Beam characterization for the TULIP accelerator for …people.na.infn.it/~mettivie/MCMA...
Transcript of Beam characterization for the TULIP accelerator for …people.na.infn.it/~mettivie/MCMA...
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Beam characterization for the TULIP accelerator for protontherapy
through Full Monte Carlo simulations
C. CuccagnaTERA Foundation (CERN) and University of Geneva
Naples, 17/10/2017
TERA: Vittorio Bencini , Daniele Bergesio , Pedro Carrio Perez , Enrico Felcini , Mohammad Varasteh Anvar , Adriano Garonna , Ugo Amaldi
CERN: Stefano Benedetti , Wioletta Kozlowska , Vasilis Vlachoudis ,
MCMA 2017
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Introduction Methods Results Conclusions
TULIP-Turning Linac for Protontherapy
Beam production and transport system Beam application system
750 MHz
CERN RFQSCDTL
LEBT
≤ 232 MeV
70 MeV+/-110 °
S. Benedetti, A. Grudiev, A.Latina, High Gradient LINACS for ProtontherapyPhysRevAccelBeams 20 040101 2017
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Introduction Methods Results Conclusions
70 MeV
LEBT
≤ 232 MeV
High efficiency Klystron (VDBT)- tested at CERN (I. Siracev)
CERN FeCo magnetprototype (D. Tommasini)
TULIP-Turning Linac for Protontherapy
70 MeV
One Backward Travelling Wave linac tank
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Introduction Methods Results Conclusions
fast longitudinal scanning: ~ 5 msTumor volume
Slice thickness (< 10 mm)
Voxel grid < 10 mmtransverse scanning: < 10
msbeam spots (FWHM: 2-14
mm)
depth in the body
4D active fast spot scanning (ACTIVE and FAST energy variation) suitable for volumetric rescanning
Lower shielding requirement wrt cyclotrons
Small beam emittance (small spots)
Proton LINAC
Courtesy of A. Degiovanni
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Introduction Methods Results Conclusions 55
Generally, for Full Photon Linac MC Modeling
2 Approaches
Phase-space approach
Primary Proton Beam
Source model approach
Calculates particle distribution differential in Energy, position or angle
Follows each particle with all the phase-spaceparameters
+ information in individual particles+ correlation between angle, energy, position preserved- large amount of information to be stored- Computing time
- lost of information on individual particles- approximated
MC techniques in Rad. therapy, Joao Seco, Frank Verhaegen, 2013
Why Full MC simulations for TULIP?
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Introduction Methods Results Conclusions 6
En =142.1 MeV INFORMATION ON INDIVIDUAL PARTICLE for each beam
Why Full MC simulations for TULIP?
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Introduction Methods Results Conclusions 7
660 multi particle files corresponding to different Energy valuesEnergy step ~0.5 MeV
0.13 MeV (≤ 0.1 % dE/E)
Why Full MC simulations for TULIP?
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Introduction Methods Results Conclusions 8
Phase-space files.dat.dst Phase-space files
.dat
Commercial TPS(Physics module)
Methods : Full MC simulations for TULIP
MATLAB Code for the integration
TULIP Beam model files
RFA300·ASCII BDS format
Linac simulations
RF TRACK* Code
Beamproduction
*CERN A. Latina, S.Benedetti
Beam transport lines simulations
MADX-PTC + Code
Beamtransport line
+CERN http://madx.web.cern.ch/madx/
Beamapplication
Beam interaction with:Last magnetsDose delivery systems WATER Phantom/AIR
FLUKA &FLAIR §
§ Ferrari A, Sala PR, Fasso A, Ranft J.
FLUKA: A multi-particletransport code, CERN-2005-10; 2005. INFN/TC05/11, SLAC-R-773
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Introduction Methods Results Conclusions 9
MODEL OF THE NOZZLE
re-adapted from CNAO nozzlespecifications
Box1
Box2
SADX =216.3 cm
SMYSMX
SADY=176.3 cm
Modelled to have an Irradiation field :35x38 cm2
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Introduction Methods Results Conclusions 10
Scanning magnet xy: Magnetic Field in Fluka
SMx
SMy
SADX =216.3 cm
SADY=176.3 cm
ISO
En =232 MeV
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Introduction Methods Results Conclusions 11
Results : Nozzle effect on the beam size
Ea= 107 MeV
ISO
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Introduction Methods Results Conclusions 12
Results : Nozzle effect on the beam size
Ea= 210 MeV
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Introduction Methods Results Conclusions 13
Results: TULIP –Beam Characterization for TPS
1. In-air fluences :
ISO-20 cm
+20 cm
z
y
2. IDD Integral Depth Dose (Bragg’s Peaks)
Distributions in air at isocenter and at other predefinedpoints before and after isocenter(in order to define the beam divergence)
VSAD
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Introduction Methods Results Conclusions 14
Results: TULIP –Beam Characterization for TPS
1. In-air fluences :ISO-20 cm +20 cm
z
y
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Introduction Methods Results Conclusions 15
Results: TULIP –Beam Characterization for TPS
1. In-air fluences :ISO-20 cm +20 cm
z
y
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Introduction Methods Results Conclusions 16
Results: TULIP –Beam Characterization for TPS
1. In-air fluences :ISO-20 cm +20 cm
z
y
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Introduction Methods Results Conclusions 17
2. IDD Integral Depth Dose curves (Bragg’s Peaks)Results: TULIP –Beam Characterization for TPS
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Introduction Methods Results Conclusions 18
2. IDD Integral Depth Dose curves (Bragg’s Peaks)Results: TULIP –Beam Characterization for TPS
80 MeV
210 MeV
232 MeV
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Introduction Methods Results Conclusions 19
Linac simulations
RF TRACK Code
Beamproduction
Beamapplication
Beam interaction with:
Last magnetsDose delivery systems WATERPhantom/AIR/
FLUKA &FLAIR
Beam transport lines simulations
MADX-PTC Code
Beamtransport line
Clinical TPS(Physics module)
Conclusions and future works
DoseComparisons
* Front. Oncol., 11 May 2016 https://doi.org/10.3389/fonc.2016.00116
Dose recalculationsWith clinical TPS
Dose recalculationsWith FLUKA QA MC TPS*And phase-space files
DICOM RT files
PATIENT
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Introduction Methods Results Conclusions 20
Thank you!!Coming together is a beginning
keeping together is progressworking together is success Henry Ford
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Introduction Methods Results Conclusions 21
Results : Nozzle effect on the energy spread
Ea= 73.2MeV
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Introduction Methods Results Conclusions 22
Results : Nozzle effect on the energy spread
Ea= 232.2MeV
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TULIP Optics in MADX
Matching for the complete spectrum of energy:70-232 MeV
Fixed value of Beta at the isocenter in vacuum (beam size ~2.5mm for all energies)
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• Orbit deviation (misalignment) correction
• Multi Particle analysis (PTC) • Optimization and linearization of the quadrupole gradients
• Field error analysis on the harmonic components on dipoles and quadrupoles
TULIP Optics in MADX-PTC
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Introduction Methods Results Conclusions 25
Conclusions and future works
En= 80 MeV
BEFORE NOZZLE En=73 MeV
AFTERNOZZLE
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Introduction Methods Results Conclusions 26
Conclusions and future works
AFTERNOZZLE
En= 122.1 MeVBEFORE NOZZLE En=107.4 MeV
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Introduction Methods Results Conclusions 27
Conclusions and future works
AFTERNOZZLE
En=232.4 MeVBEFORE NOZZLE En=142.1 MeV
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Introduction Methods Results Conclusions 28
Differences wrt the inizial Energy
Dominance energy losses in the nozzle (Landau-Vavilov distribution)
Pencil beam without energy spread
Results
Delta E
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Introduction Methods Results Conclusions 2919.09.2017 29
TULIP –Beam Characterization in air
y = 60.692x-1.719
0.00%
0.50%
1.00%
1.50%
2.00%
2.50%
3.00%
3.50%
4.00%
4.50%
0 50 100 150 200 250
Ener
gy lo
ss(%
)
En (MeV)
Energy loss in the nozzle and air
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Multi particle-Fluka Bragg’s Peak
Comparison with built-in
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31
FLu
ka
Bending effect on the beam in Fluka
Op
era
cod
e
Courtesy of R.Lopez TE-MSC-MNC
Scanning magnet : Complex Map Field Field
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Multi particle-Fluka-Energy straggling
Range stragglingand Energy spread from the accelerator
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Synchrotron for carbon ions (and protons)
CNAO in Pavia from PIMMS TERA/CERN DESIGN
Linacs for protons and carbon ions :
proton linacs: ADAM’s LIGHT and TULIP
Cyclinac & ion linacs for C-12 an He-4– under development
TErapia con Radiazioni Adroniche
Two programmes in accelerators :
AQUA* program in monitoring lead by prof. F.Sauli
*Advanced QUality Assurance
No profit Foundation created in 1992
by prof. U.Amaldi http://enlight.web.cern.ch/sites/enlight.web.cern.ch/files/media/downloads/enlight_highlights_2017-web.pdf
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Physical advantage: the Bragg’s Peak
Radiation beam in matter
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Proton Single Room facility: TULIP
http://medicalphysicsweb.org/cws/article/research/69024
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Proton SourceModulator-klystron
systems
Radio Frequency
Quadrupole (CERN-RFQ)Side Coupled Drift
Tube Linac (SCDTL)Coupled Cavity Linac
(CCL)
AVO-ADAM’s LIGHT proton system
http://www.advancedoncotherapy.com/
Linac for Image Guided Hadron Therapy