Equipment for radiation surgery using narrow 185 MeV proton beams. Dosimetry and design.
The purpose of the present work was to optimize and standardize irradiation conditions and dosimetry methods in order to investigate the prerequisites for the routine use of narrow high energy proton beams for cerebral radiation surgery. Particular importance was laid on the design of the arrangements for defining and controlling the path of the beam in the laboratory in view of the desirability of working with well-defined parallel beams containing a minimal contribution of scattered and secondary radiation. At the same time it was intended that this apparatus should be used to adjust the beam reproducibly onto an ideal beam path prior to each irradiation session. It was also considered desirable to be able to supervise the centering and the structure of the beam during the irradiations in view of the variations which can arise due to varying running conditions in the synchrocyclotron. The beam was collimated and led to the place where the irradiations were to be performed, 25 metres from the synchrocyclotron, with a system of focusing quadrupole magnets and bending magnets. Final collimation of the beam penetrating the object was arranged with a system of accurately aligned cylindrical and plane-parallel metal apertures. The energy of the protons in the beam was 185 +/- 0.2 MeV and the maximum total fluence was 5 X 10(10) protons/s. A method of 11C activation dosimetry was developed with which an absolute determination of the fluence and the dose in the proton beam could be made with good accuracy. These determinations were performed by irradiating small polystyrene cylinders placed along the beam axis at the isocentre. The activity induced in the cylinders by the protons was measured in a well-type crystal detector. The efficiency of the detector for the detection of annihilation photons was determined before each measurement by means of calibration with standardized activities of 22Na and 60Co. The overall uncertainty in the dose determinations using 11C activation dosimetry was +/- 8 per cent. Monitoring of the dose during irradiation was performed with an ionization chamber. Since it was most important to minimize the scattering of the protons, this chamber was designed as a 'free air chamber' with the electrodes parallel to the beam. The chamber could not be used for absolute measurements, however, since there was a contribution to the ionization in the chamber from scattered protons and secondary radiation from the walls of the collimator defining the cross section of the ionization volume.(ABSTRACT TRUNCATED AT 400 WORDS)
D004735:Energy Transfer; D006801:Humans; D008433:Mathematics; D008961:Models, Structural; D010300:Parkinson Disease / Q000532:radiotherapy; D011879:Radiotherapy Dosage; D011882:Radiotherapy, High-Energy / Q000295:instrumentation* / Q000592:standards; D013679:Technology, Radiologic