2nd Part Computed Tomography MEDICAL IMAGING 2nd Part Computed Tomography Introduction 2 In the last 30 years X-ray Computed Tomography development produced a great change in the role of diagnostic imaging in medicine. In convetional

More information

Measurement of depth-dose of linear accelerator and simulation by use of Geant4 computer code

Measurement of depth-dose of linear accelerator and simulation by use of Geant4 computer code reports of practical oncology and radiotherapy 1 5 (2 0 1 0) 64 68 available at www.sciencedirect.com journal homepage: http://www.rpor.eu/ Original article Measurement of depth-dose of linear accelerator

More information

Analysis of Radiation Transport through Multileaf Collimators Using BEAMnrc Code

Analysis of Radiation Transport through Multileaf Collimators Using BEAMnrc Code American Journal of Biomedical Engineering 216, 6(4): 124-131 DOI: 1.5923/j.ajbe.21664.3 Analysis of Radiation Transport through Multileaf Collimators Using BEAMnrc Code Ankit Kajaria 1,*, Neeraj Sharma

More information

Particle track plotting in Visual MCNP6 Randy Schwarz 1,*

Particle track plotting in Visual MCNP6 Randy Schwarz 1,* Particle track plotting in Visual MCNP6 Randy Schwarz 1,* 1 Visual Editor Consultants, PO Box 1308, Richland, WA 99352, USA Abstract. A visual interface for MCNP6 has been created to allow the plotting

More information

Use of Monte Carlo modelling in radiotherapy linac design. David Roberts, PhD Senior Physicist Elekta

Use of Monte Carlo modelling in radiotherapy linac design. David Roberts, PhD Senior Physicist Elekta Use of Monte Carlo modelling in radiotherapy linac design David Roberts, PhD Senior Physicist Elekta Contents Overview of Elekta What we do Where we use Monte Carlo Codes and resources Example : Agility

More information

Empirical cupping correction: A first-order raw data precorrection for cone-beam computed tomography

Empirical cupping correction: A first-order raw data precorrection for cone-beam computed tomography Empirical cupping correction: A first-order raw data precorrection for cone-beam computed tomography Marc Kachelrieß, a Katia Sourbelle, and Willi A. Kalender Institute of Medical Physics, University of

More information

GATE-RT Applications in Radiation Therapy

GATE-RT Applications in Radiation Therapy GATE-RT Applications in Radiation Therapy GATE Training, Orsay, April 2011 David SARRUT Creatis - CNRS Lyon - France GATE-RT: Radiation Therapy applications Related to dose distribution Radiotherapy: therapy

More information

Impact of X-ray Scatter When Using CT-based Attenuation Correction in PET: A Monte Carlo Investigation

Impact of X-ray Scatter When Using CT-based Attenuation Correction in PET: A Monte Carlo Investigation 26 IEEE Nuclear Science Symposium Conference Record M6-349 Impact of X-ray Scatter When Using CT-based Attenuation Correction in PET: A Monte Carlo Investigation Habib Zaidi, Senior Member, IEEE and Mohammad

More information

VALIDATION OF A MONTE CARLO DOSE CALCULATION ALGORITHM FOR CLINICAL ELECTRON BEAMS IN THE PRESENCE OF PHANTOMS WITH COMPLEX HETEROGENEITIES

VALIDATION OF A MONTE CARLO DOSE CALCULATION ALGORITHM FOR CLINICAL ELECTRON BEAMS IN THE PRESENCE OF PHANTOMS WITH COMPLEX HETEROGENEITIES VALIDATION OF A MONTE CARLO DOSE CALCULATION ALGORITHM FOR CLINICAL ELECTRON BEAMS IN THE PRESENCE OF PHANTOMS WITH COMPLEX HETEROGENEITIES by Shayla Landfair Enright A Thesis Submitted to the Faculty

More information

STIR User s Meeting. Reconstruction of PET data acquired with the BrainPET using STIR. 31. October 2013 Liliana Caldeira

STIR User s Meeting. Reconstruction of PET data acquired with the BrainPET using STIR. 31. October 2013 Liliana Caldeira STIR User s Meeting Reconstruction of PET data acquired with the BrainPET using STIR 31. October 2013 Liliana Caldeira Outline 3T MR-BrainPET System Reading BrainPET data into STIR FBP reconstruction OSEM/OSMAPOSL

More information

UNIVERSITY OF SOUTHAMPTON

UNIVERSITY OF SOUTHAMPTON UNIVERSITY OF SOUTHAMPTON PHYS2007W1 SEMESTER 2 EXAMINATION 2014-2015 MEDICAL PHYSICS Duration: 120 MINS (2 hours) This paper contains 10 questions. Answer all questions in Section A and only two questions

More information

The new version of the GATE simulation platform

The new version of the GATE simulation platform The new version of the GATE simulation platform Thibault Frisson Université de Lyon Léon Bérard anti-cancer center, CREATIS, CNRS On behalf of the OpenGATE Collaboration Outline GATE overview Main features

More information

Image Acquisition Systems

Image Acquisition Systems Image Acquisition Systems Goals and Terminology Conventional Radiography Axial Tomography Computer Axial Tomography (CAT) Magnetic Resonance Imaging (MRI) PET, SPECT Ultrasound Microscopy Imaging ITCS

More information

Influence of electron density spatial distribution and X-ray beam quality during CT simulation on dose calculation accuracy

Influence of electron density spatial distribution and X-ray beam quality during CT simulation on dose calculation accuracy JOURNAL OF APPLIED CLINICAL MEDICAL PHYSICS, VOLUME 12, NUMBER 3, summer 2011 Influence of electron density spatial distribution and X-ray beam quality during CT simulation on dose calculation accuracy

More information

Dose Point Kernel calculation and modelling with nuclear medicine dosimetry purposes

Dose Point Kernel calculation and modelling with nuclear medicine dosimetry purposes Dose Point Kernel calculation and modelling with nuclear medicine dosimetry purposes LIIFAMIRX - Laboratorio de Investigación e Instrumentación en Física Aplicada a la Medicina e Imágenes por Rayos X -

More information

Emission Computed Tomography Notes

Emission Computed Tomography Notes Noll (24) ECT Notes: Page 1 Emission Computed Tomography Notes Introduction Emission computed tomography (ECT) is the CT applied to nuclear medicine. There are two varieties of ECT: 1. SPECT single-photon

More information

Investigation of tilted dose kernels for portal dose prediction in a-si electronic portal imagers

Investigation of tilted dose kernels for portal dose prediction in a-si electronic portal imagers Investigation of tilted dose kernels for portal dose prediction in a-si electronic portal imagers Krista Chytyk MSc student Supervisor: Dr. Boyd McCurdy Introduction The objective of cancer radiotherapy

More information

REAL-TIME ADAPTIVITY IN HEAD-AND-NECK AND LUNG CANCER RADIOTHERAPY IN A GPU ENVIRONMENT

REAL-TIME ADAPTIVITY IN HEAD-AND-NECK AND LUNG CANCER RADIOTHERAPY IN A GPU ENVIRONMENT REAL-TIME ADAPTIVITY IN HEAD-AND-NECK AND LUNG CANCER RADIOTHERAPY IN A GPU ENVIRONMENT Anand P Santhanam Assistant Professor, Department of Radiation Oncology OUTLINE Adaptive radiotherapy for head and

More information

Implementation of the EGSnrc / BEAMnrc Monte Carlo code - Application to medical accelerator SATURNE43

Implementation of the EGSnrc / BEAMnrc Monte Carlo code - Application to medical accelerator SATURNE43 International Journal of Innovation and Applied Studies ISSN 2028-9324 Vol. 6 No. 3 July 2014, pp. 635-641 2014 Innovative Space of Scientific Research Journals http://www.ijias.issr-journals.org/ Implementation

More information

Ch. 4 Physical Principles of CT

Ch. 4 Physical Principles of CT Ch. 4 Physical Principles of CT CLRS 408: Intro to CT Department of Radiation Sciences Review: Why CT? Solution for radiography/tomography limitations Superimposition of structures Distinguishing between

More information

ANALYSIS OF CT AND PET/SPECT IMAGES FOR DOSIMETRY CALCULATION

ANALYSIS OF CT AND PET/SPECT IMAGES FOR DOSIMETRY CALCULATION 2009 International Nuclear Atlantic Conference - INAC 2009 Rio de Janeiro,RJ, Brazil, September27 to October 2, 2009 ASSOCIAÇÃO BRASILEIRA DE ENERGIA NUCLEAR - ABEN ISBN: 978-85-99141-03-8 ANALYSIS OF

More information

Monaco VMAT. The Next Generation in IMRT/VMAT Planning. Paulo Mathias Customer Support TPS Application

Monaco VMAT. The Next Generation in IMRT/VMAT Planning. Paulo Mathias Customer Support TPS Application Monaco VMAT The Next Generation in IMRT/VMAT Planning Paulo Mathias Customer Support TPS Application 11.05.2011 Background What is Monaco? Advanced IMRT/VMAT treatment planning system from Elekta Software

More information

Radiology. Marta Anguiano Millán. Departamento de Física Atómica, Molecular y Nuclear Facultad de Ciencias. Universidad de Granada

Radiology. Marta Anguiano Millán. Departamento de Física Atómica, Molecular y Nuclear Facultad de Ciencias. Universidad de Granada Departamento de Física Atómica, Molecular y Nuclear Facultad de Ciencias. Universidad de Granada Overview Introduction Overview Introduction Tecniques of imaging in Overview Introduction Tecniques of imaging

More information

Electron Dose Kernels (EDK) for Secondary Particle Transport in Deterministic Simulations

Electron Dose Kernels (EDK) for Secondary Particle Transport in Deterministic Simulations Electron Dose Kernels (EDK) for Secondary Particle Transport in Deterministic Simulations A. Al-Basheer, G. Sjoden, M. Ghita Computational Medical Physics Team Nuclear & Radiological Engineering University

More information

Artifact Mitigation in High Energy CT via Monte Carlo Simulation

Artifact Mitigation in High Energy CT via Monte Carlo Simulation PIERS ONLINE, VOL. 7, NO. 8, 11 791 Artifact Mitigation in High Energy CT via Monte Carlo Simulation Xuemin Jin and Robert Y. Levine Spectral Sciences, Inc., USA Abstract The high energy (< 15 MeV) incident

More information

Determination of Three-Dimensional Voxel Sensitivity for Two- and Three-Headed Coincidence Imaging

Determination of Three-Dimensional Voxel Sensitivity for Two- and Three-Headed Coincidence Imaging IEEE TRANSACTIONS ON NUCLEAR SCIENCE, VOL. 50, NO. 3, JUNE 2003 405 Determination of Three-Dimensional Voxel Sensitivity for Two- and Three-Headed Coincidence Imaging Edward J. Soares, Kevin W. Germino,

More information

Chapter 9 Field Shaping: Scanning Beam

Chapter 9 Field Shaping: Scanning Beam Chapter 9 Field Shaping: Scanning Beam X. Ronald Zhu, Ph.D. Department of Radiation Physics M. D. Anderson Cancer Center Houston, TX June 14-18, 2015 AAPM - Summer School 2015, Colorado Spring Acknowledgement

More information

Monte-Carlo-Based Scatter Correction for Quantitative SPECT Reconstruction

Monte-Carlo-Based Scatter Correction for Quantitative SPECT Reconstruction Monte-Carlo-Based Scatter Correction for Quantitative SPECT Reconstruction Realization and Evaluation Rolf Bippus 1, Andreas Goedicke 1, Henrik Botterweck 2 1 Philips Research Laboratories, Aachen 2 Fachhochschule

More information

PCRT 3D. Scalable Architecture System. User-Friendly. Traceable. Continuos Development

PCRT 3D. Scalable Architecture System. User-Friendly. Traceable. Continuos Development PCRT 3D The PCRT3D is a versatile 3D radiation treatment planning system featuring the most accurate algorithm calculations, the latest techniques in virtual simulation and the most advanced radiotherapy

More information

A CT-based Monte Carlo Dose Calculations for Proton Therapy Using a New Interface Program

A CT-based Monte Carlo Dose Calculations for Proton Therapy Using a New Interface Program World Academy of Science, Engineering and Technology 53 29 A CT-based Monte Carlo Dose Calculations for Proton Therapy Using a New Interface Program A. Esmaili Torshabi, A. Terakawa, K. Ishii, H. Yamazaki,

More information

Monte Carlo Simulation for Neptun 10 PC Medical Linear Accelerator and Calculations of Electron Beam Parameters

Monte Carlo Simulation for Neptun 10 PC Medical Linear Accelerator and Calculations of Electron Beam Parameters Monte Carlo Simulation for Neptun 1 PC Medical Linear Accelerator and Calculations of Electron Beam Parameters M.T. Bahreyni Toossi a, M. Momen Nezhad b, S.M. Hashemi a a Medical Physics Research Center,

More information

FAST, precise. qa software

FAST, precise. qa software qa software FAST, precise Software for accurate and independent verification of monitor units, dose, and overall validity of standard, IMRT, rotational or brachytherapy plans no film, no phantoms, no linac

More information

Effect of CT number stopping power conversion uncertainties on dose distributions

Effect of CT number stopping power conversion uncertainties on dose distributions Effect of CT number stopping power conversion uncertainties on dose distributions Stella Flampouri Roelf Slopsema, Daniel Yeung, Zuofeng Li 23 May 2007 PTCOG Intro Treatment planning system dose calculations

More information

The theory and practical aspects of proton imaging proton radiography (prad) and proton tomography (pct)

The theory and practical aspects of proton imaging proton radiography (prad) and proton tomography (pct) The theory and practical aspects of proton imaging proton radiography (prad) and proton tomography (pct) Fritz DeJongh, ProtonVDA Inc August 30 2018 Stay away from negative people. They have a problem

More information

Future is Effortless

Future is Effortless AQUATM Radiology is a machine Quality Assurance management solution that standardizes, streamlines and automates QA procedures throughout rediology department and across multiple sites. AQUATM Radiology

More information

Computer-Tomography II: Image reconstruction and applications

Computer-Tomography II: Image reconstruction and applications Computer-Tomography II: Image reconstruction and applications Prof. Dr. U. Oelfke DKFZ Heidelberg Department of Medical Physics (E040) Im Neuenheimer Feld 280 69120 Heidelberg, Germany u.oelfke@dkfz.de

More information

An approach to calculate and visualize intraoperative scattered radiation exposure

An approach to calculate and visualize intraoperative scattered radiation exposure Peter L. Reicertz Institut für Medizinische Informatik An approach to calculate and visualize intraoperative scattered radiation exposure Markus Wagner University of Braunschweig Institute of Technology

More information

Betatron Core Slow Extraction at CNAO

Betatron Core Slow Extraction at CNAO Betatron Core Slow Extraction at CNAO Dr. Luciano Falbo CNAO Machine CNAO is the only Italian facility for cancer treatment with protons (60-250 MeV) and carbon ions (120-400 MeV/u). The first patient

More information

DUE to beam polychromacity in CT and the energy dependence

DUE to beam polychromacity in CT and the energy dependence 1 Empirical Water Precorrection for Cone-Beam Computed Tomography Katia Sourbelle, Marc Kachelrieß, Member, IEEE, and Willi A. Kalender Abstract We propose an algorithm to correct for the cupping artifact

More information

Physical bases of X-ray diagnostics

Physical bases of X-ray diagnostics Physical bases of X-ray diagnostics Dr. István Voszka Possibilities of X-ray production (X-ray is produced, when charged particles of high velocity are stopped) X-ray tube: Relatively low accelerating

More information

Assesing multileaf collimator effect on the build-up region using Monte Carlo method

Assesing multileaf collimator effect on the build-up region using Monte Carlo method Pol J Med Phys Eng. 2008;14(3):163-182. PL ISSN 1425-4689 doi: 10.2478/v10013-008-0014-0 website: http://www.pjmpe.waw.pl M. Zarza Moreno 1, 2, N. Teixeira 3, 4, A. P. Jesus 1, 2, G. Mora 1 Assesing multileaf

More information

Constructing System Matrices for SPECT Simulations and Reconstructions

Constructing System Matrices for SPECT Simulations and Reconstructions Constructing System Matrices for SPECT Simulations and Reconstructions Nirantha Balagopal April 28th, 2017 M.S. Report The University of Arizona College of Optical Sciences 1 Acknowledgement I would like

More information