Abstract

In response to recommendations in the 2013 update of the European Strategy for Particle Physics, a conceptual design effort for an energy upgrade of the Large Hadron Collider (LHC) at CERN, the so-called high-energy LHC (HE-LHC), was launched as part of the Future Circular Collider study. The HE-LHC machine, which is meant to use 16 T magnet technologies in the existing LHC tunnel, would provide proton collisions at a center-of-mass energy of 27 TeV ($\ensuremath{\sim}2\ifmmode\times\else\texttimes\fi{}\mathrm{LHC}$) with a total stored energy of 1.34 GJ ($\ensuremath{\sim}4\ifmmode\times\else\texttimes\fi{}\mathrm{LHC}$) per beam. By adapting the LHC collimation system, a first layout of the HE-LHC's betatron cleaning insertion was conceived, with the requirement to sustain---for at least 10 seconds---the impact of about 1.86 MW, corresponding to a beam lifetime of 12 minutes, without inducing any magnet quench nor any damage to other accelerator components. In this article, we evaluate the power deposition on the collimation insertion for proton beam operation in the HE-LHC machine at top energy, by means of particle tracking and interaction calculations. The beam loss effects on the warm elements as well as on the superconducting dispersion suppressor magnets are assessed through a three-step simulation approach. In particular, for the proposed future high-energy LHC, we demonstrate the necessity of adding local collimators in the dispersion suppressor, and we uncover the harmful consequences of a potential removal of the beam line ``dogleg'' in the collimation insertion.

Highlights

  • With the aim of proposing designs for a post-Large Hadron Collider (LHC) particle accelerator, the Future Circular Collider (FCC) study developed and evaluated three accelerator options, which are documented in a four-volume FCC conceptual design report: a 100 km circumference hadron collider (FCC-hh) carrying a total energy of about 8500 MJ (∼20 times the LHC), a highest-luminosity high-energy lepton collider (FCC-ee), and an energy upgrade of the LHC based on FCC-hh technology to increase the center-of-mass energy by a factor of 2 (HE-LHC) [1,2,3,4]

  • The results presented in the following clearly demonstrate the need for the two local DS collimators (TCLD), which are integrated in the high-energy LHC (HE-LHC) baseline

  • We have evaluated the radiation impact on the accelerator elements in the betatron cleaning insertion of the proposed future high-energy LHC, considering a conservative regular beam loss scenario

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Summary

INTRODUCTION

With the aim of proposing designs for a post-LHC particle accelerator, the Future Circular Collider (FCC) study developed and evaluated three accelerator options, which are documented in a four-volume FCC conceptual design report: a 100 km circumference hadron collider (FCC-hh) carrying a total energy of about 8500 MJ (∼20 times the LHC), a highest-luminosity high-energy lepton collider (FCC-ee), and an energy upgrade of the LHC based on FCC-hh technology to increase the center-of-mass energy by a factor of 2 (HE-LHC) [1,2,3,4]. As a design criterion we specify that the HE-LHC collimation system is required to cope with a temporary drop of the beam lifetime (BLT) down to 12 minutes, corresponding to an instantaneous beam loss power of 1.86 MW. This loss power has to be sustained over ten seconds without any superconducting (SC) magnet quench. Studies for the LHC [9], HL-LHC [10,11], and FCC-hh [12] have shown that, in each of these machines, the dispersion suppressor (DS) downstream of IR7 is the ring location with the highest losses on SC magnets caused by leakage from the collimation system. Results are normalized to the design beam loss scenario and compared to those for the LHC

BETATRON CLEANING INSERTION OF THE HE-LHC MACHINE
SIMULATION WORKFLOW
Beam particle tracking around the ring
Particle shower calculation
ENERGY DEPOSITION
IR7 warm section
Collimators
Warm dipoles
IR7 cold section
ROLE OF THE DOGLEG
Findings
CONCLUSIONS
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