Circular accelerator
US-2019239334-A1 · Aug 1, 2019 · US
US10624201B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-10624201-B2 |
| Application number | US-201716341077-A |
| Country | US |
| Kind code | B2 |
| Filing date | Feb 1, 2017 |
| Priority date | Feb 1, 2017 |
| Publication date | Apr 14, 2020 |
| Grant date | Apr 14, 2020 |
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Conventional cyclotrons have been incapable of changing energy of a beam to be extracted. Conventional synchrotrons have been difficult to output beams in a continuous manner. An accelerator has a dense region dense region in which orbits of different energies densely gather as a result of using a radiofrequency electric field to accelerate an ion orbiting in an isochronous magnetic field in order to cause a beam orbit to be displaced in a specific direction with increasing acceleration, and a sparse region in which orbits of different energies are sparsely discrete from each other. The accelerator has a feature that a magnetic field has a magnetic field gradient in a radial direction of a beam orbit in the dense region, and a product of a gradient of magnetic field gradient and a beam size passing through the dense region becomes smaller than the magnetic field gradient.
Opening claim text (preview).
The invention claimed is: 1. An accelerator, comprising: a dense region in which orbits of different energies densely gather as a result of using a radiofrequency electric field to accelerate an ion orbiting in an isochronous magnetic field in order to cause a beam orbit to be displaced in a specific direction with increasing acceleration; and a sparse region in which orbits of different energies are sparsely discrete from one another, wherein the magnetic field has a magnetic field gradient in a radial direction of a beam orbit in the dense region, and a product of a gradient of magnetic field gradient and a beam size passing through the dense region becomes smaller than the magnetic field gradient. 2. The accelerator according to claim 1 , wherein the magnetic field gradient in the radial direction in the dense region is approximately linear. 3. The accelerator according to claim 1 , wherein a sextupole magnetic field in the dense region is zero. 4. An accelerator, comprising: a pair of magnets that are placed facing each other to create a magnetic field between them; and a radiofrequency cavity in which ion beams are accelerated, wherein the magnets create a magnetic field such that a plurality of beam closed orbits of a ring shape on which the ion beams of different energies respectively orbit and the closed orbits densely gather on one side, the magnetic field created by the magnets has a magnetic field gradient in a radial direction of the closed orbits, and in the magnetic field created by the magnets, a product of a gradient of the magnetic field gradient and a size of the ion beam becomes smaller than the magnetic field gradient. 5. The accelerator according to claim 4 , wherein the magnetic field created by the magnets has the magnetic field gradient in the radial direction of a region in which the closed orbits densely gather, the magnetic field being approximately linear. 6. The accelerator according to claim 4 , further comprising: a trim coil for a dense region that is placed in a region in which the closed orbits densely gather.
Synchrocyclotrons, i.e. frequency modulated cyclotrons · CPC title
Methods or devices for acceleration of charged particles not otherwise provided for {, e.g. wakefield accelerators} · CPC title
Ions; Protons · CPC title
Electromagnets for high magnetic field strength (for superconducting electromagnets H01F6/00; for transformers or inductances without a magnetic core H01F30/08) · CPC title
Cyclotrons · CPC title
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