Orthogonal double dipole cancer therapy treatment beam scanning apparatus and method of use thereof

US11000696B2 · US · B2

Patent metadata
FieldValue
Publication numberUS-11000696-B2
Application numberUS-201916601592-A
CountryUS
Kind codeB2
Filing dateOct 15, 2019
Priority dateMay 27, 2016
Publication dateMay 11, 2021
Grant dateMay 11, 2021

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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

Official abstract text for this publication.

The invention comprises a method and apparatus for scanning charged particles in a cancer therapy system, comprising the steps of: (1) providing a first and second dipole magnet system and a gap, the gap comprising a common gap length, along a path of the charged particles, within both the first and second dipole magnet systems, the gap comprising a progressively increasing x/y-plane cross-section area from an entrance area of the charged particles into the double dipole magnet system to an exit area of the double dipole magnet system, the x/y-plane perpendicular to a z-axis from a center of the entrance area to a center of the exit area; (2) scanning the positively charged particles along a first axis of the x/y-plane using the first dipole magnet system; and (3) scanning the positively charged particles along a second axis of the x/y-plane using the second dipole magnet system.

First claim

Opening claim text (preview).

The invention claimed is: 1. A method for steering positively charged particles in a cancer therapy system, comprising the steps of: steering the positively charged particles along a first axis of an x/y-plane through a double dipole magnet system, comprising: (1) a first dipole magnet system; (2) a second dipole magnet system; and (3) a gap comprising a common gap length along a path of the positively charged particles both: (a) within said first dipole magnet system and (b) within said second dipole magnet system, said gap comprising progressively increasing x/y-plane cross-section areas, separated from each other by greater than one millimeter, from an entrance area into said double dipole magnet system to an exit area of said double dipole magnet system, the x/y-plane perpendicular to a z-axis from a center of the entrance area to a center of the exit area, said first dipole magnet system, comprising: a first magnet core of a first magnet half of said first dipole magnet system, said first magnet core comprising a first gap surface proximate a gap and a set of winding surfaces; and a first set of windings wound longitudinally around said first magnet core along said set of winding surfaces; and scanning the positively charged particles along a second axis of the x/y-plane through passage of a first current through said second dipole magnet system. 2. The method of claim 1 , further comprising the step of: carrying a second current from a power supply along a first set of windings wound longitudinally around a first magnet core along a set of winding surfaces, said first magnet core comprising a first magnet half of said first dipole magnet system, said set of winding surfaces comprising faces of a truncated rectangular pyramid. 3. The method of claim 2 , further comprising the step of: cooling said first dipole magnet, said step of cooling further comprising the step of: flowing a fluid through a first set of hollow core windings of said first set of windings, said first set of hollow core windings comprising: a first winding comprising m turns, said m turns comprising a first mean distance from said first magnet core; and a second winding comprising n turns, said n turns comprising a second mean distance from said first magnet core, the second distance greater than the first distance, wherein m>n. 4. The method of claim 2 , further comprising the step of: transporting the positively charged particles from a synchrotron through the gap, the gap length centered between: (1) first and second halves of said first dipole magnet system and (2) first and second sides of said second dipole magnet system. 5. The method of claim 2 , the gap comprising a truncated rectangular pyramid volume comprising a first rectangular entrance side, a second rectangular exit side, and four trapezoid shaped sides, said first rectangular entrance side at least ten percent smaller than said second rectangular exit side. 6. The method of claim 5 , further comprising the step of: treating a tumor location with the charged particles, the charged particles comprising at least one of: H + ; C 4+ ; and C 6+ .

Assignees

Inventors

Classifications

  • A61N5/1043Primary

    Scanning the radiation beam, e.g. spot scanning or raster scanning · CPC title

  • Rotating beam systems with a specific mechanical construction, e.g. gantries · CPC title

  • Cyclotrons · CPC title

  • for beam deflection · CPC title

  • Ions; Protons · CPC title

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What does patent US11000696B2 cover?
The invention comprises a method and apparatus for scanning charged particles in a cancer therapy system, comprising the steps of: (1) providing a first and second dipole magnet system and a gap, the gap comprising a common gap length, along a path of the charged particles, within both the first and second dipole magnet systems, the gap comprising a progressively increasing x/y-plane cross-sect…
Who is the assignee on this patent?
Elgart Faye Hendley, Ruebel Nick, Amato Mark R, and 2 more
What technology area does this patent fall under?
Primary CPC classification A61N5/1043. Mapped technology areas include Human Necessities.
When was this patent published?
Publication date Tue May 11 2021 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 2 related publications on this page (citations in our corpus or others sharing the same primary CPC).