Energy degrader, charged particle beam emission system provided with same, and method of producing graphite film

US10420959B2 · US · B2

Patent metadata
FieldValue
Publication numberUS-10420959-B2
Application numberUS-201615779656-A
CountryUS
Kind codeB2
Filing dateNov 30, 2016
Priority dateNov 30, 2015
Publication dateSep 24, 2019
Grant dateSep 24, 2019

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  1. Title

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  2. Abstract

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  3. Assignees and inventors

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  4. Key dates

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  5. First independent claim

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Abstract

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Provided is an energy degrader including an attenuation member that becomes radioactive only to a lesser extent than conventional attenuation members. An attenuation member ( 11 ) is a graphite film, the graphite film has a thermal conductivity, in a surface direction, of 1200 W/(m·K) or greater, and the graphite film has a thickness of 0.1 μm or greater and 50 μm or less.

First claim

Opening claim text (preview).

The invention claimed is: 1. An energy degrader comprising one or more attenuation members configured to attenuate energy of a charged particle beam incident thereon, wherein at least one of the one or more attenuation members is a graphite film placed such that the charged particle beam is incident on a surface thereof, the graphite film has a thermal conductivity, in a surface direction, of 1200 W/(m·K) or greater, the graphite film has a thickness of 0.1 μm or greater and 50 μm or less, and the charged particle beam is a proton beam. 2. The energy degrader according to claim 1 , wherein the thermal conductivity in the surface direction of the graphite film is equal to or greater than 50 times a thermal conductivity in a thickness direction of the graphite film. 3. The energy degrader according to claim 1 , wherein an electric conductivity in the surface direction of the graphite film is 12000 S/cm or greater. 4. The energy degrader according to claim 1 , wherein an electric conductivity in the surface direction of the graphite film is equal to or greater than 100 times an electric conductivity in a thickness direction of the graphite film. 5. The energy degrader according to claim 1 , wherein the graphite film has a density of 1.40 g/cm 3 or greater and 2.26 g/cm 3 or less. 6. An energy degrader comprising an attenuation structure constituted by a plurality of attenuation members each configured to attenuate energy of a charged particle beam incident thereon, the attenuation structure having a multilayer structure composed of the plurality of attenuation members stacked together along a thickness direction, the plurality of attenuation members being constituted by graphite films each placed such that the charged particle beam is incident on a surface thereof; the graphite film has a thermal conductivity, in a surface direction, of 1200 W/(mK) or greater, the graphite film has a thickness of 0.1 μm or greater and 50 μm or less; and the charged particle beam is a proton beam. 7. The energy degrader according to claim 6 , wherein the multilayer structure varies in thickness along a surface direction. 8. The energy degrader according to claim 7 , wherein the multilayer structure has a stepped shape and progressively increases in thickness along the surface direction from one side of the attenuation structure to the other side of the attenuation structure, the one side and the other side being parallel to a surface on which the charged particle beam is incident. 9. A charged particle emission system comprising the energy degrader recited in claim 1 and configured to emit the charged particle beam, the charged particle emission system comprising: an accelerator configured to accelerate charged particles which are to enter the energy degrader; and an emission device configured to emit the charged particle beam whose energy has been attenuated by the energy degrader. 10. A charged particle emission system comprising the energy degrader recited in claim 6 and configured to emit the charged particle beam, the charged particle emission system comprising: an accelerator configured to accelerate charged particles which are to enter the energy degrader; and an emission device configured to emit the charged particle beam whose energy has been attenuated by the energy degrader. 11. The energy degrader according to claim 1 , wherein the energy of the charged particle beam ranges from 1 MeV to 3 GeV before attenuation. 12. A method of attenuating the energy of a proton beam, the method comprising: allowing the proton beam having an energy within the range of from 1 MeV to 3 GeV to incident on a surface of a graphite film, wherein the graphite film has a thermal conductivity, in a surface direction of 1200 W/(m K) or greater, and wherein the graphite film has a thickness of 0.1 μm or greater and 50 μm or less.

Assignees

Inventors

Classifications

  • X-ray therapy; Gamma-ray therapy; Particle-irradiation therapy (A61N5/01 takes precedence) · CPC title

  • Ions; Protons · CPC title

  • Density · CPC title

  • G21K5/04Primary

    with beam-forming means · CPC title

  • Preparation · CPC title

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Frequently asked questions

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What does patent US10420959B2 cover?
Provided is an energy degrader including an attenuation member that becomes radioactive only to a lesser extent than conventional attenuation members. An attenuation member ( 11 ) is a graphite film, the graphite film has a thermal conductivity, in a surface direction, of 1200 W/(m·K) or greater, and the graphite film has a thickness of 0.1 μm or greater and 50 μm or less.
Who is the assignee on this patent?
Kaneka Corp
What technology area does this patent fall under?
Primary CPC classification G21K5/04. Mapped technology areas include Physics.
When was this patent published?
Publication date Tue Sep 24 2019 00:00:00 GMT+0000 (Coordinated Universal Time) (B2). Legal status and post-grant events are not shown on this page.
What related patents are in patentsdb?
We list 12 related publications on this page (citations in our corpus or others sharing the same primary CPC).