Radiation Pressure Acceleration (RPA) and Target Normal Sheath Acceleration (TNSA) are the two most significant methods for designing Laser-Accelerated Proton Beam (LAP) systems. LAP technology has inspired innovative applications that leverage the unique properties of proton bunches, distinguishing them from conventionally accelerated proton beams. In previous simulations, we presented a fundamental model of the proton beamline based on two pulsed-power solenoids, utilizing Monte Carlo simulations with the GEANT4 toolkit. We conducted adjustments to the magnetic field of the first solenoid and precisely calculated the flux of primary protons and secondary radiations in the beamline. This article introduces the second solenoid, providing detailed specifications and incorporating it into the previous simulations, optimizing its magnetic field. Additionally, the absorbed dose from RPA protons in a water phantom has been calculated. The simulation results demonstrated that incorporating and optimizing the second solenoid within the beamline significantly enhanced proton beam energy selection and shaping. This optimization effectively filtered out lower-energy protons, reduced the effective energy spread, and consequently shifted the maximum dose deposition to a greater depth within the water phantom. Furthermore, as the incident energy dispersion decreased, the dose profile became more concentrated, and the width of the high-dose region was reduced. Analysis of secondary neutron and photon doses also revealed that controlling the incident proton energy spectrum has a pronounced effect on reducing secondary photon doses. The calculations presented in this paper constitute a preliminary step toward completing the full RPA beamline simulation model.
扫码关注我们
求助内容:
应助结果提醒方式:
