Disclosed are systems and methods for characterizing interactions or proton beams in tissues. In certain embodiments, charged particles emitted during passage of protons, such as those used for therapeutic and/or imaging purposes, can be detected at relatively large angles. In situations where beam
Disclosed are systems and methods for characterizing interactions or proton beams in tissues. In certain embodiments, charged particles emitted during passage of protons, such as those used for therapeutic and/or imaging purposes, can be detected at relatively large angles. In situations where beam intensity is relatively low, such as in certain imaging applications, characterization of the proton beam with charged particles can provide sufficient statistics for meaningful results while avoiding the beam itself. In situations where beam intensity is relatively high, such as in certain therapeutic applications, characterization of the proton beam with scattered primary protons and secondary protons can provide information such as differences in densities encountered by the beam as it traverses the tissue and dose deposited along the beam path. In certain situations, such beam characterizations can facilitate more accurate planning and monitoring of proton-based therapy.
대표청구항▼
1. A method for monitoring proton therapy, the method comprising: positioning a patient along a beam path;delivering a plurality of protons along the beam path to the patient;detecting interactions of at least some of the plurality of protons delivered to the patient, the detected interactions compr
1. A method for monitoring proton therapy, the method comprising: positioning a patient along a beam path;delivering a plurality of protons along the beam path to the patient;detecting interactions of at least some of the plurality of protons delivered to the patient, the detected interactions comprising scattering locations of protons from within the patient, the detected interactions providing information about numbers of scattering protons at the scattering locations, wherein detecting interactions comprises detecting the protons scattered at an angle relative to the beam path, the scattering angle relative to the beam path being within a range of approximately 20 degrees to 90 degrees; andestimating a dose deposited for the plurality of protons based on the numbers of scattering protons at the scattering locations. 2. The method of claim 1, wherein the angle is within a range of approximately 25 degrees to 70 degrees. 3. The method of claim 2, wherein the angle is within a range of approximately 30 degrees to 60 degrees. 4. The method of claim 3, wherein the angle is approximately 45 degrees. 5. The method of claim 1, wherein a beam comprising the plurality of protons has an average kinetic energy in a range of approximately 45 MeV to 300 MeV. 6. The method of claim 5, wherein a beam comprising the plurality of protons has an average kinetic energy in a range of approximately 80 MeV to 270 MeV. 7. The method of claim 6, wherein a beam comprising the plurality of protons is configured for cancer therapy based on a Bragg peak effect. 8. The method of claim 7, wherein a beam comprising the plurality of protons has an average kinetic energy of approximately 100 MeV. 9. The method of claim 6, wherein a beam comprising the plurality of protons is configured for radiosurgery application based on ionization by the protons. 10. The method of claim 9, wherein a beam comprising the plurality of protons has an average kinetic energy of approximately 250 MeV. 11. The method of claim 1, wherein the detecting of the interactions comprises characterizing tracks associated with the interactions with one or more silicon strip detectors and a proton calorimeter. 12. The method of claim 1, wherein the detecting of the interactions comprises characterizing tracks associated with the interactions on a plurality of sides about the beam path. 13. The method of claim 12, wherein the tracks associated with the interactions are characterized at two opposing sides substantially symmetrical about the beam path. 14. The method of claim 1, further comprising: adjusting the scattering angle relative to the beam path at which the protons are detected; anddetecting interactions of at least some of the protons delivered to the patient at the adjusted scattering angle. 15. The method of claim 1, further comprising positioning a detector assembly to detect protons scattered at the scattering angle. 16. The method of claim 1, further comprising detecting scattering locations of protons from within the patient at a second scattering angle relative to the beam path, the second scattering angle different from the scattering angle. 17. The method of claim 16, further comprising positioning a second detector assembly to detect protons scattered at the second scattering angle. 18. The method of claim 12, wherein characterizing tracks associated with the interactions comprises generating interaction profiles.
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Zwart, Gerrit Townsend; Jones, Mark R.; Cooley, James, Collimator and energy degrader.
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