Abstract: A pencil beam system includes a charged particle beam generator, a transport beamline apparatus, a scan nozzle, a fast deflector electromagnet, and a controller. After a therapeutic dose is delivered to a first target spot, the fast deflector electromagnet generates a first magnetic field that causes the net deflection of the charged particle beam to transition from the first target spot to an adjacent target spot. After the charged particle beam is directed to the adjacent target spot, the controller simultaneously adjusts the first magnetic field and the scan nozzle magnetic field to reduce and eliminate the contribution of the first magnetic field to the net deflection. The fast deflector electromagnet is deliberately designed with limited magnetic field and limited deflecting power to provide a higher slew rate, faster settling and less hysteresis contribution to beam position as compared to the scan nozzle electromagnets.

Abstract: The present disclosure is directed to systems and methods for real-time control of a charged particle pencil beam system during therapeutic treatment of a patient. In an aspect, the present disclosure is directed to measuring an actual shape, an actual intensity distribution, and an actual location at isocenter of the charged particle pencil beam. The actual data is compared to model treatment data in real time to determine if a statistically significant variance occurs in which case the charged particle pencil beam can be stopped mid-treatment for correction and/or analysis.

Abstract: An assembly for preventing an overdose of a charged particle beam during therapy to a patient includes a pixelated detector apparatus and a controller. The controller includes, for each pixel: a current integrator circuit that converts the local measured current into a total local detected charge integrated from a start time, the integrator circuit outputting an integrator voltage that corresponds to the total local detected charge; and a discriminator circuit that compares the integrator voltage with a reference voltage, the reference voltage corresponding to a maximum acceptable dose for the patient. A logic circuit generates an overdose fault signal if, at any of the pixels, the integrator voltage is higher than the reference voltage.

Abstract: A control system for fine tuning or spreading a charged particle pencil beam includes a low-inductance, low-power compensation or fine-tuning magnet assembly. The feedback loop that includes the compensation magnet assembly has a faster response rate than the feedback loop that includes the scan nozzle. The compensation or fine-tuning magnet assembly is preferably disposed upstream of the scan nozzle magnet(s) with respect to the beam path to make rapid but minor adjustments to the beam position between iterations of the scan nozzle.

Abstract: The present disclosure is directed to systems and methods for real-time control of a charged particle pencil beam system during therapeutic treatment of a patient. In an aspect, the present disclosure is directed to measuring an actual shape, an actual intensity distribution, and an actual location at isocenter of the charged particle pencil beam. The actual data is compared to model treatment data in real time to determine if a statistically significant variance occurs in which case the charged particle pencil beam can be stopped mid-treatment for correction and/or analysis.

Abstract: A control system for providing a closed loop, real time control of a charged particle pencil beam is disclosed. The system includes a first detector apparatus, a second detector apparatus, a first orthogonal magnetic deflector apparatus, a second orthogonal magnetic deflector apparatus, and a controller. The controller compares the measured position and beam angle of the beam with a model position and beam angle of a model beam to determine an offset error and a beam angle error. The first orthogonal magnetic deflector apparatus includes a pair of electromagnets to correct a first component of the offset and beam angle errors. The second orthogonal magnetic deflector apparatus includes a pair of electromagnets to correct a second component of the offset and beam angle errors. The beam can be iteratively adjusted during patient therapy or short pauses in patient therapy.

Abstract: An assembly for preventing an overdose of a charged particle beam during therapy to a patient includes a pixelated detector apparatus and a controller. The controller includes, for each pixel: a current integrator circuit that converts the local measured current into a total local detected charge integrated from a start time, the integrator circuit outputting an integrator voltage that corresponds to the total local detected charge; and a discriminator circuit that compares the integrator voltage with a reference voltage, the reference voltage corresponding to a maximum acceptable dose for the patient. A logic circuit generates an overdose fault signal if, at any of the pixels, the integrator voltage is higher than the reference voltage.

Abstract: The present disclosure is directed to systems and methods for real-time control of a charged particle pencil beam system during therapeutic treatment of a patient. In an aspect, the present disclosure is directed to measuring an actual shape, an actual intensity distribution, and an actual location at isocenter of the charged particle pencil beam. The actual data is compared to model treatment data in real time to determine if a statistically significant variance occurs in which case the charged particle pencil beam can be stopped mid-treatment for correction and/or analysis.

Abstract: A control system for fine tuning or spreading a charged particle pencil beam includes a low-inductance, low-power compensation or fine-tuning magnet assembly. The feedback loop that includes the compensation magnet assembly has a faster response rate than the feedback loop that includes the scan nozzle. The compensation or fine-tuning magnet assembly is preferably disposed upstream of the scan nozzle magnet(s) with respect to the beam path to make rapid but minor adjustments to the beam position between iterations of the scan nozzle.

Abstract: A control system for providing a closed loop, real time control of a charged particle pencil beam is disclosed. The system includes a first detector apparatus, a second detector apparatus, a first orthogonal magnetic deflector apparatus, a second orthogonal magnetic deflector apparatus, and a controller. The controller compares the measured position and beam angle of the beam with a model position and beam angle of a model beam to determine an offset error and a beam angle error. The first orthogonal magnetic deflector apparatus includes a pair of electromagnets to correct a first component of the offset and beam angle errors. The second orthogonal magnetic deflector apparatus includes a pair of electromagnets to correct a second component of the offset and beam angle errors. The beam can be iteratively adjusted during patient therapy or short pauses in patient therapy.

Abstract: The present disclosure is directed to systems and methods for real-time control of a charged particle pencil beam system during therapeutic treatment of a patient. In an aspect, the present disclosure is directed to measuring an actual shape, an actual intensity distribution, and an actual location at isocenter of the charged particle pencil beam. The actual data is compared to model treatment data in real time to determine if a statistically significant variance occurs in which case the charged particle pencil beam can be stopped mid-treatment for correction and/or analysis.

Abstract: The present disclosure is directed to systems and methods for real-time control of a charged particle pencil beam system during therapeutic treatment of a patient. In an aspect, the present disclosure is directed to measuring an actual shape, an actual intensity distribution, and an actual location at isocenter of the charged particle pencil beam. The actual data is compared to model treatment data in real time to determine if a statistically significant variance occurs in which case the charged particle pencil beam can be stopped mid-treatment for correction and/or analysis.

Abstract: A multi-resolution detector includes a high-resolution pixelated electrode and a low-resolution pixelated electrode. The high-resolution pixelated electrode includes a plurality of sub-arrays of first pixels. Each respective first pixel at each relative position in each sub-array is electrically connected in parallel with one another. The low-resolution pixelated electrode includes a plurality of second pixels. A control system receives as inputs an output from each pixelated detector. The control system uses the inputs to determine a physical position and a transverse intensity distribution of an incident charged particle pencil beam at the resolution of the high-resolution pixelated electrode.

Abstract: A multi-resolution detector includes a high-resolution pixelated electrode and a low-resolution pixelated electrode. The high-resolution pixelated electrode includes a plurality of sub-arrays of first pixels. Each respective first pixel at each relative position in each sub-array is electrically connected in parallel with one another. The low-resolution pixelated electrode includes a plurality of second pixels. A control system receives as inputs an output from each pixelated detector. The control system uses the inputs to determine a physical position and a transverse intensity distribution of an incident charged particle pencil beam at the resolution of the high-resolution pixelated electrode.

Abstract: A system for calibrating a charged particle pencil beam includes a first pixelated detector, a second pixelated detector, a beam stop, and a diagnostics system. The first and second pixelated detectors measure the pencil beam at positions proximal and/or distal to an isocenter plane. The beam stop is configured to detect an energy level of the pencil beam. The diagnostics system is configured to transmit a signal to request a generation of the charged particle pencil beam at different settings. The diagnostics system is also configured to update a calibration parameter for each setting based on the data received from the pixelated detectors and the beam stop.

Abstract: An ionization chamber with spatial distribution electrode for monitor hadron beam currents used for therapeutic treatment. Ionization chamber comprises humidity control, environmental sensing and real-time correction thereof. A flexible hermetic seal provide for ambient pressure equalization. X-Y electrode planes measure Gaussian distribution of incident particle beam. Methods described herein are suitable to fabricate highly accurate, low scattering electrodes with high spatial resolutions.

Abstract: A system for calibrating a charged particle pencil beam includes a first pixelated detector, a second pixelated detector, a beam stop, and a diagnostics system. The first and second pixelated detectors measure the pencil beam at positions proximal and/or distal to an isocenter plane. The beam stop is configured to detect an energy level of the pencil beam. The diagnostics system is configured to transmit a signal to request a generation of the charged particle pencil beam at different settings. The diagnostics system is also configured to update a calibration parameter for each setting based on the data received from the pixelated detectors and the beam stop.

Abstract: The present disclosure is directed to systems and methods for real-time control of a charged particle pencil beam system during therapeutic treatment of a patient. In an aspect, the present disclosure is directed to measuring an actual shape, an actual intensity distribution, and an actual location at isocenter of the charged particle pencil beam. The actual data is compared to model treatment data in real time to determine if a statistically significant variance occurs in which case the charged particle pencil beam can be stopped mid-treatment for correction and/or analysis.

Abstract: An ionization chamber with spatial distribution electrode for monitor hadron beam currents used for therapeutic treatment. Ionization chamber comprises humidity control, environmental sensing and real-time correction thereof. A flexible hermetic seal provide for ambient pressure equalization. X-Y electrode planes measure Gaussian distribution of incident particle beam. Methods described herein are suitable to fabricate highly accurate, low scattering electrodes with high spatial resolutions.

Abstract: A variety of systems, apparatus and methods for deflecting a particle beam are described. An apparatus comprises at least six electromagnetic portions disposed on a plane. Each of the at least six electromagnetic portions is aligned with a radius emanating from an axis normal to the plane and is distanced from the axis to form a volume about the axis. At least six coils are configured for affecting a dipole magnetic field in the volume in response to electrical currents applied to physically opposing coils where a particle beam entering the volume is deflected. Each of the at least six coils is disposed about a one of the at least six electromagnetic portions. A yoke structure is configured for returning a generated magnetic flux.