DOSE DELIVERY SYSTEM OF THE VARIAN PROBEAM SYSTEM WITH CONTINUOUS BEAM

Similar documents
Implementing a Proton Beam Scanning System within an Operating Clinical Facility

Quality Assurance Implementation at the Roberts Proton Therapy Center. James McDonough 3 August 2013

Promises and Perils of Proton Therapy Beam Delivery (Implications) or Towards Cost Effective Particle Therapy

National Institute of Radiological Sciences. Naoya Saotome

PBS Products from Pyramid

Particle Beam Production - A Synchrotron-Based System - Prof. Dr. Thomas Haberer Scientific-technical Director Heidelberg Iontherapy Center

Recent developments in cyclotrons for proton therapy at IBA

G. Pittá(*), S. Braccini TERA Foundation, Novara, Italy (*) Corresponding author.

Therapy Control and Patient Safety for Proton Therapy

A NOVEL GANTRY FOR PROTON THERAPY AT THE PAUL SCHERRER INSTITUTE

III. Proton-therapytherapy. Rome SB - 3/5 1

The PEFP 20-MeV Proton Linear Accelerator

Particle Therapy with the Varian / ACCEL 250 MeV S.C. Proton Cyclotron

Commissioning of the ATLAS Transition Radiation Tracker (TRT)

CHAPTER 4: HIGH ENERGY X-RAY GENERATORS: LINEAR ACCELERATORS. Jason Matney, MS, PhD

4.9 BEAM BLANKING AND PULSING OPTIONS

Development of New Carbon Therapy Facility and Future Plan of HIMAC

PRESENT STATUS OF J-PARC

Beam Loss Detection for MPS at FRIB

INSTRUMENT CATHODE-RAY TUBE

High Resolution Multicolor Contrast Scanner. Dimensioned drawing

Development of Continuous Line Scanning System Prototype for Proton Beam Therapy

The Construction Status of CSNS Linac

Electrical and Electronic Laboratory Faculty of Engineering Chulalongkorn University. Cathode-Ray Oscilloscope (CRO)

Proton Engineering Frontier Project

Test beam data analysis for the CMS CASTOR calorimeter at the LHC

Commissioning of Accelerators. Dr. Marc Munoz (with the help of R. Miyamoto, C. Plostinar and M. Eshraqi)

High Power Cyclotrons

Hall-B Beamline Commissioning Plan for CLAS12

THE IBA SUPERCONDUCTING SYNCHROCYCLOTRON PROJECT S2C2

-Technical Specifications-

Operation of CEBAF photoguns at average beam current > 1 ma

In-process inspection: Inspector technology and concept

Practicum 3, Fall 2010

In PS 3.3, Section C RT Ion Beams Session Record Module, add the following attributes and make the changes indicated:

An extreme high resolution Timing Counter for the MEG Upgrade

Basic rules for the design of RF Controls in High Intensity Proton Linacs. Particularities of proton linacs wrt electron linacs

Laser Beam Analyser Laser Diagnos c System. If you can measure it, you can control it!

Published text: Institute of Cancer Research Repository Please direct all s to:

Neutron Irradiation Tests of an S-LINK-over-G-link System

EPJ Web of Conferences 95,

RX40_V1_0 Measurement Report F.Faccio

PIECEWISE PRODUCTION MACHINES

An Overview of Beam Diagnostic and Control Systems for AREAL Linac

Advanced Test Equipment Rentals ATEC (2832)

The temperature management of photo cathodes at MAMI and MESA

INCA ENERGY EDS TRAINING. System Block Diagram. INCA Energy Software. Xiang Yang EM SMU. Navigators. Point & ID Navigator.

Detailed Design Report

Joint ICTP/IAEA Advanced School on Dosimetry in Diagnostic Radiology and its Clinical Implementation May 2009

BEAM DIAGNOSTICS IN THE CNAO INJECTION LINES COMMISSIONING

THE NEW LASER FAMILY FOR FINE WELDING FROM FIBER LASERS TO PULSED YAG LASERS

... A COMPUTER SYSTEM FOR MULTIPARAMETER PULSE HEIGHT ANALYSIS AND CONTROL*

New Results on the Electron Cloud at the Los Alamos PSR

arxiv: v1 [physics.ins-det] 1 Nov 2015

Characterization and improvement of unpatterned wafer defect review on SEMs

Approved by: / / R. Battaglia 12/16/2016

Pixel Detector Control System

30 GHz Power Production / Beam Line

Hadron Therapy Technologies

PHY221 Lab 1 Discovering Motion: Introduction to Logger Pro and the Motion Detector; Motion with Constant Velocity

A SQUID-BASED BEAM CURRENT MONITOR FOR FAIR / CRYRING

COMPOSITE VIDEO LUMINANCE METER MODEL VLM-40 LUMINANCE MODEL VLM-40 NTSC TECHNICAL INSTRUCTION MANUAL

BEAMAGE 3.0 KEY FEATURES BEAM DIAGNOSTICS PRELIMINARY AVAILABLE MODEL MAIN FUNCTIONS. CMOS Beam Profiling Camera

Interface Practices Subcommittee SCTE STANDARD SCTE Measurement Procedure for Noise Power Ratio

Beam test of the QMB6 calibration board and HBU0 prototype

HIGH POWER BEAM DUMP AND TARGET / ACCELERATOR INTERFACE PROCEDURES *

Practical Application of the Phased-Array Technology with Paint-Brush Evaluation for Seamless-Tube Testing

Product Brochure Version R&S RSC Step Attenuator Where precise signal levels count

Agilent 5345A Universal Counter, 500 MHz

The hybrid photon detectors for the LHCb-RICH counters

Commissioning and Performance of the ATLAS Transition Radiation Tracker with High Energy Collisions at LHC

Development of an Abort Gap Monitor for High-Energy Proton Rings *

E X P E R I M E N T 1

1.2 Universiti Teknologi Brunei (UTB) reserves the right to award the tender in part or in full.

Report from the 2015 AHCAL beam test at the SPS. Katja Krüger CALICE Collaboration Meeting MPP Munich 10 September 2015

LIGHT PROTON THERAPY PROJECT

Linatron - M9 & M9A. Modular high-energy X-ray source. 2.0 Performance

New Spill Structure Analysis Tools for the VME Based Data Acquisition System ABLASS at GSI

New Filling Pattern for SLS-FEMTO

Application Note #63 Field Analyzers in EMC Radiated Immunity Testing

Semiconductors Displays Semiconductor Manufacturing and Inspection Equipment Scientific Instruments

Low-Energy Electron Linacs and Their Applications in Cargo Inspection

INSTRUMENT CATHODE-RAY TUBE

Introducing Purion H, a Scanned Spot Beam High Current Ion Implanter

DARK CURRENT IN SUPERCONDUCTING RF PHOTOINJECTORS MEASUREMENTS AND MITIGATION

HAPD and Electronics Updates

Development of beam-collision feedback systems for future lepton colliders. John Adams Institute for Accelerator Science, Oxford University

Characterizing Transverse Beam Dynamics at the APS Storage Ring Using a Dual-Sweep Streak Camera

Activities from Cyclotron facility at German Cancer Research Center (DKFZ), Heidelberg

Model 7330 Signal Source Analyzer Dedicated Phase Noise Test System V1.02

The FLASH objective: SASE between 60 and 13 nm

Requirements for the Beam Abort Magnet and Dump

V DD V DD V CC V GH- V EE

Cyclotron Institute upgrade project. H. L. Clark, F. Abegglen, G. Chubarian, G. Derrig, G. Kim, D. May, B. Roeder and G. Tabacaru

Undulator Protection for FLASH and for the European XFEL

Development of high power gyrotron and EC technologies for ITER

A fast and precise COME & KISS* QDC and TDC for diamond detectors and further applications

BitWise (V2.1 and later) includes features for determining AP240 settings and measuring the Single Ion Area.

Commissioning of the CNGS Extraction in SPS LSS4

First LHC Beams in ATLAS. Peter Krieger University of Toronto On behalf of the ATLAS Collaboration

Transcription:

DOSE DELIVERY SYSTEM OF THE VARIAN PROBEAM SYSTEM WITH CONTINUOUS BEAM EUCARD 2 WORKSHOP ON INNOVATIVE DELIVERY SYSTEMS IN PARTICLE THERAPY TORINO, 23 25 FEB 2017 VARIAN PARTICLE THERAPY HOLGER GÖBEL MANGER BEAM DELIVERY

TOPICS Commissioning and performance of Varian ProBeam System - Central Beam - Beam Delivery System - Beam Matching Continuous Beam versus Pulsed Beam - Pencil Beam Scanning - Challenges for Pulsed Beam Treatment Time Dose Monitor Stability

Dynamic Peak Scanning 2 nd Generation IMPT Dynamic Peak Scanning Varian IMPT since 2009 clinical Focus on dedicated scanning nozzles 2 Gy / L / min Documented beam precision <0.5 mm radius sphere 30 x 40 cm field size Total of 17 treatment rooms in Munich, San Diego, Baltimore and Cincinnati 3 VARIAN PARTICLE THERAPY

PROPERTIES BEAM DELIVERY I CENTRAL AXIS BEAM COMMISSIONING RESULTS VARIAN PARTICLE THERAPY

Beamline Bragg Peaks at isocenter peak measurements 5 VARIAN PARTICLE THERAPY

Beamline Fine Steering to Isocenter DEDICATED MEASUREMENT TOOLS DEVELOPED BY VARIAN AUTOMATED AND INTEGRATED INTO COMMISSIONING SOFTWARE TOOL 6 VARIAN PARTICLE THERAPY

Beamline Beam shape at isocenter 7 VARIAN PARTICLE THERAPY

PROPERTIES BEAM DELIVERY II SCANNING BEAM COMMISSIONING RESULTS VARIAN PARTICLE THERAPY

Pro Beam Delivery Nozzle Scanning Magnets asi Flat Panels (kv imaging) Vacuum Chamber Dose and Position Monitors Nozzle extension for Range-Shifter(s) 9 VARIAN PARTICLE THERAPY

Spot measurements with imaging system 244 MeV 69 MeV Active detection area 30cm x 40cm 10 VARIAN PARTICLE THERAPY

Scanning Magnets uncalibrated SPTC TR3 11 VARIAN PARTICLE THERAPY

Scanning Magnets calibrated SPTC TR3 12 VARIAN PARTICLE THERAPY

PROPERTIES BEAM DELIVERY III BEAM MATCHING BETWEEN ROOMS VARIAN PARTICLE THERAPY

Pencil Beam Scanning Commissioning of ECLIPSE Treatment Planning System PENCIL BEAM SCANNING ALGORITHM RELATIVE INTEGRATED DEPTH DOSE CALIBRATION OF DEPTH DOSE CURVES 2D SPOT SHAPES AT DIFFERENT DISTANCES ALL MEASUREMENTS CAN BE ACQUIRED WITHIN LESS THAN A DAY 14 VARIAN PARTICLE THERAPY

IPDD [%] Matching of beam data: PDDs PDDs measured at different gantries 120 100 typical residual of two PDDs (230 MeV, different gantries) 80 60 40 20 0-1 Residual of 2 Bragg Peaks of same beam energy at two different gantries -2-3 0 50 100 150 200 250 300 350 400 depth in water [mm] 15 VARIAN PARTICLE THERAPY

Pencil Beam Scanning Dose-to-MU Output Calibration STABLE PERFORMANCE OF SYSTEM NO DAILY OUTPUT ADJUSTMENTS NECESSARY DD<1% NO GANTRY ANGLE DEPENDENCE LONG-TIME STABILITY initial system setup in San Diego vs. RPTC Munich 16 VARIAN PARTICLE THERAPY

planned vs. measured dose INTITAL SETUP OF TREATMENT PLANNING SYSTEM WITHOUT REFINEMENTS CUBIC VOLUMES IRRADIATED AND DISTIBUTION MEASURED WITH PTW 2DARRAY PASSRATE 99% FOR GAMMA-TEST (3%/3MM) (2Gy central TR3/16Aug2013) 17 VARIAN PARTICLE THERAPY

CONTINUOUS BEAM VERSUS PULSED BEAM CHALLENGES VARIAN PARTICLE THERAPY

Pencil Beam Scanning Scanning Control System One subsystem out of many for Proton Therapy System Treatment Planner (Eclipse ) User Interface treatment results Gantry angle for the field, energy for each layer, (x, y, MU) for each spot start, hold and pause irradiation progress data Scanning Subsystem beam current and Energy for each layer Turn beam on and off, Terminate irradiation Beam Adjustment Server Proton Cyclotron Controls beam current 19 VARIAN PARTICLE THERAPY

Pencil Beam Scanning Sequence during irradiation 1. Adjust beam energy 2. Set scanning magnet currents for first spot 3. Regulate the required accelerator beam current 4. Start irradiation 5. Measure monitor units until switch limit reached 6. Move beam to next spot (w/ or wo/ beam turned off) 7. Goto 5) until last spot in layer 8. Switch off beam and goto 1) until last layer Add-ons Checking various devices Pause, resume, or terminate irradiation at any time Acquire irradiation results 20 VARIAN PARTICLE THERAPY

Spot position Spot position Pencil Beam Scanning Scanning Method Far away spot Close spot Beam on time Beam on time 21 VARIAN PARTICLE THERAPY

POSITION DOSE BEAM Pencil Beam Scanning Scanning Method DOSE DRIVEN SPOT SCANNING D 1 D 2 D3 ON OFF CONTINUOUS BEAM FROM CYCLOTRON FAST BEAM ON/OFF BETWEEN CONSECUTIVE SPOTS IN E.G. MEANDER PATTERN OPTIMIZED DELIVERY FOR SHORT TREATMENT TIMES TIME DEFLECTION IN X- AND Y-DIRECTION:. 0,3 0,5 ms (spot to spot) Irradiation pattern /order of spots is given by treatment plan VARIATION OF ENERGY LAYER: < 0.9s. TYPICAL SPOT DURATION: 3 50 ms 22 VARIAN PARTICLE THERAPY

Pencil Beam Scanning 23 VARIAN PARTICLE THERAPY

Pencil Beam Scanning Basic Characteristics for Scanning Technique FEATURE energy range at isocenter average dose rate maximum field size at isocenter beam accuracy at isocenter (radius) SCANNING Typically 70-245 MeV 2 Gy / l / min 30 x 40 cm 1 mm nominal spot size (one sigma value) 5.4 4 mm (+/- 15%) layer switching time IMPT capable < 0.9 s yes 24 VARIAN PARTICLE THERAPY

POSITION DOSE BEAM Continuous beam versus pulsed beam Challenges Precision and a minimum spot weight of 1cGy at Bragg Peak and total spot area (1cm 2 ) translates into 8 10 6 protons at 70 MeV and 2.5 10 7 protons at 250 MeV ON OFF Spots with high spot weight up to 50cGy: 4 10 8 protons at 70 MeV and 1 10 9 protons at 250 MeV (4mm spot spacing, focused beam) TIME Time to switch to the next spot / switch off the beam @ high dose rates: ~200µs With a continuous beam, one can predict, when to switch 25 VARIAN PARTICLE THERAPY

Continuous beam versus pulsed beam Challenges Several pulses will be needed to get to the needed precision: Case 1: precision 2% per spot, uncertainty of the number of protons per pulse 20% => the planned MU per spot can be irradiated with 3 pulses: 83% + 14% + 3% Case 2: precision 2%, uncertainty of the number of protons per pulse 50% => the planned MU per spot can be irradiated with 5 pulses 67% + 22% + 7% + 3% + 1% If the beam is off, this amount of contribution of a pulse to the whole spot is too high, in order to stay within the 0,25 Gy to terminate the irradiation, and second for steering of the beam position, one needs to reduce the contribution of each pulse even more. 26 VARIAN PARTICLE THERAPY

Continuous beam versus pulsed beam Challenges A high beam current in the pulse is needed due to low duty factor in order to keep treatment time low Very good control of number of protons extracted per pulse by the accelerator High variability of the number of protons extracted per pulse in order to irradiate spots with high spot weight fast enough and with the needed precision Control loop and interfaces for the next pulse must be very fast in order to take into account the already delivered monitor units (collecting time of ionization chamber is ~100-200µs) and the measured beam position 27 VARIAN PARTICLE THERAPY

Continuous beam versus pulsed beam Challenges Saturation effects at high beam currents have to be corrected for the used primary and secondary dose monitor system Saturation of commercial available dosimetry equipment may be possible 70MeV: 8 10 6 protons / 10µs = 128nA in the peak (0.13nA averaged) 250MeV: 2.5 10 7 protons / 10µs = 400nA in the peak (0.4nA averaged) 70MeV: 4 10 8 protons / 10µs = 6.4µA in the peak (6.4nA averaged) 250MeV: 1 10 9 protons / 10µs = 20µA in the peak (20nA averaged) (average curent for 1kHz beam pulse repetiton) Beam position and beam width measurement have to be synchronous with the pulse beam time structure 28 VARIAN PARTICLE THERAPY

Continuous beam versus pulsed beam Impact on treatment time Increase the minimum spot weight from 1 cgy to several cgy in order to delivery faster with a focused beam, AND to still keep the clinical requirements Enlarge the spots by using a range-shifter as a scatterer in order to delivery faster by lowering the precision specifications and by increasing the minimum spot weight, BUT with a much less dose conformity than with focused beam. 29 VARIAN PARTICLE THERAPY

PROPERTIES BEAM DELIVERY IV TREATMENT TIME DOSE MONITOR STABILITY VARIAN PARTICLE THERAPY

Fast Treatment times Lung case Summary of treatment times (calculated) No layer switch time 200 ms 500 ms 900 ms 2F Plan Field 1/2 6.6 s 7.8 s 9.6 s 12 s Field 2/2 7.6 s 9 s 11.1 s 13.9 s 3F Plan Field 1/3 4 s 4.8 s 6 s 7.6 s Field 2/3 4.1 s 4.9 s 6.1 s 7.7 s Field 3/3 3.5 s 4.7 s 6.5 s 8.9 s 31 VARIAN PARTICLE THERAPY

Case 1 Liver Motion Managed Using Gating Moving shallow liver tumor of close to 1 Liter in size 2 field treatment 15 fractions of 4.5 Gy The Qfix SDX spirometry system was used 32 VARIAN PARTICLE THERAPY

Case 1 Liver Motion Managed Using Gating Fast beam delivery aids in motion management Field 1 delivered in 2 breath-holds Field 2 delivered in 1 breath-hold 33 VARIAN PARTICLE THERAPY

deviation (%) Dose Monitor Stability Stability Results of the absolute dose measurements over a 6months period Deviation measuremant to referenz [%] 03 02 01 00-01 chamber 1 chamber 2 chamber 3 chamber 4 chamber 5-02 -03 time data courtesy of Mr Skalsky / RPTC Munich 34 VARIAN PARTICLE THERAPY

Planned vs measured dose 10cm x 10cm x 10 cm @ 15 cm depth Gamma Criteria of 3%/3mm: 98.5% (green area) 35 VARIAN PARTICLE THERAPY

Dynamic Peak Scanning 2 nd Generation IMPT Dynamic Peak Scanning Varian IMPT since 2009 clinical Focus on dedicated scanning nozzles 2 Gy / L / min Documented beam precision <0.5 mm radius sphere 30 x 40 cm field size Total of 17 treatment rooms in Munich, San Diego, Baltimore and Cincinnati 36 VARIAN PARTICLE THERAPY

Summary Pencil Beam Scanning with continuous beam High experience in clinical environment Short irradiation time per field, even within one breath hold Dose delivery is very stable very good dose conformity Well understood technology installation, commissioning and service can be handled by technicians not experts 37 VARIAN PARTICLE THERAPY

THANK YOU FOR YOUR ATTENTION THANKS TO THE ORGANIZERS VARIAN PARTICLE THERAPY HOLGER GÖBEL MANGER BEAM DELIVERY