Particle accelerator that produces charged particles having variable energies
US-9730308-B2 · Aug 8, 2017 · US
US10028369B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-10028369-B2 |
| Application number | US-201715552719-A |
| Country | US |
| Kind code | B2 |
| Filing date | Mar 13, 2017 |
| Priority date | Mar 17, 2016 |
| Publication date | Jul 17, 2018 |
| Grant date | Jul 17, 2018 |
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Ions are released over time from an ion source into a beam area proximate a central axis. A radiofrequency (RF) system with a variable frequency and variable voltage accelerates the ions in orbiting trajectories expanding outward from the central axis. The ions are accelerated to different extraction energy levels within a given design range at a shared extraction radius from the central axis. An RF-frequency versus ion-time-of-flight scenario is set such that the frequency versus time scenario is the same for any ion extraction energy from the given design range, and a constant-or-variable-RF-voltage versus ion-time-of-flight scenario is adjusted to provide ion acceleration from injection to extraction for ions with different respective extraction energy levels within the given design range; and the ions are extracted at the different energy levels at the shared extraction radius.
Opening claim text (preview).
What is claimed is: 1. A method for particle acceleration in a variable-energy synchrocyclotron utilizing a single-tuned variable frequency RF drive, the method comprising: releasing ions over time from an ion source into a beam area proximate a central axis; using a radiofrequency (RF) system with a variable frequency and variable voltage to accelerate the ions in orbiting trajectories expanding outward from the central axis; accelerating the ions using the synchrocyclotron to different extraction energy levels within a given design range at a shared extraction radius from the central axis; setting an RF-frequency versus ion-time-of-flight scenario such that the scenario is the same for any ion extraction energy from the given design range of extraction energy levels; adjusting a constant-or-variable-RF-voltage versus ion-time-of-flight scenario to provide ion acceleration from injection to extraction at the shared extraction radius for ions with different respective extraction energy levels within the given design range; and extracting the ions at the different energy levels at the shared extraction radius using the synchrocyclotron. 2. The method of claim 1 , further comprising: passing electrical current through first and second superconducting primary coils, wherein each superconducting primary coil is centered symmetrically about a central axis, one on each side of a midplane intersected perpendicularly by the central axis, wherein the electrical current is passed through the first superconducting primary coil in the same direction as the direction in which electrical current is passed through the second superconducting primary coil; passing electrical current through at least a first and a second magnetic-field-shielding coil, wherein the first magnetic-field-shielding coil is on the same side of the mid plane as the first superconducting primary coil and beyond the outer radius of the first superconducting primary coil, wherein the second magnetic-field-shielding coil is on the same side of the midplane as the second superconducting primary coil and beyond the outer radius of the second superconducting primary coil, wherein electrical current is passed through the first and second magnetic-field-shielding coils in a direction opposite to the direction in which electrical current is passed through the superconducting primary coils, and wherein passing electrical current through the magnetic-field-shielding coils generates a canceling magnetic field that reduces the magnetic field generated at radii from the central axis beyond the magnetic-field-shielding coils; and shaping the magnetic field in the midplane using at least a first and a second superconducting magnetic-field-shaping coil, wherein the first and second superconducting magnetic-field-shaping coils are positioned at shorter radii from the central axis than are the superconducting primary coils. 3. The method of claim 1 , wherein the variable-frequency voltage is generated by intermittently applying a voltage to a radiofrequency drive selected from a rotating capacitor, digital RF amplifiers, a solid state resonator, and a fast ferrite tuner, wherein the radiofrequency drive exhibits a radiofrequency cycle to trigger generation of a voltage at a particular radiofrequency band in a radiofrequency cycle of the radiofrequency drive. 4. The method of claim 3 , wherein the radiofrequency drive is a rotating capacitor. 5. The method of claim 1 , wherein ions are extracted with energy levels that differ by over 100 MeV from one another. 6. A variable-energy synchrocyclotron utilizing a single-tuned variable frequency RF drive, comprising: first and second superconducting primary coils, wherein each superconducting primary coil is centered about a central axis, one on each side of a midplane intersected perpendicularly by the central axis; a current source electrically coupled with the first and second superconducting primary coils and configured to direct electrical current through the first and second superconducting primary coils in the same direction; at least a first and a second magnetic-field-shielding coil centered about the central axis and at radii from the central axis beyond the superconducting primary coils, wherein the first magnetic-field-shielding coil is positioned on the same side of the midplane as the first superconducting primary coil, wherein the second magnetic-field-shielding coil is positioned on the same side of the midplane as the second superconducting primary coil, wherein the current source is electrically coupled with the first and second magnetic-field-shielding coils and configured to direct electrical current through the first and second magnetic-field-shielding coils in a direction that is opposite to the direction in which the electrical current is passing through the superconducting primary coils; an ion source positioned to release an ion in the midplane for an outwardly orbiting acceleration; at least a first and a second superconducting magnetic-field-shaping coil, wherein the first and second superconducting magnetic-field-shaping coils are positioned at shorter radii from the central axis than are the superconducting primary coils; and a radiofrequency system including electrodes positioned on opposite sides of the midplane, a radiofrequency drive, and a voltage source configured to supply an electrical voltage to the radiofrequency drive and then to the electrodes, wherein the radiofrequency drive is configured to establish a radiofrequency upon a voltage delivered from the voltage source to the electrodes. 7. The variable-energy synchrocyclotron of claim 6 , wherein the radiofrequency drive is selected from a rotating capacitor, digital RF amplifiers, a solid state resonator, and a fast ferrite tuner, and wherein the radiofrequency drive is configured to exhibit a radiofrequency cycle to trigger generation of a voltage at a particular radiofrequency band in a radiofrequency cycle of the radiofrequency drive. 8. The variable-energy synchrocyclotron of claim 7 , wherein the radiofrequency drive is a rotating capacitor.
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