Abstract

This paper presents the design of a compact gantry that uses superconducting bending magnets (BMs), for use in carbon-ion beam therapy. The size of the gantry is comparable to those of existing gantries that are used for proton-beam therapy. The designed gantry provides point-to-parallel scanning over an area of $20\text{ }\text{ }\mathrm{cm}\ifmmode\times\else\texttimes\fi{}20\text{ }\text{ }\mathrm{cm}$ at the isocenter, and has rotationally invariant optics, which are enabled by quadrupole and dipole magnets together with a 90\ifmmode^\circ\else\textdegree\fi{} combined-function magnet with 18.6-cm bore radius. A 90\ifmmode^\circ\else\textdegree\fi{} BM accommodates large scanning angles; it also provides equal focusing in horizontal and vertical planes, and zero-integrated nonlinear fields to minimize beam distortion at the isocenter. Three-dimensional field analysis of the magnet, and particle-tracking simulation, validate the beam optics of the gantry and point-to-parallel scanning. The Taylor map and the Lie map are shown to be useful in the analysis of magnetic fields and in optimizing the coil windings.

Highlights

  • Carbon-ion radiotherapy (CIRT) is a favorable method to kill deeply situated tumor cells by exploiting the physical properties and biological effects of a beam of carbon nuclei (C6þ ion beam) [1]

  • The second CIRT gantry uses superconducting technologies; it was installed at the National Institute of Radiological Sciences (NIRS) [4,5,6]

  • Using a 130-mm bore radius 5-T superconducting combined-function magnet as a final bending magnets (BMs) [8], we could reduce the size of a CIRT gantry to L 1⁄4 12 m × r 1⁄4 6 m [8,9], which is as compact as existing gantries for use in proton-beam therapy

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Summary

INTRODUCTION

Carbon-ion radiotherapy (CIRT) is a favorable method to kill deeply situated tumor cells by exploiting the physical properties and biological effects of a beam of carbon nuclei (C6þ ion beam) [1]. Using a 130-mm bore radius 5-T superconducting combined-function magnet as a final BM [8], we could reduce the size of a CIRT gantry to L 1⁄4 12 m × r 1⁄4 6 m [8,9], which is as compact as existing gantries for use in proton-beam therapy With parallel scanning, this gantry can cover a 15 cm × 15 cm scanning area at the isocenter. We present a compact CIRT gantry that covers 20 cm × 20 cm scanning area with parallel scanning and rotation-invariant beam sizes These abilities are realized by using a superconducting 5-T combined-function magnet that has a bore radius of 18.6 cm.

LINEAR OPTICS
Equal focusing for horizontal and vertical planes
Zero-integrated fields for both sextupole and octupole
FIELD ANALYSIS
PARTICLE TRACKING
Lie map
CONCLUSION
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