Flash proton therapy apparatus and method of use thereof
The invention comprises a method and apparatus for treating a tumor of a patient with positively charged particles, comprising the steps of: (1) transporting the positively charged particles sequentially from an accelerator, through a beam transport line, through a nozzle, and toward a position of the tumor; (2) treating the tumor with first particles, of the positively charged particles, where at least fifty percent of the first particles pass through a patient position, from the nozzle, to a post-patient position; and (3) detecting a beam position of the first particles in the post-patient position with a detector. The flash treatment preferably delivers the first particles at a rate exceeding one MHz.
1. A method for treating a tumor of a patient with positively charged particles, comprising the steps of:
transporting the positively charged particles sequentially from an accelerator, through a beam transport line, through a nozzle, and toward a position of the tumor;
treating the tumor with first particles, of the positively charged particles, wherein at least fifty percent of the first particles pass through a patient position, from said nozzle, to a post-patient position; and
detecting a beam position of the first particles in said post-patient position with a detector.
2. The method of claim 1 , said step of treating further comprising the step of:
delivering the first particles at a rate exceeding one MHz.
3. The method of claim 2 , said step of detecting further comprising the step of:
determining said beam position with an organic film charged particle detector.
4. The method of claim 2 , said step of treating further comprising the step of:
delivering second particles, of the positively charged particles, to said tumor, said second particles comprising a Bragg peak position in the tumor.
5. The method of claim 4 , further comprising the steps of:
said step of detecting further comprising the step of passing the passing the positively charged particles through a first time of flight detector element and at least into a second time of flight detector element;
receiving, into a beam state determination system, (1) a first signal related to an initial time of passage of the positively charged particles through said first time of flight detector and (2) a second signal related to an arrival time of the positively charged particles to said second time of flight detector element;
in a step of imaging the patient:
calculating a residual velocity of the positively charged particle after passing through the patient;
determining a velocity of the positively charged particle using a distance between the first time of flight detector element and the second time of flight detector element; and
determining an energy of the positively charged particle using the first signal, the arrival time, and a pathlength of the positively charged particles between the first time of flight detector and the second time of flight detector.
6. The method of claim 4 , said step of transporting further comprising the step of:
slowing the positively charged particles in an extraction step of moving said positively charged particles from said accelerator to said beam transport line.
7. The method of claim 1 , further comprising the step of:
verifying alignment of the first particles on a tumor position with said beam position.
8. The method of claim 1 , said step of detecting further comprising the steps of:
detecting a missed treatment voxel of the tumor; and
treating said missed treatment voxel in accordance to a prescribed treatment.
9. The method of claim 1 , further comprising the steps of:
accelerating the positively charged particles to a current relativistic energy using said accelerator;
said step of transporting passing the positively charged particles through the patient to yield a residual particle beam comprising a residual relativistic velocity;
determining the residual relativistic velocity using a first time of flight detector and a second time of flight detector separated by a separation distance; and
generating a positively charged particle computed tomography image with at least one of:
the residual relativistic velocity;
an increased mass of the positively charged particles determined using the residual relativistic velocity; and
an energy of the residual particle beam associated with the residual relativistic velocity,
wherein individual particles in the residual particle beam comprise a second mass of at least 1.02 times that of the individual particles prior to said step of accelerating.
10. The method of claim 1 , said step of detecting further comprising the steps of:
passing the positively charged particles into a multi-layer detector element;
detecting first secondary photons, resultant from passage of the positively charged particles, over a first wavelength range from a first layer of said multi-layer detector, said first layer comprising a first scintillation material; and
detecting second secondary photons, resultant from passage of the positively charged particles, over a second wavelength range from a second layer of said multi-layer detector element, the first wavelength range differing from the second wavelength range.
11. The method of claim 1 , further comprising the steps of:
using a double dipole scanning system, in said nozzle, to scan the positively charged particles along a first axis and a second axis, said double dipole scanning system comprising:
a beam path chamber comprising an entrance side and an exit side, the entrance side comprising a smaller area than the exit side,
a first dipole magnet, said first dipole magnet comprising a first coil and a third coil on first opposite sides of said beam path chamber; and
a second dipole magnet, said second dipole magnet comprising a second coil and a fourth coil on second opposite sides of said beam path chamber;
scanning the charged particles along the first axis with said first dipole magnet; and
scanning the charged particles along the second axis with said second dipole magnet.
12. The apparatus of claim 1 , said nozzle further comprising:
a dual axis scanning system; comprising:
a first pair of magnets;
a second pair of magnets; and
a beam path chamber comprising an entrance side and an exit side, said entrance side comprising a smaller area than the exit side,
wherein said first pair of magnets and said second pair of magnets circumferentially surround a common volume of a longitudinal axis of said beam path chamber.
13. An apparatus for treating a tumor of a patient with positively charged particles, comprising:
a cancer therapy system comprising a transport path of the positively charged particles sequentially passing from an accelerator, through a beam transport line, through a nozzle, and toward a position of the tumor; and
a detector positioned in a post-patient position relative to a treatment path from said nozzle passing through the patient position, said detector configured to detect a position of first particles, of the positively charged particles, in said post-patient position, wherein at least fifty percent of the first particles pass from said nozzle, through the patient position, to said detector, where said first particles flash treat the tumor.
14. The apparatus of claim 13 , said detector further comprising:
an organic film charged particle detector comprising germanium.
15. The apparatus of claim 13 , further comprising:
a winding about a core of a magnet about said beam transport line, said winding comprising:
a first width and a first thickness at a first cross-sectional position of said winding; and
a second width at least fifty percent larger than said first width and a second thickness less than half said first thickness at a second cross-sectional position of said winding.