Abstract

The collimation system for the Spallation Neutron Source accumulator ring is designed for a capture efficiency close to 95% of the proton beam halo, dissipating about 2 kW of beam power. The collimation system consists of a two-stage collimation system (one scraper and two absorbers) cleaning the transverse halo and a beam-in-gap kicker system cleaning the gap residual and longitudinal halo. Preliminary studies indicate that a maximum level of uncontrolled loss of 0.01% of the total beam is achievable. On the other hand, the energy lost in the primary scraper may kick protons outside the rf bucket concentrating uncontrolled losses in areas of maximum dispersion. We use Monte Carlo simulations to clarify some beam dynamic issues that may compromise the high efficiency required. The material interacting with the beam and the shape of the scraper and absorbers have been carefully chosen to maximize the collimation efficiency and to minimize radioactivation. Furthermore, a realistic distribution of losses around the machine is used to identify potential hot areas. Finally, we determine the sensitivity of the collimation efficiency to misalignments and closed orbit errors. This paper describes the latest design of the collimation system and summarizes the results of these numerical studies.

Highlights

  • The Spallation Neutron Source (SNS) is designed to deliver a proton beam with 2 MW of beam power to a liquid mercury target

  • The best performance regarding loss control in high intensity machines is achieved at the proton storage ring (PSR) at Los Alamos where the fractional uncontrolled beam loss is about 1023 [3]

  • A collimation scheme including transverse and longitudinal cleaning has been designed for the SNS accumulator ring

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Summary

INTRODUCTION

The Spallation Neutron Source (SNS) is designed to deliver a proton beam with 2 MW of beam power to a liquid mercury target. The expected fractional beam loss, due mainly to the strong space charge in the presence of magnetic errors, is of the order of 1023 without collimation system. To achieve hands-on maintenance, we place collimators at strategic positions around the ring to remove particles outside the beam core and to localize the beam loss. These locations become the only “hot spots” of the machine where remote handling is required. We study the dependence of the cleaning efficiency on parameters such as the impact parameter, the machine tune, and the primary aperture

Acceptance
Lattice
CHOICE OF THE HARDWARE
Primary scraper
Secondary absorbers
Collimator aperture
Beam in gap cleaner
Beam halo simulation
Efficiency
RELIABILITY OF THE COLLIMATION SYSTEM
Closed orbit and misalignments
Tunability
Halo drift velocity
Primary aperture
LOSS DISTRIBUTION
Findings
CONCLUSIONS
Full Text
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