Abstract

Fully stripped carbon ions generated in a laser-ablation ion source are directly injected into a small-scale induction synchrotron. Carbon-ion beams of ${\mathrm{C}}^{6+}$, ${\mathrm{C}}^{5+}$, and ${\mathrm{C}}^{4+}$ are trapped in the barrier bucket. Beam properties, such as the momentum spread and beam lifetime in the low-energy ring, are measured and discussed in relation to the essential characteristics required in a carbon driver for future carbon therapies.

Highlights

  • Energy sweep extraction in a single acceleration cycle from a fast-cycling synchrotron has been proposed [1], where a fast-cycling induction synchrotron requiring no large-scale injector is used as a driver and a beam is continuously extracted by a new beam-handling method to allow continuous beam-spill loss from the barrier bucket

  • A fully stripped carbon-ion beam produced by the laser-ablation ion source (LAIS) was directly injected into the fast-cycling induction synchrotron called the KEK Digital Accelerator (DA) and captured by the barrier bucket for its lifetime, which is determined by electron capture caused by the interaction with residual atoms and molecules

  • The laser irradiation chamber is embedded in the high-voltage platform (HVP) of the core body of the LAIS, which accommodated the electron cyclotron resonance ion source (ECRIS) until 2015

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Summary

INTRODUCTION

Energy sweep extraction in a single acceleration cycle from a fast-cycling synchrotron has been proposed [1], where a fast-cycling induction synchrotron requiring no large-scale injector is used as a driver and a beam is continuously extracted by a new beam-handling method to allow continuous beam-spill loss from the barrier bucket. Okamura and colleagues produced a C6þ beam of several tens of milliamps in their LAIS driven by a medium-energy CO2 laser (4 J) [7] and attempted immediate acceleration of a carbon-ion beam by an RFQ without charge separation. Based on these studies, research has begun on practical application of these carbon-ion beams in particle cancer therapy at various institutes, including in the private sector [8]. Some beam properties of the injected C4þ, C5þ, and C6þ beams are determined

Outline
LAIS and carbon ions
KEK-DA
Free run
BEAM LIFETIME
SUMMARY AND FUTURE PROSPECTS

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