A pixel chamber as beam monitor for IMRT S. Belletti 4, A.Boriano 6, F.Bourhaleb 5,7, R. Cirio 6, M. Donetti 5,6, B. Ghedi 4, E. Madon 2, F. Marchetto.

Slides:



Advertisements
Similar presentations
Cirrone G. A. P. , Cuttone G. , Raffaele L. , Sabini M. G
Advertisements

Chapter 4 Radiation Dosimeters
Ionization Chamber Array for External Beam Radiotherapy
RapidArc plan verification using ArcCHECK™
The pixel ionisation chamber: a detector for beam monitor and dosimetry A.Boriano 1,2, F.Bourhaleb 2,3, R. Cirio 2, M. Donetti 2,4, F. Marchetto 2, C.
TileCal Electronics A Status Report J. Pilcher 17-Sept-1998.
Lic. Pedro Antonio Pérez.  To develop a simple and versatile dosimetric method capable of determining changes in matter (Xylenol Orange added Fricke.
Lotte Verbunt Investigation of leaf positioning accuracy of two types of Siemens MLCs making use of an EPID.
Design and test of a high-speed beam monitor for hardon therapy H. Pernegger on behalf of Erich Griesmayer Fachhochschule Wr. Neustadt/Fotec Austria (H.
Mauro Raggi Status report on the new charged hodoscope for P326 Mauro Raggi for the HODO working group Perugia – Firenze 07/09/2005.
DOSIMETRY COMMISSIONING OF THE LNS-INFN PROTON THERAPY FACILITY THE DOSIMETRIC CHARACTERISTICS OF NARROW PROTON BEAMS USED IN EYE THERAPY HAVE BEEN DEFINED.
Performances of a pixel ionization chamber to monitor a voxel scan hadron beam A.Boriano 3, F.Bourhaleb 2,3, R. Cirio 3, M. Donetti 2,3, F. Marchetto 3,
Dosimetric evaluation of a new design MOSFET detector Per H. Halvorsen* & Stephanie Parker University of North Carolina.
Michele Togno ARDENT ESR 11 – 2D Ionization Chambers Array for Clinical Applications Michele Togno – ARDENT midterm review preparatory meeting, CERNJune,
Quality Control in Radiation Therapy, A New Concept: Dosimetry Check
PAIR SPECTROMETER DEVELOPMENT IN HALL D PAWEL AMBROZEWICZ NC A&T OUTLINE : PS Goals PS Goals PrimEx Experience PrimEx Experience Design Details Design.
Научно-практический центр протонной лучевой терапии и радиохирургии (Москва-Дубна) A SYSTEM FOR MEASUREMENT OF A THERAPEUTIC PROTON BEAM DOSE DISTRIBUTION.
Why silicon detectors? Main characteristics of silicon detectors: Small band gap (E g = 1.12 V)  good resolution in the deposited energy  3.6 eV of deposited.
Test of the proposed method Introduction CCD Controller CCD Illuminator gel Filter 585nm Assembling the phantom before its irradiation. The phantom, ready.
In vivo dosimetry Eirik Malinen Eva Stabell Bergstrand Dag Rune Olsen.
The Magic Cube and the Pixel Ionization Chamber: detectors for monitor and dosimetry of radiotherapy beams S. Amerio 1, A. Boriano 2, F. Bourhaleb 2,3,
Application of a 2-D ionization chamber array for dose verification of dynamic IMRT with a micro-MLC Fujio ARAKI, PhD 1, S. TAJIRI 2, H. TOMINAGA 2, K.
Medical Accelerator F. Foppiano, M.G. Pia, M. Piergentili
Use of the IC Profiler detector array for comprehensive machine QA ESTRO QA & Dosimetry Satellite Symposium Steve Morgan, Medical Physics Dept,
Araki F. Ikegami T. and Ishidoya T.
AIR CORE SCINTILLATION DOSIMETER SUMMARY We have shown that Cerenkov light can be reduced to a negligible level in scintillation dosimetry by using an.
A solution for dosimetry and quality assurance in IMRT and hadrontherapy: the pixel ionization chamber. S. Amerio a, S. Belletti b, A. Boriano c, R. Cirio.
Total Cross Section, Elastic Scattering and Diffraction Dissociation at the LHC January 17, 2003TOTEM plenary meeting -Marco Bozzo1 CSC detectors for T1.
DEAR SDD --> SIDDHARTA
K. Matsuoka (Kyoto Univ.) for T2K muon monitor group
R. Pani Department of Experimental Medicine and Pathology University of Rome La Sapienza-Italy. Flat Panel PMT: advances in position sensitive photodetection.
SIDDHARTA future precision measurement of kaonic atoms at DA  NE Florin Sirghi LNF SPRING SCHOOL "Bruno Touschek" In Nuclear, Subnuclear and Astroparticle.
The development of the readout ASIC for the pair-monitor with SOI technology ~irradiation test~ Yutaro Sato Tohoku Univ. 29 th Mar  Introduction.
LHC Beam Loss Monitors, B.Dehning 1/15 LHC Beam loss Monitors Loss monitor specifications Radiation tolerant Electronics Ionisation chamber development.
On a eRHIC silicon detector: studies/ideas BNL EIC Task Force Meeting May 16 th 2013 Benedetto Di Ruzza.
A. G. Argentieri 1), E. Cisbani 2), S. Colilli 2), F. Cusanno 2), R. De Leo 1), R. Fratoni 2), F. Garibaldi 2), F. Giuliani 2), M. Gricia 2), M. Lucentini.
TLD POSTAL DOSE QUALITY AUDIT FOR 6MV AND 15MV PHOTON BEAMS IN RADIOTHERAPY CLINICAL PRACTICE Sonja Petkovska 1, Margarita Ginovska 2, Hristina Spasevska.
FrontierScience G.P.1 MATRIX an innovative Pixel Ionization Chamber for Online Monitoring of Hadrontherapy Treatments Giuseppe Pittà.
J. Alozy, S. George, F.Murtas, M. Silari 1 CERN GEMPIX detectors as hadron therapy beam monitors and radioactive waste detectors GEMPIX construction.
Implementation of a New Monte Carlo Simulation Tool for the Development of a Proton Therapy Beam Line and Verification of the related Dose Distributions.
NUMI Primary Beam Review August 14, 2001 NUMI PRIMARY BEAM INSTRUMENTATION Multiwires, Loss Monitors, Toroids Gianni Tassotto.
Beam Profile Monitor for Spot-Scanning System Yoshimasa YUASA.
Siena, May A.Tonazzo –Performance of ATLAS MDT chambers /1 Performance of BIL tracking chambers for the ATLAS muon spectrometer A.Baroncelli,
SDHCAL. outline  SDHCAL concept, validation and construction  Test Beam and technological prototype performance  Perspectives and Conclusion  SDHCAL.
Update on works with SiPMs at Pisa Matteo Morrocchi.
WP 7 (RDH) Detector for high intensity beam WP 6 (IRPT) New TERA chip development Leslie Karen Fanola Guarachi.
Philip Bambade, Pierre Barillon, Frédéric Bogard, Selma Conforti, Patrick Cornebise, Shan Liu, Illia Khvastunov Journée PHIL
Attività WP8: sviluppo sistema dosimetrico INFN Firenze M. Bruzzi, M. Bucciolini, E. Pace, M. Scaringella, C. Talamonti, M. Zani, A. Baldi.
V.Aulchenko 1,2, L.Shekhtman 1,2, B.Tolochko 3,2, V.Zhulanov 1,2 Budker Institute of Nuclear Physics, , Novosibirsk, Russia Novosibirsk State University,
CONFIDENTIAL MATERIAL Michele Togno - II Annual ARDENT Meeting, Milan – October, 14 th D Ionization Chambers Array for Clinical Applications.
Study of the Radiation Damage of Hamamatsu Silicon Photo Multipliers Wander Baldini Istituto Nazionale di Fisica Nucleare and Universita’ degli Studi di.
Beam detectors in Au+Au run and future developments - Results of Aug 2012 Au+Au test – radiation damage - scCVD diamond detector with strip metalization.
Page Detector and Electronics R&D for picosecond resolution, single photon detection and imaging J.S. MilnesPhotek Ltd T.M. ConneelyUniversity.
 13 Readout Electronics A First Look 28-Jan-2004.
Dosimetry with diamond detectors G. Gervino1, C. Marino1, F
Silicon microstrip detector for imaging of fast processes at high intensity synchrotron radiation beam. Budker INP V.Aulchenko1,2, L.Shekhtman1,2, B.Tolochko3,2,
Entrance Muon Counter (EMC)
Triple GEM detectors : measurements of stray neutron.
Dr: Mohamed Afifi By Lecturer Radiological Science
HERD Prototype Beam Test
IHEP group Shashlyk activity towards TDR
AQUA-ADVANCED QUALITY ASSURANCE FOR CNAO
Influence of the grid size on the dosimetric characteristics of IMRT beams and on overall treatment plans G. Pittomvils1, L. Olteanu1, B. Vanderstraeten1,
Gaseous Beam Position Detectors, with Low Cost and Low Material Budget
Arghya Chattaraj, T. Palani Selvam, D. Datta
A First Look J. Pilcher 12-Mar-2004
BESIII EMC electronics
AIMS 1- Build SDHCAL prototype of 1m3 as close as possible to the one
Why silicon detectors? Main characteristics of silicon detectors:
Gain measurements of Chromium GEM foils
Presentation transcript:

A pixel chamber as beam monitor for IMRT S. Belletti 4, A.Boriano 6, F.Bourhaleb 5,7, R. Cirio 6, M. Donetti 5,6, B. Ghedi 4, E. Madon 2, F. Marchetto 6, U. Nastasi 3, C. Peroni 6, C.J. Sanz Freire 1,6, E. Trevisiol 2 1 IBA, Ion Beam Applications, Louvain la-Neuve, Belgium 2 OIRM S. Anna, Torino, Italy 3 Servizio di Fisica Sanitaria, S. Giovanni A.S. Hospital, Torino, Italy 4 Servizio di Fisica Sanitaria, Spedali Civili, Brescia, Italy 5 TERA Foundation, Novara, Italy 6 University and INFN, Torino, Italy 7 University Mohamed First, Oujda, Morocco

1 st Euro-mediterranean meeting on radiotherapy –Oujda (Morocco) Outline Outline IMRT measurements IMRT measurements Mechanical structure of the pixel ionisation chamber Mechanical structure of the pixel ionisation chamber Read-out: electronics and performances Read-out: electronics and performances Characterization of the detector with hadron beams Characterization of the detector with hadron beams Characterization of the detector with photon beams Characterization of the detector with photon beams

1 st Euro-mediterranean meeting on radiotherapy –Oujda (Morocco) The pixel chamber   parallel plate ionization chamber   anode segmented in 1024 square pixels   pixel dimension = 7.5 x 7.5 mm 2   sensitive area = 24 x 24 cm 2   1 mm water equivalent thickness   front-end electronics, located around the chamber, to perform analog to digital conversion

1 st Euro-mediterranean meeting on radiotherapy –Oujda (Morocco) Detector design When used in plastic phantom the detector can be thick. Anode and cathode are glued to a plastic slab, which is a grid of 1024 holes. Each hole can be considered as an independent sensitive volume and the material around provides lateral electronic equilibrium.

1 st Euro-mediterranean meeting on radiotherapy –Oujda (Morocco) Detector design

1 st Euro-mediterranean meeting on radiotherapy –Oujda (Morocco) Front-end electronics   located around the chamber   we have developed a full custom chip (TERA05)   every chip has 64 channels. Each one converts the charge collected by a pixel into counts

1 st Euro-mediterranean meeting on radiotherapy –Oujda (Morocco) Linearity at 100 fC charge quantum   20 pA < I < 0.6  A   Linearity better than 0.7 %

1 st Euro-mediterranean meeting on radiotherapy –Oujda (Morocco) Linearity at 600 fC charge quantum   10 pA < I < 2  A   Linearity better than 0.3 %

1 st Euro-mediterranean meeting on radiotherapy –Oujda (Morocco) Reproducibility of charge quantum   I = nA   Qc = 600 fC   24 ºC < T < 27 ºC   1 month   6 measures

1 st Euro-mediterranean meeting on radiotherapy –Oujda (Morocco) Beam test at PSI (CH) PSI test with a 138 MeV proton beam PSI test with a 138 MeV proton beam 7 mm FWHM beam 7 mm FWHM beam Spot-scanning Spot-scanning Uniformity of the response ~0.9% Uniformity of the response ~0.9% Profiles measurement ok Profiles measurement ok

1 st Euro-mediterranean meeting on radiotherapy –Oujda (Morocco) Beam test at GSI (D) Beam characteristics   raster-scan delivery system   C +6, beam dimension = 8.8 mm (FWHM)   data acquisition synchronized with raster-scan Aims   spatial resolution   homogeneity of response

1 st Euro-mediterranean meeting on radiotherapy –Oujda (Morocco) Spatial resolution: 16 spot

1 st Euro-mediterranean meeting on radiotherapy –Oujda (Morocco) Spatial resolution Spatial resolution  < 0.2 mm

1 st Euro-mediterranean meeting on radiotherapy –Oujda (Morocco) Homogeneity of the response 18 × 18 cm 2 uniform field  = 1.1 %  = 2.0 %

1 st Euro-mediterranean meeting on radiotherapy –Oujda (Morocco) Q.A. with photon beams A Quality Assurance protocol establish:  Physic and dosimetric parameters to be measured  Procedures followed for the measurements  Frequency of the controls  Reference values 1. 1.Homogeneity, symmetry, penumbra, energy stability 2. 2.Calibration of the monitor system, stability. Conventional instrumentation:  Thimble ion chamber (Farmer) One point measurement  Diode array 1D measurement

1 st Euro-mediterranean meeting on radiotherapy –Oujda (Morocco) Q.A. with photon beams S. Giovanni A.S. and S. Anna hospitals – Torino Aims   Depth dose profile measurements and comparison to a reference ion chamber (Farmer)   Profile measurements and comparison Measurements to a reference ion chamber   Stability of the response To perform these kind of measurements, there are no time constrains. The only information needed is the final measurement

1 st Euro-mediterranean meeting on radiotherapy –Oujda (Morocco) Depth dose curve Depth dose profiles have been measured for different photon energy. We have used a Farmer ion chamber in a plastic phantom as a reference An excellent agreement has been found for each photon energy.

1 st Euro-mediterranean meeting on radiotherapy –Oujda (Morocco) Profiles Profile comparison with a Farmer in a water phantom Field 10 X 10 cm 2 Depth 10 cm Field 20 X 20 cm 2 Depth 10 cm

1 st Euro-mediterranean meeting on radiotherapy –Oujda (Morocco) Profiles Field 5 X 5 cm 2 Depth 10 cm

1 st Euro-mediterranean meeting on radiotherapy –Oujda (Morocco) Long-term stability Stability measured during a one month period Stability measured during a one month period Stability within 1.5% Stability within 1.5% Mechanical problem caused variations in the sensitive volume Mechanical problem caused variations in the sensitive volume ±1% ±5%

1 st Euro-mediterranean meeting on radiotherapy –Oujda (Morocco) IMRT measurements Dynamic wedge case By moving each side of the collimator with different speed one obtains a wedge shape of the dose At the end of the treatment one has to check the delivered dose in different points The pixel ion chamber can measure precisely the 2D dose in 1024 points.

1 st Euro-mediterranean meeting on radiotherapy –Oujda (Morocco) IMRT measurements The pixel ion chamber has a fast read out. Every 1ms a complete read out can be performed. It is possible to monitor the 2D dose in real time. Dynamic multi leaves collimator (DMLC) case: independent leaves can be moved to shape the beam field one needs to check as a function of time the 2D delivered dose

1 st Euro-mediterranean meeting on radiotherapy –Oujda (Morocco) IMRT measurements Total dose delivered Example: small square dose distribution going to large square dose distribution

1 st Euro-mediterranean meeting on radiotherapy –Oujda (Morocco) IMRT measurements Delivered dose in function of time Time: 0 secTime: 1 secTime: 2 secTime: 3 secTime: 4 secTime: 5 secTime: 6 secTime: 7 secTime: 8 secTime: 9 secTime: 10 secTime: 11 secTime: 12 secTime: 13 secTime: 14 sec

1 st Euro-mediterranean meeting on radiotherapy –Oujda (Morocco)

1 st Euro-mediterranean meeting on radiotherapy –Oujda (Morocco) Detector design Thin version When used as monitor the detector has to be thin to minimize the changes on the beam energy and shape. For this configuration, anode and cathode are glued to frames in order to assure the mechanical rigidity and the gap thickness. Water equivalent thickness < 1 mm.

1 st Euro-mediterranean meeting on radiotherapy –Oujda (Morocco) Read out electronics Recycling Integrator architecture.

1 st Euro-mediterranean meeting on radiotherapy –Oujda (Morocco) TERA05 Very Large Scale Integration (VLSI) i  f conversion output  Q int 100 fC<charge quantum<800 fC I max = 4  A 64 channels 16 bit wide counters multiplexed digital output dead-time free readout max read out rate = 10 MHz channel # 1 channel # 64

1 st Euro-mediterranean meeting on radiotherapy –Oujda (Morocco) Fast Data acquisition Signals (RS422 standard) are delivered via twisted pair flat cables (100 m maximum length) max transfer rate = 10 MHz = 40 Mbyte/s read out transfer time = 50  s read out cycle total time = 100  s real time operating system <100 m

1 st Euro-mediterranean meeting on radiotherapy –Oujda (Morocco) Slow Data acquisition connection by twisted pair flat cables (100 m max) max rate transfer = 1 MHz = 2 Mbyte/s read out transfer time = 1 ms PCI DAQ card LabVIEW software cheap solution easy to handle Slow data acquisition

1 st Euro-mediterranean meeting on radiotherapy –Oujda (Morocco) Reproducibility Several measurements have been performed to evaluate the reproducibility. After a pre-irradiation reproducibility is better than 1% 100 MU per irradiation field bigger than sensitive volume

1 st Euro-mediterranean meeting on radiotherapy –Oujda (Morocco) OUTPUT FACTOR 3.4% No solution so far: Higher sensitivity of the pixel chamber to low energy photons due to a different structure Disagreement between the pixel chamber and the Farmer