Abstract

The Facility for Rare Isotope Beams driver linac was designed for acceleration of multiple-charge-state beams after the stripping at ion beam energies of 17 to $20\text{ }\text{ }\mathrm{MeV}\mathrm{/u}$ depending on the ion species. The linac includes a 180\ifmmode^\circ\else\textdegree\fi{} achromatic bend to select multiple charge states for further acceleration and to dump unwanted charge states after the first 45\ifmmode^\circ\else\textdegree\fi{} magnet. Two rf rebunchers between the stripper and the linac segment 2 (LS2) are required to minimize the effective emittance growth of the multiple-charge-state beams and provide matching to the LS2. Recent studies have shown that the best choice for these two rebunchers is a room-temperature (RT) accelerating structure capable of providing robust operation in the presence of the stripped heavy ion beam contaminants. The latter can result in uncontrolled losses of contaminant ions after the passage off the stripper. Therefore, using a superconducting (SC) rebuncher after the stripper is not rational due to possible contamination and performance degradation of SC cavities over a long period of operation. For the beam bunching in the energy range from 13 to $22\text{ }\text{ }\mathrm{MeV}\mathrm{/u}$, two 161 MHz rebunchers based on interdigital H-type (IH) structure were developed, built, installed and commissioned with beam at the FRIB linac. This is the first experimental demonstration for application of a cw RT drift tube accelerating structure in this energy range.

Highlights

  • The folding segment 1 (FS1) of the Facility for Rare Isotope Beams (FRIB) linac includes three rebunchers as shown in Fig. 1 [1]

  • The third rebuncher provides matching to the following accelerating section linac segment 2 (LS2)

  • The beam was tracked from the ion source through the radio-frequency quadrupole (RFQ) and linac segment 1 (LS1) to the stripper

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Summary

INTRODUCTION

The folding segment 1 (FS1) of the Facility for Rare Isotope Beams (FRIB) linac includes three rebunchers as shown in Fig. 1 [1]. The first rebuncher is required to create a time focus of the beam at the location of the stripper to minimize longitudinal emittance growth due to energy straggling. This rebuncher is located prior to the stripper and requires the highest voltage, which is provided by four quarter-wave superconducting (SC) cavities operating at 80.5 MHz. The second rebuncher is necessary to minimize the bunch momentum spread during the transport through the 180° bend. The third rebuncher provides matching to the following accelerating section linac segment 2 (LS2). These two rebunchers require lower voltage due to increased charge-to-mass ratio, q/A, after the stripper.

BEAM DYNAMICS REQUIREMENTS IN THE FS1
MULTIPHYSICS DESIGN OF THE ACCELERATING STRUCTURE
MECHANICAL DESIGN AND FABRICATION
RF AND BEAM TESTING
DISCUSSION
SUMMARY
Full Text
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