Abstract

The CERN Large Hadron Collider (LHC) is designed to collide proton beams of unprecedented energy, in order to extend the frontiers of high-energy particle physics. During the first very successful running period in 2010--2013, the LHC was routinely storing protons at 3.5--4 TeV with a total beam energy of up to 146 MJ, and even higher stored energies are foreseen in the future. This puts extraordinary demands on the control of beam losses. An un-controlled loss of even a tiny fraction of the beam could cause a superconducting magnet to undergo a transition into a normal-conducting state, or in the worst case cause material damage. Hence a multi-stage collimation system has been installed in order to safely intercept high-amplitude beam protons before they are lost elsewhere. To guarantee adequate protection from the collimators, a detailed theoretical understanding is needed. This article presents results of numerical simulations of the distribution of beam losses around the LHC that have leaked out of the collimation system. The studies include tracking of protons through the fields of more than 5000 magnets in the 27 km LHC ring over hundreds of revolutions, and Monte-Carlo simulations of particle-matter interactions both in collimators and machine elements being hit by escaping particles. The simulation results agree typically within a factor 2 with measurements of beam loss distributions from the previous LHC run. Considering the complex simulation, which must account for a very large number of unknown imperfections, and in view of the total losses around the ring spanning over 7 orders of magnitude, we consider this an excellent agreement. Our results give confidence in the simulation tools, which are used also for the design of future accelerators.

Highlights

  • The Large Hadron Collider (LHC) [1,2] at CERN is designed to collide protons with an unprecedented energy of 7 TeV and a total stored energy of about 362 MJ per beam

  • We focus our comparisons on the betatron losses in IR7, since they are the limiting losses for the machine performance, and we do not study primary off-momentum losses in IR3 in this article

  • The importance of different types of imperfections varies between observables, e.g. the strongest effect on ηc is caused by aperture misalignments, while at the Tertiary collimators (TCTs), the tilt, center, and flatness errors dominate

Read more

Summary

INTRODUCTION

The Large Hadron Collider (LHC) [1,2] at CERN is designed to collide protons with an unprecedented energy of 7 TeV and a total stored energy of about 362 MJ per beam. In order to perform a quantitative comparison with measurements, and to predict critical quantities such as the power density in the superconducting magnets, the proton losses produced by SixTrack are used as a starting distribution for a second stage of simulations of the secondary showers, induced by the lost protons. This is done using the Monte Carlo code FLUKA [16,17,18,19]. VI, we present the FLUKA shower simulations of a few relevant regions and compare the results of the combined SixTrack and FLUKA calculation with BLM measurements

THE LHC AND ITS COLLIMATION SYSTEM
SixTrack
MEASUREMENTS OF LHC BEAM LOSS DISTRIBUTIONS
Perfect machine
Machine imperfections
QUANTITATIVE COMPARISONS WITH MEASUREMENTS USING FLUKA
Losses in the IR7 DS
TCT losses
Findings
CONCLUSIONS
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call