Particle Beam Therapy Device Secondary Beam Shielding
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Solution Overview
Problem
In particle beam therapy devices, the generation of beams with different nuclides from the primary cation beam can result in unnecessary irradiation of patients, leading to potential damage to non-target areas due to varying mass numbers and charge states, as these secondary beams penetrate deeper into the body.
Innovation Solution
A particle beam therapy device that includes a cyclotron to produce a cation beam, a degrader to reduce the beam's energy and generate secondary beams, a bending electromagnet to deflect the mixed beam based on momentum per unit charge, and a passage selection unit to selectively pass through the cation beam while shielding the secondary beams, ensuring only the cation beam reaches the treatment area.
Engineering Contradictions & Design Principles
Engineering Contradiction Analysis
1Use of energy by moving object
If a degrader is used to reduce the energy of the cation beam, then the beam energy can be adjusted for treatment, but other species of beams with different nuclides are generated from the cation beam
Solution Approach 1:
The passage selection unit extracts and removes the harmful secondary beams from the mixed beam while allowing the primary cation beam to pass through to the treatment area, effectively separating the useful beam from the harmful byproducts generated by the degrader
Solution Approach 2:
The passage selection unit acts as an intermediary component between the degrader and the treatment area, selectively filtering which beams are allowed to proceed based on their trajectory and momentum characteristics
2Ease of operation
If the mixed beam is deflected by a bending electromagnet, then the trajectory can be adjusted, but the beam path becomes more complex
Solution Approach 1:
The bending electromagnet changes the trajectory parameter of the mixed beam by applying a magnetic field that deflects beams based on their momentum per unit charge, enabling selective routing of different beam species through the passage selection unit
3Quantity of substance
If secondary beams are allowed to reach the patient, then the treatment area receives beam irradiation, but non-target areas are damaged due to deeper penetration
Solution Approach 1:
The passage selection unit extracts and blocks the harmful secondary beams before they can reach the patient, while allowing the primary cation beam to pass through to the treatment area, preventing non-target area damage
Solution Approach 2:
The system converts the harmful effect of secondary beam generation into a useful separation mechanism by using the momentum differences caused by the bending electromagnet to enable selective filtering of beam species
Applied Scientific Principles
This section explains which scientific principles are used to turn an abstract innovation direction into a practical engineering solution.
Function Achieved in This Case
This configuration effectively reduces the transmission of secondary beams to the patient, minimizing unnecessary irradiation and associated damage, while allowing the primary cation beam to be precisely targeted, thus enhancing treatment accuracy and reducing radio-activation risks.
Implementation Method 1
a cyclotron that exits the cation beam
Implementation Method 2
a degrader that is provided on a downstream side of the cyclotron, reduces energy of the cation beam
Implementation Method 3
a bending electromagnet that is provided on a downstream side of the degrader, deflects a mixed beam in which the cation beam and the other species of the beam are mixed, and causes a trajectory of a beam included in the mixed beam to be different depending on momentum per unit charge
Data Source
AI summary
A particle beam therapy device that irradiates a patient with a cation beam to perform treatment, the device including a passage selection unit that selectively passes through the cation beam among a mixed beam in which the cation beam and other species of a beam having a nuclide different from that of the cation beam are mixed after passing through a deflection magnetic field, after causing the mixed beam to pass through the deflection magnetic field, in a case where the other species of the beam is generated from the cation beam.


