Development of elements of 3D planning program for radiotherapy Graphical editor options  automated enclose of contour  correction of intersections 

Slides:



Advertisements
Similar presentations
Image Reconstruction.
Advertisements

بسم الله الرحمن الرحيم ﴿و قل رب زدنى علماً﴾ صدق الله العظيم.
Pencil-Beam Redefinition Algorithm Robert Boyd, Ph.D.
In the past few years the usage of conformal and IMRT treatments has been increasing rapidly. These treatments employ the use of tighter margins around.
Energy deposition and neutron background studies for a low energy proton therapy facility Roxana Rata*, Roger Barlow* * International Institute for Accelerator.
Experience, Expertise and a Commitment to Excellence™
Photon Beam Monitor-Unit Calculations
Computed Tomography III
Optimisation of X-ray micro-tomography to perform low-dose imaging of highly-dosed gels P.M.Jenneson, E.C.Atkinson, P.Wai and S.J.Doran In 1993, Maryanski.
Lotte Verbunt Investigation of leaf positioning accuracy of two types of Siemens MLCs making use of an EPID.
tomos = slice, graphein = to write
Tissue inhomogeneities in Monte Carlo treatment planning for proton therapy L. Beaulieu 1, M. Bazalova 2,3, C. Furstoss 4, F. Verhaegen 2,5 (1) Centre.
Part 1 Introduction to Radiotherapy and External Beam Radiation Deepak Khuntia, MD Vice President, Medical Affairs Varian Medical Systems.
At the position d max of maximum energy loss of radiation, the number of secondary ionizations products peaks which in turn maximizes the dose at that.
Conventional and Computed Tomography
Radiotherapy Treatment Planning
Dose Distribution and Scatter Analysis
بسم الله الرحمن الرحيم و قل رب زدنى علماً ﴿و قل رب زدنى علماً﴾ صدق الله العظيم.
به نام خداوند بخشایندۀ بخشایشگر
The external beam radiotherapy and Image-guided radiotherapy (2)
Augen-Tumor-Therapie mit 68 MeV Protonen am Hahn-Meitner-Institut Berlin C.Rethfeldt / SF4-ATT 1. Ionenstrahllabor ISL 2. Augen-Tumor-Therapie als Anwendung.
Treatment Techniques for the Pelvis Region - Prostate - (- Cervix Ca -) Uwe Götz, Bernd Schicker Institute of Radiation Oncology Limburg, Germany Treatment.
Научно-практический центр протонной лучевой терапии и радиохирургии (Москва-Дубна) A SYSTEM FOR MEASUREMENT OF A THERAPEUTIC PROTON BEAM DOSE DISTRIBUTION.
External Beam Radiotherapy
Kelly Younge, Ph.DKelly Younge, Ph.D Don Roberts, Benedick Fraass, Daniel McShan, and Martha Matuszak University of Michigan, Department of Radiation Oncology,University.
Applications of Geant4 in Proton Radiotherapy at the University of Texas M.D. Anderson Cancer Center Jerimy C. Polf Assistant Professor Department of Radiation.
Radiation Protection in Radiotherapy
In vivo dosimetry Eirik Malinen Eva Stabell Bergstrand Dag Rune Olsen.
Surface dose prediction and verification for IMRT plans using line dose profiles † Ronald E. Berg, † Michael S. Gossman and ‡ Stephen J. Klash † Erlanger.
Seeram Chapter 9: Image Manipulation in CT
May 31, th PTCOG in Catania, Italy1 Treatment Planning for Broad-Beam 3D Irradiation Heavy-Ion Radiotherapy N. Kanematsu, M. Endo, and T. Kanai,
Medical Accelerator F. Foppiano, M.G. Pia, M. Piergentili
RESULTS 4D-Computed Tomography Guided Treatment Planning for Intrahepatic Tumors Yen-Lin Chen, M.D. 1,2, Eike Rietzel, Ph.D. 1,2, Judith Adams 1,2, John.
APPLICATION TO THE HADROTHERAPY FOR OCULAR MELANOMAS G.A. Pablo Cirrone Qualified Medical Physicist and PhD Student University of Catania and Laboratori.
1 Radiotherapy, hadrontherapy and treatment planning systems. Faiza Bourhaleb INFN-Torino University Med 1er-Morocco  Radiotherapy  Optimization techniques.
Physics of carbon ions and principles of beam scanning G. Kraft Biophysik, GSI, Darmstadt, Germany PTCOG43 Educational Satellite Meeting: Principles of.
CT IMAGE RECONSTRUCTION  Hounsfield envisioned dividing a slice into a matrix of 3-dimensional rectangular boxes (voxels) of material (tissue). Conventionally,
Part No...., Module No....Lesson No
F. Foppiano, M.G. Pia, M. Piergentili
Somvilai Mayurasakorn, MD. Division of Therapeutic Radiology and Oncology, Faculty of Medicine, Chiang Mai University Somvilai Mayurasakorn, MD. Division.
Geant4 Activities in Japan Some news from Takashi Sasaki, Koichi Murakami, Akinori Kimura and colleagues.
8/Mar./041st Workshopon the Italy-Japan Collaboration on Geant4 Medical Application 1 Use-Case on treatment planning at HIMAC Koichi Murakami KEK 1 st.
Introduction to Radiation Therapy
Optimization of Volumetric Modulated Arc Therapy (VMAT) Planning Strategy Using Ring-shaped ROI for Localized Prostate cancer Kentaro Ishii, Masako Hosono,
If information seems to be missing, make any reasonable assumptions. 1.A target has an areal density of 2.3 g/cm 2 and a thickness of 0.8 inch. What is.
Purpose N-isopropylacrylamide (NIPAM) polymer gel dosimeters were employed to verify the dose distribution of clinical intensity modulated radiation therapy.
© 2013 MITSUBISHI HEAVY INDUSTRIES, LTD. All Rights Reserved. An example of Technical Innovation Cascade Dynamic Tracking Radiation Therapy System US-Japan.
Thickness of CZT detector 110 MeV140 MeV DETECTOR A (1 mm CZT + 5 mm CZT) DETECTOR B (1 mm CZT + 10 mm CZT) DETECTOR C (1 mm CZT + 15 mm CZT) A. Generation.
Dae-Hyun Kim Dept. of Biomedical Engineering The Catholic University of Korea Department of Biomedical Engineering Research Institute.
Principles and Practice of Radiation Therapy
Koichi MurakamiGeant4 Physics Verification and Validation (17-19/Jul./2006) 1 Results from the recent carbon test beam at HIMAC Koichi Murakami Statoru.
Treatment Chart Record of patients radiation therapy history. Must contain: History and diagnosis Rationale for treatment Treatment plan Consent Documentation.
J Cho, G Ibbott, M Kerr, R Amos, and O Mawlawi
J Cho, G Ibbott, M Gillin, C Gonzalez-Lepera, U Titt and O Mawlawi
Kasey Etreni BSc., MRT(T), RTT, CTIC
Electron Beam Therapy.
Development and characterization of the Detectorized Phantom for research in the field of spatial fractionated radiation therapy. D. Ramazanov, V. Pugatch,
Implementation of Object Spot Avoidance in Proton Pencil Beam Treatment on Whole Breast with Implant Metal Injector Peng Wang, PhD, DABR, Karla Leach,
Reducing Treatment Time and MUs by using Dynamic Conformal Arc Therapy for SBRT Breath-Hold Patients Timothy Miller, Sebastian Nunez Albermann, Besil Raju,
APPLICATION TO THE HADROTHERAPY FOR OCULAR MELANOMAS
Basic Principles of CT Chapter 1.
Chapter 17 Intensity-Modulated Radiation Therapy
Technical Advances of Radiation Therapy for Thymic Malignancies
Innovations in the Radiotherapy of Non–Small Cell Lung Cancer
Hot and cold spots are common problems associated with planning:
Figure 3 Craniospinal irradiation proton therapy for medulloblastoma
GHG meeting at ESTRO36 May, 2017
Surface doses of flattening filter free beams with volumetric modulated arc therapy dose delivery for breast cancer  Jan Seppälä, Aleksi Voutilainen,
Planning techniques of proton boost
Presentation transcript:

Development of elements of 3D planning program for radiotherapy Graphical editor options  automated enclose of contour  correction of intersections  editing of drawing structure  calculating of external contour  calculating sections of structures on anterior and coronal planes Program includes a developed graphical editor which allows drawing anatomical structures on axial CT slices. Main application window Drawing anatomical structures

Anatomical structures sections on anterior view Anatomical structures sections on coronal view

Calculation of aperture of individual collimator Each treatment plan contains one or more sub-plans, so-called treatment prescriptions. Each prescription contains one or more beams (fields). After drawing of anatomical structures program calculates aperture of individual collimator for each beam. Simple round collimator Simple rectangular collimator Individual collimator Multileaf collimator

Calculation of 3D dose distributions A pencil beam algorithm for calculation of 3D dose distribution developed in medical technical complex was incorporated to the program. Calculated dose distribution in a water phantom

Verification of Patient Positioning in Proton Therapy based on Digital X-ray Images Necessary condition! If the proton beam has not the accurate way through the target, we have no full irradiation of important volume of the target and on the other hand we can find over irradiation of critical structures of the brain with located near the target.

Production of the digital X-ray image by digitizer REGIUS170 of Konica Minolta Company takes 20 seconds

Digital reconstruction radiogram (DRR) X-ray image

This program is the first version. In this version the superposition can’t be made without an operator. The next version of the program is being written now and it will have a function for the automatic superposition.

DEVELOPMENT OF A HARDWARE-SOFTWARE SYSTEM FOR A DYNAMIC IRRADIATION METHOD IN PROTON THERAPY Spread-out Bragg peak (SOBP) formation in a passive beam spreading technique in the proton radiation therapy can be conditionally divided into two different methods: irradiation with fixed and variable SOBP. Problem of Fixed SOBP One of the major limitations in the conventional proton therapy technique using range modulation device such as a Ridge Filter, a Fixed Range Shifter and a collimator, is that a fixed width of the SOBP has to cover the 3D target volume. Therefore, it is usually inevitable for the fixed SOBP to extend to healthy tissues. In this case 1/3 of a treated volume is out of the target Idea of Variable SOBP The dynamic irradiation (or layer-stacking method) was proposed to resolve problem of excessively irradiation of healthy tissue in the Fixed SOBP method by producing a variable SOBP without requiring a drastic modification of the conventional beam delivery system. In this case a treated volume is almost equal to the target volume

In the dynamic irradiation technique, a target volume is virtually divided into several thin layers in the depth direction using a Multi-Leaf Collimator and a Dynamic Range Shifter. These imaginary individual layers are treated with the conventional non-modified proton beam, different beam ranges, and conformal fields. Dynamic Irradiation System

Multi-Leaf Collimator Leaf material – steel Number of leaves - 60 Max field size – 100x100 mm Height of one leaf – 2,9mm Individual leaf travel – 100mm Average transmission ~3% max Dynamic Range Shifter Material of the shifter – PMMA Max. thickness at the beam axis – 108mm(H2O) Output scattering angle of about 17,0mrad or 1,0degree

Dynamic Range Shifter and MLC are synchronously controlled with the dose delivery.

* Kanematsu et al.: Treatment planning for the layer-stacking irradiation system. Clinical Effectiveness (expected results) Dose distribution for a tumor in the bone and soft tissue region*; Target contour and the isodose lines are overloaded on the patient CT image for (a) the dynamic irradiation and (b) the conventional irradiation. The yellow line shows the target contour while the isodose lines are in colors of the corresponding dose-percentage numbers shown. Generally effective for – large target volume – single or a few beam directions – small organ motion