geant4 based monte carlo simulations of a transport beam
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MCMA 2017 Napoli, Italy 17 th October 2017 Geant4-based Monte Carlo simulations of a transport beam line for multidisciplinary applications of laser-driven proton beams Giuliana Milluzzo On behalf of the ELIMED collaboration INFN -


  1. MCMA 2017 Napoli, Italy 
 17 th October 2017 Geant4-based Monte Carlo simulations of a transport beam line for multidisciplinary applications of laser-driven proton beams Giuliana Milluzzo On behalf of the ELIMED collaboration INFN - Laboratori Nazionali del Sud, Catania, Italy Università degli Studi di Catania G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it 1

  2. Conventional RF accelerators vs laser-driven for hadrontherapy 2 • An intense laser field (> 10 18 W/cm 2 ) blows off electrons from a target surface • Fast electrons penetrate the foil and ionize atoms along their path à a strong electric field is created (≈ TV/m) In a few microns mul0-Mev protons and ions are accelerated G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it

  3. Laser-driven beams peculiarities 3 • Wide angular distribu2ons • Large energy spread • Extremely high dose rate per pulse New paradigms for 10 7 -10 9 Gy/min (vs 10-50 Gy/min) beam dosimetry G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it

  4. ELIMED beam line layout 4 4 Collection and diagnostics Selection, transport and diagnostics Dosimetry and sample irradiation Front. Oncol. (in press) NIM A, Vol. 829 (2016) JINST, Vol. 11 (2016) Graphics by L. Allegra JINST, Vol. 10 (2015) G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it

  5. ELIMED WPs 5 G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it

  6. ELIMED WPs 5 G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it

  7. The ELIMED application J. Pipek, F. Romano, G. Milluzzo et al.,, Journal of Instrumentation, Volume 12, March 2017 6 Application structure Requirements from ELI Component realistic model Easily modify geometrical configurations Magnetic and electric field implementation Accurate transport in magnetic fields Realistic laser-driven particle source User friendly Information scoring along the beamline PMQs Energy selector system Source Conventional transport elements Dosimetry devices OUTPUT 70 PIC simulation 60 50 40 30 20 10 0 20 100 40 60 80 G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it

  8. The ELIMED application as a tool for beam optimization and feasibility studies for multi-disciplinary applications G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it

  9. 60 MeV ΔE/E Tr. Eff. 11% 9.9% 8% 8.0% 7% 4.9% G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it

  10. 60 MeV ΔE/E Tr. Eff. 11% 9.9% 8% 8.0% 7% 4.9% G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it

  11. 2 m air + 100 um Ta 2 m air + 300 um Ta + 10 mm collimator + 20 mm collimator 10 % 10 % 10 mm 20 mm G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it

  12. Towards dose delivery of clinical relevance: feasibility studies for multi-disciplinary applications G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it

  13. ESS as an active energy modulator? 11 PMQs configuration fixed for the maximum energy transport optimization (60 MeV) 4 10 3 10 Counts 2 10 1 10 10 20 30 40 50 60 70 Energy [MeV] G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it

  14. ESS as an active energy modulator? 11 PMQs configuration fixed for the maximum energy transport optimization (60 MeV) 4 10 3 10 Counts range in 2 10 water between 1 1 and 2 cm 10 10 20 30 40 50 60 70 Energy [MeV] G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it

  15. ESS as an active energy modulator? 11 Protons in the energy selector PMQs configuration fixed for the maximum energy transport optimization (60 MeV) 4 10 3 10 Counts range in 2 10 water between 1 1 and 2 cm 10 10 20 30 40 50 60 70 Energy [MeV] G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it

  16. ESS as an active energy modulator? 11 Protons in the energy selector PMQs configuration fixed for the maximum energy transport optimization (60 MeV) 4 10 3 10 Counts range in 2 10 water between 1 1 and 2 cm 10 10 20 30 40 50 60 70 Energy [MeV] G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it

  17. ESS as an active energy modulator? 11 Protons in the energy selector PMQs configuration fixed for the maximum energy transport optimization (60 MeV) 4 10 3 10 Counts range in 2 10 water between 1 1 and 2 cm 10 10 20 30 40 50 60 70 Energy [MeV] G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it

  18. ESS as an active modulator: results 12 G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it

  19. ESS as an active modulator: results 12 3% of dose homogeneity in 2 cm of modula5on region! G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it

  20. ESS as an active modulator: results 12 3% of dose homogeneity in 2 cm of modula5on region! Normalization to typical doses per session delivered in ocular melanoma proton treatments (15 Gy) Re-calculation of the absolute weights (in Gy) of any single peak Computation of number of shots per single peak to achieve the required dose G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it

  21. ESS as an active modulator: results 12 3% of dose homogeneity in 2 cm of modula5on region! Normalization to typical doses per session delivered in ocular melanoma proton treatments (15 Gy) Re-calculation of the absolute weights (in Gy) of any single peak Computation of number of shots per single peak to achieve the required dose ̴ 1000 shots in total Considering both laser repetition rate and and ESS field frequency oh 1 Hz ̴ 16 minutes Considering laser repetition rate of 10 Hz and and ESS field frequency oh 1 Hz ̴ 2 minutes G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it

  22. Conclusions and future developments 13 Conclusions • ELIMED application has been designed to be a Geant4 User-oriented application • Geant4 fits well all the requirements from ELI management: • Simulate complex geometrical elements with the possibility to switch on/off components modularity • Easy methods for changing geometrical configurations interactive commands • Reliability for particle transport in magnetic fields robust tracking • Accurate energy/dose depositions predictions and secondary particles production -> well tested and validated physics models • User-friendly and easy-to-use for non experienced Users -> Qt interface with the possibility of changing all the key parameters/elements of the beamline Future developments • Voxel phantom import (from DICOM) • Calculation of LET distributions (and RBE?) in the perspective of future in-vitro/in-vivo experiments to be performed at ELI-Beamline • Implementation of Geant4-DNA models? spatio-temporal track correlations due to the extremely high dose rate per pulse G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it

  23. Thank you G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it

  24. Validation with reference code: magnetic fields& tracking 15 Comparison with COMSOL and SIMION software Magnetic field gradient within the 160 mm quad Magnetic field intensity along the radial axis of the dipole G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it

  25. Validation with reference code: magnetic fields& tracking 15 Comparison with COMSOL and SIMION software Magnetic field gradient within the 160 mm quad Magnetic field intensity along the radial axis of the dipole 60 MeV p track 60 MeV p track within PMQ system in the x-z plane within ESS system in the x-z plane G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it

  26. Adaptive source 16 Monoenerge'c G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it

  27. Adaptive source 16 Monoenerge'c Analytic G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it

  28. Adaptive source 16 Monoenerge'c Detailed laser-driven proton Analytic and ion beam source to use as input PIC 2D PIC 3D G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it

  29. Adaptive source 16 Monoenerge'c Detailed laser-driven proton Analytic and ion beam source to use as input PIC 2D PIC 3D G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it

  30. Adaptive source 16 Monoenerge'c Detailed laser-driven proton Analytic and ion beam source to use as input PIC 2D PIC 3D G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it

  31. Weighting low energy conventionally accelerated proton beams for modulators 17 G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it

  32. Weighting low energy conventionally accelerated proton beams for modulators 17 Spread Out Bragg Peak Tumor thickness G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it

  33. Weighting low energy conventionally accelerated proton beams for modulators 17 Spread Out Bragg Peak B. Jia, F. Romano, G.A.P. Cirrone, G. CuEone, M.H. Hadizadeh, A.A. Mowlavi, L. Raffaele. NIM A (Jan 2016) Tumor thickness G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it

  34. Weighting low energy conventionally accelerated proton beams for modulators 17 Spread Out Bragg Peak B. Jia, F. Romano, G.A.P. Cirrone, G. CuEone, M.H. Hadizadeh, A.A. Mowlavi, L. Raffaele. NIM A (Jan 2016) Tumor thickness G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it

  35. Weighting low energy conventionally accelerated proton beams for modulators 17 Spread Out Bragg Peak B. Jia, F. Romano, G.A.P. Cirrone, G. CuEone, M.H. Hadizadeh, A.A. Mowlavi, L. Raffaele. NIM A (Jan 2016) Tumor thickness G. Milluzzo- INFN-LNS (Italy) - gmilluzzo@lns.infn.it

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