Abstract

A large-scale proton or ${\mathrm{H}}^{\ensuremath{-}}$ accelerator often requires a jump in radio frequency, typically in the beam velocity range of $\ensuremath{\beta}=0.4--0.6$. The MYRRHA linac has two frequency jumps: one at $\ensuremath{\beta}\ensuremath{\cong}0.2$ and another one in the typical beam velocity range at $\ensuremath{\beta}=0.56$. Using the MYRRHA linac as an example, this study investigates two new solutions, whereby the frequency jump in the range of $\ensuremath{\beta}=0.4--0.6$ is eliminated. A single frequency jump at $\ensuremath{\beta}\ensuremath{\cong}0.2$ can shorten the whole linac considerably and reduce the construction and operation costs. The proposed frequency jump sections will use 704.4 MHz radio-frequency quadrupole and cross-bar $H$-type drift tube linear accelerators. To ensure a safe and reliable cw operation at such very high frequency for these kinds of accelerating structures, careful design studies with respect to beam dynamics and rf structures including water-cooling channels have been performed. The results demonstrated the feasibility of both solutions.

Highlights

  • In order to maintain high radio-frequency efficiency as well as to save construction costs, accelerating cells need to be kept reasonably short

  • A large-scale proton or H− accelerator often requires a jump in radio frequency, typically in the beam velocity range of β 1⁄4 0.4–0.6

  • Using the MYRRHA linac as an example, this study investigates two new solutions, whereby the frequency jump in the range of β 1⁄4 0.4–0.6 is eliminated

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Summary

INTRODUCTION

In order to maintain high radio-frequency (rf) efficiency as well as to save construction costs, accelerating cells need to be kept reasonably short. To accomplish the new frequency jump from 176.1 to 704.4 MHz, a section dedicated to the frequency jump will be placed directly at the end of each injector and will follow the same reliability strategy for the injector. It should have a compact layout, but the energy gain is not a design goal. For the MYRRHA linac, the upper limit for beam interruptions longer than 3 seconds is only 10 per three-month operating cycle [5]

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