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SU‐E‐T‐47: A Monte Carlo Model of a Spot Scanning Proton Beam Based On a Synchrotron Proton Therapy Accelerator

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Purpose:To build the model of a spot scanning proton beam for the dose calculation of a synchrotron proton therapy accelerator, which is capable of accelerating protons from 50 up to 221 MeV.Methods:The spot scanning beam nozzle is modeled using TOPAS code, a simulation tool based on Geant4.9.6. The model contained a beam pipe vacuum window, a beam profile monitor, a drift chamber, two plane‐parallel ionization chambers, and a spot‐position monitor consisted of a multiwire ionization chamber. A water phantom is located with its upstream surface at the isocenter plane. The initial proton beam energy and anglar deflection are modeled using a Gaussian distribution with FWHM (Full Widths at Half Maximum) deponding on its beam energy. The phase space file (PSF) on a virtual surface located at the center between the two magnets is recorded. PSF is used to analyze the pencil beam features and offset the pencil beam position. The source model parameters are verificated by fitting the simulated Result to the measurement.Results:The simulated percentage depth dose (PDD) and lateral profiles of scanning pencil beams of various incident proton energies are verificated to the measurement. Generally the distance to agreement (DTA) of Bragg peaks is less than 0.2cm. The FWHM of Gaussian anglar distribution was adjusted to fit the lateral profile difference between the simulation and the measurement to less than 2∼3cm.Conclusion:A Monte Carlo model of a spot scanning proton beam was bullt based on a synchrotron proton therapy accelerator. This scanning pencil beam model will be as a block to build the broad proton beam as a proton TPS dose verification tool.
Title: SU‐E‐T‐47: A Monte Carlo Model of a Spot Scanning Proton Beam Based On a Synchrotron Proton Therapy Accelerator
Description:
Purpose:To build the model of a spot scanning proton beam for the dose calculation of a synchrotron proton therapy accelerator, which is capable of accelerating protons from 50 up to 221 MeV.
Methods:The spot scanning beam nozzle is modeled using TOPAS code, a simulation tool based on Geant4.
9.
6.
The model contained a beam pipe vacuum window, a beam profile monitor, a drift chamber, two plane‐parallel ionization chambers, and a spot‐position monitor consisted of a multiwire ionization chamber.
A water phantom is located with its upstream surface at the isocenter plane.
The initial proton beam energy and anglar deflection are modeled using a Gaussian distribution with FWHM (Full Widths at Half Maximum) deponding on its beam energy.
The phase space file (PSF) on a virtual surface located at the center between the two magnets is recorded.
PSF is used to analyze the pencil beam features and offset the pencil beam position.
The source model parameters are verificated by fitting the simulated Result to the measurement.
Results:The simulated percentage depth dose (PDD) and lateral profiles of scanning pencil beams of various incident proton energies are verificated to the measurement.
Generally the distance to agreement (DTA) of Bragg peaks is less than 0.
2cm.
The FWHM of Gaussian anglar distribution was adjusted to fit the lateral profile difference between the simulation and the measurement to less than 2∼3cm.
Conclusion:A Monte Carlo model of a spot scanning proton beam was bullt based on a synchrotron proton therapy accelerator.
This scanning pencil beam model will be as a block to build the broad proton beam as a proton TPS dose verification tool.

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