On the use of thin scrapers for momentum collimation

In transverse collimation systems, thin scrapers are used as primary collimators to interact with the beam halo and increase its impact parameter on the secondary collimators or absorbers. In the same way, placing the primary collimator in a dispersion region is used for momentum collimation. However, the use of scrapers for momentum collimation presents an additional disadvantage when handling medium-low energy beams. The energy lost by ionization is non negligible and the proton can be kicked out of the RF bucket. The material and thickness of the scraper have to be carefully adjusted according to the position of secondary collimators and momentum aperture of the machine. We derive simple analytical expressions for a generic case. The same calculations have been applied to the case of the SNS accumulator ring. After careful considerations, the use of scrapers for momentum collimation was ruled out in favor of a beam in gap kicker system.

1 INTRODUCTION

Momentum collimation is typically performed by placing the primary collimator in a dispersion region [1], [2]. On the other hand, thin scrapers are used as primary collimator in low and medium energy machines to enhance the divergence of the halo partcicles and drive them into the collimator without absorbing them.