Abstract

We have developed an interdigital H-mode (IH) drift-tube linac (DTL) design with an alternative phase focusing (APF) scheme for a muon linac, in order to measure the anomalous magnetic moment and electric dipole moment (EDM) of muons at the Japan Proton Accelerator Research Complex (J-PARC). The IH-DTL accelerates muons from $\ensuremath{\beta}=v/c=0.08$ to 0.28 at an operational frequency of 324 MHz. The output beam emittances are calculated as $0.315\ensuremath{\pi}$ and $0.195\ensuremath{\pi}\text{ }\text{ }\mathrm{mm}\text{ }\mathrm{mrad}$ in the horizontal and vertical directions, respectively, which satisfies the experimental requirement.

Highlights

  • The design of an interdigital H-mode (IH) drift-tube linac (DTL) for the acceleration of low-velocity protons was first proposed in 1956 [1], and this concept has been studied throughout the intervening decades [2,3]

  • We describe the design of the alternating phase focusing (APF) IH-DTL for the Japan Proton Accelerator Research Complex (J-PARC) experiment in detail

  • The transverse emittance growths were calculated to be approximately 0.02π mm mrad, and are considered to be due to the nonlinear focusing generated by the APF scheme

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Summary

INTRODUCTION

The design of an interdigital H-mode (IH) drift-tube linac (DTL) for the acceleration of low-velocity protons was first proposed in 1956 [1], and this concept has been studied throughout the intervening decades [2,3]. This paper describes the first attempt to adopt the APF IH-DTL for a low-emittance muon beam. We are developing a muon linac for the ðg − 2Þμ experiment at the Japan Proton Accelerator Research Complex (J-PARC) [13], in order to realize a low-emittance muon beam. One solution involves the use of an H-mode accelerating structure with permanent-magnet quadrupole (PMQ) magnets in the drift tubes [23] This setup provides sufficient transverse focusing, the production cost is increased. As a sufficient focusing force and a reduced production cost are desirable, APF is the dominant candidate; in this approach, the transverse and longitudinal focusing are achieved with the rf field only, and no additional focusing element is necessary.

APF IH-DTL DESIGN
Synchronous phase array optimization
IH cavity optimization
Particle tracking
RESULTS AND DISCUSSION
CONCLUSION
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