Abstract

Many future projects plan using high-current, high-energy, multipass energy-recovery linacs that are based on superconducting rf (SRF) cavities. The necessity of ensuring the transverse stability of the beam in such accelerators imposes strict limits on the high order modes (HOMs) impedances, and demands effective HOM damping. The latter requirement often precludes achieving a high real-estate accelerating gradient in such structures. The modular structure of long SRF linacs also requires incorporating vacuum flanges; however, these flanges have surface contacts and cannot tolerate strong rf fields. Locating them in the low-field areas of the linac structure may involve considerably elongating the intermodular interfaces, a change that would reduce the linac’s real-estate accelerating gradient. In this paper, I propose a novel method to resolve this issue, using compact interconnects between the SRF cavities wherein to locate effective HOM dampers and vacuum flanges.

Highlights

  • This means that superconducting rf (SRF) cavities should not have trapped dipole high order modes (HOMs), and possibly no quadrupole ones

  • One of the foremost reasons for using SRF linacs lies in their low losses that are related directly to the very high Q of the fundamental mode (FM)

  • I discuss the attractive option of a unit-length tube, wherein the HOM absorbers and the vacuum flange are located near its center

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Summary

INTRODUCTION

Several proposals for electron-hadron colliders and light sources [1,2,3,4,5,6,7,8,9,10,11,12,13,14,15] and advanced electron coolers [16,17,18,19] are based on superconducting energy-recovery linacs (SRF ERLs) operating with very high average currents. Using six HOM waveguides per cavity, as they suggested, significantly complicates the design, and requires having six additional large transitions from 2 K to room temperature. The applicability of the proposed method to interconnects with a different geometry is discussed later

EVANESCENT WAVE IN THE INTERCONNECTING TUBE
THE BNL FIVE-CELL SRF CAVITY
EFFECTIVE MULTICELL HOM-DAMPED SRF LINACS
SENSITIVITY OF ERRORS
PULSED MODE OF OPERATION AND TRANSIENTS
VIII. DISCUSSION
Findings
CONCLUSIONS

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