Response Characteristics of a Large-Area Ion Chamber with Various Radiotherapy Beams Makan Farrokhkish, B.Sc.

Similar documents
A comparison of methods for monitoring photon beam energy constancy

Neutron source strength measurements for Varian, Siemens, Elekta, and General Electric linear accelerators

8/4/2016. Determination of small field output factors, advantages and limitations of Monte Carlo simulations

factors for NE2561 ionization chambers in 3 cm x 3 cm beams of 6 MV and 10 MV photons

1 Introduction. A Monte Carlo study

) for Varian TrueBeam high-dose-rate therapy beams

Commissioning measurements for photon beam data on three TrueBeam linear accelerators, and comparison with Trilogy and Clinac 2100 linear accelerators

Implementation of the IAEA-AAPM Code of Practice for the dosimetry of small static fields used in external beam radiotherapy

Monitor backscatter factors for the Varian 21EX and TrueBeam linear accelerators: measurements and Monte Carlo modelling.

The Radiological Physics Center s standard dataset for small field size output factors

Comparison of Primary Doses Obtained in Three 6 MV Photon Beams Using a Small Attenuator

Estimate of Photonuclear Reaction in a Medical Linear Accelerator Using a Water-Equivalent Phantom

Battling Maxwell s Equations Physics Challenges and Solutions for Hybrid MRI Systems

Time-resolved beam symmetry measurement for VMAT commissioning and quality assurance

Visual Analysis of the Daily QA Results of Photon and Electron Beams of a Trilogy Linac over a Five-Year Period

Calculations of Photoneutrons from Varian Clinac Accelerators and Their Transmissions in Materials*

Linac activation of radioisotopes and underground gammaspectrometric analyses

Photon-beams monitor-unit calculations

ACCELERATORS AND MEDICAL PHYSICS

Measurements and comparisons for data of small beams of linear accelerators

International Journal of Scientific & Engineering Research, Volume 7, Issue 2, February-2016 ISSN

Objectives. Tolerance Limits and Action Levels for IMRT QA. The Overall Process of IMRT Planning and Delivery. Chain of IMRT Process

Simulation Modeling in Dosimetry

IRPA 2 nd European Congress, Paris, May Session: RP in Medicine - Workers. Activation Products In Medical Linear Accelerators

Radiation Protection Dosimetry (2007), Vol. 126, No. 1 4, pp Advance Access publication 11 May 2007

Evaluation of different methods for determining the magnitude of initial recombination in ionization chambers

Quality-Assurance Check of Collimator and Phantom- Scatter Factors

A Thesis. entitled. Micro Ionization Chamber. Vidheesha Arora. Master of Science Degree in. Biomedical Sciences: Medical Physics

Variations in daily quality assurance dosimetry from device levelling, feet position and backscatter material

The Influence of Brass Compensator Thickness and Field Size on Neutron Contamination Spectrum in 18MV Elekta SL 75/25 Medical Linear Accelerator

DOI /

Diamond detector in absorbed dose measurements in high-energy linear accelerator photon and electron beams

Michael Dunn Nuclear Data Group Leader Nuclear Science & Technology Division Medical Physics Working Group Meeting October 26, 2005

Electron therapy Class 2: Review questions

Comparison between TG-51 and TRS-398: Electron Contamination Effect on Photon Beam Quality Specification.

Dosimetric Properties of the Field Sizes of 12MV Photon Beams: A Monte Carlo Study

Monte Carlo simulation of the photoneutron field in linac radiotherapy treatments with different collimation systems

Estimation of neutron and gamma radiation doses inside the concrete shield wall for 10 and 15 MV medical linear accelerators

NEUTOR: Neutrons Monitor for. Project financed by: Radiotherapy

BEAMnrc: a code to simulate radiotherapy external beam sources

1.1.4 What are the differences between the Varian 600C and the Siemens KD2?

Neutron Fluence and Energy Spectra Around the Varian Clinac 2lOOC/23OOC Medical Accelerator

Evaluation of an electron Monte Carlo dose calculation algorithm for electron beams

A Measuring System with Recombination Chamber for Photoneutron Dosimetry at Medical Linear Accelerators

Physics. Sunday, March 4, :30 a.m. 10:00 a.m.

(INCLUDING THIS FRONT PAGE)

Secondary neutron spectra from modern Varian, Siemens, and Elekta linacs with multileaf collimators

Progress in Nuclear Science and Technology, Volume 6,

General characteristics of radiation dosimeters

Medical Linac. Block diagram. Electron source. Bending magnet. Accelerating structure. Klystron or magnetron. Pulse modulator.

Clinical Implementation of the IPEM 2003 Code of Practice for Electron Dosimetry

Magnetic removal of electron contamination in radiotherapy x-ray beams

Chapter 4. QUANTIFYING THE HAZARD II: DATA & ANALYSIS. The dose equivalents for spheres in air with 10 cm radius centred at a point in the

City University of Hong Kong

Volume 1 No. 4, October 2011 ISSN International Journal of Science and Technology IJST Journal. All rights reserved

The effect of dose calculation uncertainty on the evaluation of radiotherapy plans

Monte Carlo simulation with Geant4 for verification of rotational total skin electron therapy (TSET)

Evaluation of the truebeam machine performance check (MPC): mechanical and collimation checks

Radiation protection issues in proton therapy

Low energy linear acceleratordriven subcritical assembly

The neutron dose equivalent evaluation and shielding at the maze entrance of a Varian Clinac 23EX treatment room

Point dose measurements in VMAT: an investigation of detector choice and plan complexity.

Small Field Dosimetry and IAEA/AAPM Protocol

PHYS 5020 Computation and Image Processing

CHARACTERISTICS OF DEGRADED ELECTRON BEAMS PRODUCED BY NOVAC7 IORT ACCELERATOR

Experimental validation of the Eclipse AAA algorithm

A Study on Effective Source-Skin Distance using Phantom in Electron Beam Therapy

Science, Ami, Ami-machi, Inashiki-gun, Ibaraki , Japan. Ibaraki , Japan. Japan. *Corresponding author:

A Brief Introduction to Medical Imaging. Outline

Acquisition and analysis of megavoltage linac beam transmission data for direct verification of photon spectra models in a treatment planning system

Analysis of Image Noise in 3D Cone-Beam CT: Spatial and Fourier Domain Approaches under Conditions of Varying Stationarity

Surface Analysis - The Principal Techniques

Sensitivity of megavoltage photon beam Monte Carlo simulations to electron beam and other parameters

Comparison of two commercial detector arrays for IMRT quality assurance

Composite field dosimetry

Monitor Unit Calculations for Photon and Electrons. AAMD Meeting Raleigh, NC October 3, John P. Gibbons Chief of Clinical Physics

The impact of detector volume on penumbral dose prediction in a 6 MV radiation therapy X-ray beam

The EPOM shift of cylindrical ionization chambers - a status report Hui Khee Looe 1, Ndimofor Chofor 1, Dietrich Harder 2, Björn Poppe 1

Measurement of Neutron Activation from a High Energy Varian Linear Accelerator

ABSORBED DOSE TO WATER MEASUREMENTS IN HIGH ENERGY ELECTRON BEAMS USING DIFFERENT PLANE PARALLEL CHAMBERS *

Updating reference dosimetry a decade after TG-51

I. INTRODUCTION EXPERIMENTAL

Overview and Status of the Austrian Particle Therapy Facility MedAustron. Peter Urschütz

Towards efficient and accurate particle transport simulation in medical applications

Small Field Dosimetric Measurements with TLD-100, Alanine, and Ionization Chambers

Determination of absorbed dose to water for 60Co by the scaling theorem. M. Boutillon and A.-M. Perroche (1)

Monte Carlo Analyses of X-Ray Absorption, Noise, and Detective Quantum Efficiency Considering Therapeutic X-Ray Spectrum in Portal Imaging Detector

Interpretation of in-air output ratio and its impact on Dose Calculation

Simulations in Radiation Therapy

arxiv: v2 [physics.med-ph] 29 May 2015

Keywords: mechanical property, polymer optical fibre, radiation, transmission.

M d e i di l ca A pplilli t ca i ttions o f P arti ttic ti l P e h Physics Saverio Braccini INSEL

Neutron Sources in the Varian Clinac 2100~2300C Medical Accelerator Calculated by the EGS4 Code

Radiation Dosimetry. Electron interactions with matter. Important processes in radiotherapy. Contents. Alun Beddoe

The volume effect of detectors in the dosimetry of small fields used in IMRT

Current and Recent ICRU Activities in Radiation Protection Dosimetry and Measurements

SPARCLAB. Source For Plasma Accelerators and Radiation Compton with Laser And Beam

M [scale units/s] of the system

8/2/2012 UPDATING TG-51. When will it end? Part 1 - photon addendum. What are these updates? Photons: Electrons: More widespread revision required

TERA CONTRIBUTIONS TO PARTNER

Transcription:

Response Characteristics of a Large-Area Ion Chamber with Various Radiotherapy Beams Makan Farrokhkish, B.Sc. Department of Radiation Physics, Radiation Medicine Program Princess Margaret Cancer Centre, Toronto

S M Dose Area Photon Source Collimating elements Large Ion Chamber

Factors that influence IQM signals Linac Head Structure Beam Energy Beam Calibration

Varian Millennium Collimator Elekta MLCi2 Elekta Agility

IQM Response Characteristics With Different Radiotherapy Beam IQM Intrinsic and effective spatial sensitivity Response as a function of field size Response as a function of beam energy IQM response as a function of dose rates

Studied Linac Models TrueBeam (Varian Medical Systems, Palo Alto, CA). Millennium MLC. 6 MV, 10 MV, 6 FFF, 10 FFF Clinac ix (Varian Medical Systems, Palo Alto, CA). Millennium MLC. 6 MV, 18 MV Infinity ( Elekta AB, Stockholm, Sweden). Agility Collimator. 6MV, 18 MV Infinity ( Elekta AB, Stockholm, Sweden). MLCi2 Collimator. 6 MV, 18 MV

Objectives IQM Intrinsic and effective spatial sensitivity

-500 V 0 V

Normalized Signal Central Gradient Profile ( Normalized To Centre) 1.6 1.4 1.2 1.0 Loss of lateral 0.8 Electron 0.6 Equilibrium 0.4 0.2 0.0-15 -10-5 0 5 10 15 Off Axis Distance (cm)

Normalized Signal 1.6 1.2 1.4 1.0 1.2 1.0 0.8 Canteral None-Gradient Profile ( Normalized To Centre) 0.8 0.6 0.6 0.4 0.4 0.2 0.2 0.0-15 -10-5 0 5 10 15 Off Axis Distance (cm)

Normalized IQM Signal IQM Intrinsic Response (Gradient Direction) 1.60 TB 6X TB 6FFF 10 FFF 6X Agility 1.40 1.20 1.00 0.80 0.60 0.40 0.20 0.00-15 -10-5 0 5 10 15 Off Axis Distance In Transverse Plane (cm)

Normalized IQM Signal IQM Intrinsic Response (None Gradient Direction) 1.05 TB 6X TB 6 FFF 10 FFF 6X Agility 1.00 0.95 0.90 0.85 0.80 0.75-15 -10-5 0 5 10 15 Off Axis Distance In Radial Plane (cm)

IQM Signal Normalized to Centre 1.20 1.15 1.10 Effective IQM Spatial Sensitivity for a 3X3 cm2 field True Beam 6 MV True Beam 10 MV Int Gradient Slope R Value Int Gradient -0.050 1.000 True Beam 6 MV -0.030 0.986 True Beam 10 MV -0.031 0.931 1.05 1.00 0.95 0.90 0.85 0.80-3 -2-1 0 1 2 3 Off axis field shift (cm)

IQM Signal Normalized to Centre Effective IQM Spatial Sensitivity for a 3X3 cm2 field 1.20 1.15 1.10 MLCi2 6 MV MLCi2 18 MV Int Gradient Slope R Value Int Gradient -0.050 1.000 MLCi2 6 MV -0.026 0.997 MLCi2 18 MV -0.024 0.974 1.05 1.00 0.95 0.90 0.85 0.80-3 -2-1 0 1 2 3 Off axis field shift (cm)

IQM Signal Normalized to Centre Effective IQM Spatial Sensitivity for a 3X3 cm2 field 1.20 1.15 1.10 Agility 6 MV Agility 18 MV Int Gradient Slope R Value Int Gradient -0.050 1.000 Agility 6 MV -0.230 0.954 Agility 18 MV -0.012 0.771 1.05 1.00 0.95 0.90 0.85 0.80-3 -2-1 0 1 2 3 Off axis field shift (cm)

IQM Signal Normalized to Centre 1.20 Effective IQM Spatial Sensitivity for a 3X3 cm2 field True Beam 6FFF True Beam 10FFF Int Gradient 1.15 1.10 1.05 1.00 0.95 0.90 0.85 0.80-3 -2-1 0 1 2 3 Off axis field shift (cm)

IQM Response Characteristics Response as a function of field size

Normalized IQM REF Signal 4.50 4.00 REF IQM REF Signal = C x 2 100 3.50 3.00 2.50 2.00 1.50 1.00 0.50 0.00 0 2 4 6 8 10 12 14 16 18 20 Side of square (cm)

Normalized IQM REF Signal 4.5 4 3.5 3 2.5 2 1.5 1 0.5 0 REF 0 2 4 6 8 10 12 14 16 18 20 Side of square (cm) Deviations from REF caused by: Difference in LINAC output with field size Difference in beam flatness and symmetry Difference in beam transmission through collimating elements

IQM Signal Normalized to 10X10 1.0 0.9 0.8 0.7 0.6 0.5 0.4 Signal % Diff With respect to REF Side of Square (cm) True Beam 6 MV True Beam 6 MV ix 6 MV REF ix 6 MV 1-22.2-10.7 3-15.9-12.6 5-9.7-7.6 8-3.3-2.6 10 0.0 0.0 0.3 0.2 0.1 0.0 1 3 5 7 9 Side of square (cm)

IQM Signal Normalized to 10X10 4.5 4.0 3.5 3.0 2.5 Signal % Diff With respect to REF Side of Square (cm) True Beam 6 MV True Beam 6 MV ix 6 MV REF ix 6 MV 10 0.0 0.0 15 5.4 4.0 20 8.8 6.0 2.0 1.5 1.0 0.5 0.0 10 12 14 16 18 20 Side of square (cm)

IQM Response Characteristics Response as a function of beam energy

IQM signal normalized to 6 MV 1.4 True Beam 10 MV Agility 18 MV MLCi2 18 MV ix 18MV 1.2 1.0 0.8 0.6 0 5 10 15 20 Side of square (cm)

IQM signal normalized to 6 MV FFF 1.2 True Beam 10FFF 6 FFF 10 FFF 1.0 0.8 0.6 0 5 10 15 20 Side of square (cm)

IQM Response Characteristics IQM response as a function of dose rates

IQM Dose Rate Dependency (Varian TB) Signal Normalized To 600 MU / Min For 6 MV,10 MV, 6 FFF And Normalized to 800 MU / Min For 10 FFF Dose Rate 6 MV IQM 10 MV IQM 6 FFF IQM 10 FFF IQM 20 1.000 0.999 - - 40 1.001 0.999 - - 100 1.001 0.999 - - 400 1.000 1.000 1.000-600 1.000 1.000 1.000-800 - - 0.999 1.000 1000 - - 1.000-1200 - - 1.000 0.999 1400 - - 1.000-1600 - - - 0.999 2000 - - - 0.999 2400 - - - 0.999

Summary Only minor deviations in IQM intrinsic spatial sensitivity was observed across different energies and platforms The effective spatial sensitivity is affected by beam profile parameters and beam attenuation The signal for square field size depends on the design of the LINAC head components The IQM energy discrimination varies with field size, design of the LINAC head components, and beam profile IQM system exhibits negligible dose rate dependency

Acknowledgments Dr. Mohammad Islam Dr. Robert Heaton Bern Norrlinger Dr. David Jaffray Yinkun Wang Andrew Jung Graham Wilson Dr. Ivan Yeung Marlyn McIntosh Renata Chmielewski Thank You