Abstract
Abstract
In high-intensity proton synchrotrons, controlling beam loss during machine operation is
crucial to prevent radiation damage. Uncontrolled beam loss poses a significant challenge in
achieving higher beam intensity and power in these synchrotrons. The beam collimation system plays
a vital role in removing halo particles and localizing beam loss, serving as a critical tool for
controlling uncontrolled beam loss in high-intensity proton accelerators. To address the issue of
uncontrolled beam loss, a two-stage transverse collimation system was designed at the rapid
cycling synchrotron (RCS) of China Spallation Neutron Source (CSNS). However, during the beam
commissioning, it was found that the collimation efficiency was compromised due to the small ratio
of the physical acceptance to the collimator acceptance and insufficient phase advances between
the primary and secondary collimators. To address this issue, the designed two-stage collimator
was modified to a one-stage collimator. Through optimization of the collimation system, the beam
loss was effectively localized within the collimator area. As a result, CSNS achieved the design
power of 100 kW with minimal uncontrolled beam loss.
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