Abstract

The CERN accelerator complex is undergoing an upgrade in order to meet the requirements of the High-Luminosity Large Hadron Collider (HL-LHC). One of the key needs is to increase the intensity of beams injected into the LHC from the current $1.15\ifmmode\times\else\texttimes\fi{}{10}^{11}$ to $2.3\ifmmode\times\else\texttimes\fi{}{10}^{11}\text{ }\text{ }{\mathrm{p}}^{+}/\mathrm{bunch}$. This requires a beam intensity at injection in the Super Proton Synchrotron (SPS), the last injector before the LHC, as high as $2.6\ifmmode\times\else\texttimes\fi{}{10}^{11}\text{ }\text{ }{\mathrm{p}}^{+}/\mathrm{bunch}$, given that a budget for losses of about 10% is included in the design. However, previous experience with high intensity beams suggests that the total amount of losses in the SPS can be even higher, causing an increased activation, faster aging, and consequent early failure of machine equipment, in addition to an increase in the requirements for preinjectors in order to still meet the HL-LHC target in spite of higher losses. In this paper, we propose a collimation system to be used with HL-LHC proton beams in the SPS in order to intercept and safely dispose of beam losses in ad hoc locations and therefore provide the machine with protection against activation and equipment aging. The design is based on a two-stage concept, where the primary stage intercepts particles that otherwise would be lost, and the secondary stage employing an absorber where lost particles are finally disposed of. Numerical simulations prove a cleaning efficiency of the proposed system of at least 80%, substantially reducing the spreading of particle losses around the machine. Furthermore, the performance of the collimation system has a low sensitivity to common machine errors, and the design is cost efficient, with minimal hardware changes.

Highlights

  • The CERN Super Proton Synchrotron (SPS) [1] is the last accelerator in the injection chain of the Large Hadron Collider (LHC) [2]

  • The cleaning performance of the presented design of the SPS off-momentum collimation system is mostly evaluated by means of the global cleaning efficiency, which is the number of protons lost in the collimators (Ncoll) divided by the total losses, i.e., the number of protons lost in the aperture (N aper )

  • LHC beams in the SPS are affected by losses at injection, at the flat bottom and at the beginning of the ramp

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Summary

INTRODUCTION

The CERN Super Proton Synchrotron (SPS) [1] is the last accelerator in the injection chain of the Large Hadron Collider (LHC) [2]. We propose the design of an offmomentum collimation system to be used with HL-LHC proton beams in the SPS in order to intercept and safely dispose of beam losses in ad hoc locations. At this stage, the proposed design is not a part of the LIU project baseline and it might be implemented in the case of loss issues revealed by the SPS operation that starts in 2021

Proton beams
Heavy ion beams
Particle losses in the SPS
Constraints and requirements for the collimation system design
Simulation setup
BASELINE DESIGN OF THE COLLIMATION SYSTEM AND EXPECTED PERFORMANCE
System layout
The primary collimator
The secondary collimator
Operational settings
Cleaning performance
Standard operation
Hierarchy breakage
Orbit errors
Optics errors
Combined orbit and optics errors
Compatibility with other SPS beams
Effect on machine impedance
Findings
CONCLUSIONS
Full Text
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