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IEEE Transactions on Nuclear Science | 2011

FLUKA Simulations for SEE Studies of Critical LHC Underground Areas

K. Røed; V. Boccone; Markus Brugger; A. Ferrari; D. Kramer; Elias Lebbos; Roberto Losito; Alessio Mereghetti; Giovanni Spiezia; Roberto Versaci

FLUKA Monte Carlo simulations have been performed to identify particle energy spectra and fluences relevant for evaluating the risk of single event effects in electronics installed in critical LHC underground areas. Since these simulations are associated with significant uncertainties, the results will compared with an online monitoring system installed to evaluate radiation levels at the location of the electronics. This comparison approach have been benchmarked in a mixed field reference facility and for a preliminary LHC monitoring case study.


Physical Review Special Topics-accelerators and Beams | 2014

Simulations and measurements of beam loss patterns at the CERN Large Hadron Collider

Roderik Bruce; G. Robert-Demolaize; R. Assmann; V. Boccone; Chiara Bracco; M. Brugger; Marija Cauchi; F. Cerutti; D Deboy; A. Ferrari; L Lari; Aurelien Marsili; Alessio Mereghetti; Daniele Mirarchi; Elena Quaranta; Stefano Redaelli; A Rossi; Belen Salvachua; Eleftherios Skordis; Claudia Tambasco; Gianluca Valentino; T Weiler; V. Vlachoudis; D Wollmann

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.


Archive | 2018

Special Collimation System Configuration for the LHC High-Beta Runs

Hector Garcia Morales; Stefano Redaelli; Roderik Bruce; Helmut Burkhardt; Alessio Mereghetti; Mario Deile; S. Jakobsen

H. Garcia-Morales∗, Royal Holloway University of London, UK, CERN, Geneva, Switzerland R. Bruce, H. Burkhardt, M. Deile, S. Jakobsen, A. Mereghetti, S. Redaelli, CERN, Geneva, Switzerland Abstract Special LHC high-β∗ optics is required for the forward physics program of TOTEM and ATLAS-ALFA. In this configuration, the beam is de-squeezed (the β-function at the collision point is increased) in order to minimize the divergence for measurements at very small scattering angles. In these low beam intensity runs, it is important to place the Roman Pots (RPs) as close as possible to the beam, which demands special collimator settings. During Run I, a significant amount of background was observed in the forward detectors due to particles outscattered from the primary collimator. During Run II, a different collimation configuration was used where a tungsten collimator was used as primary collimator instead of the usual one made of carbon. Using this configuration, a significant reduction of the background at the RPs was observed. In this paper we present a description of the new collimator configuration and the results obtained during the high-β∗ run carried out in 2016.


Archive | 2017

Study of the 2015 Top Energy LHC Collimation Quench Tests Through an Advanced Simulation Chain

Eleftherios Skordis; Francesco Cerutti; Vasilis Vlachoudis; Roderik Bruce; Stefano Redaelli; Alessio Mereghetti; Pascal Dominik Hermes; Alfredo Ferrari; Belen Salvachua; Carsten Welsch; Anton Lechner

While the LHC has shown record-breaking performance during the 2016 run, our understanding of the behaviour of the machine must also reach new levels. The collimation system and especially the betatron cleaning insertion region (IR7), where most of the beam halo is intercepted to protect superconducting (SC) magnets from quenching, has so far met the expectations but could nonetheless pose a bottleneck for future operation at higher beam intensities for HL-LHC. A better understanding of the collimation leakage to SC magnets is required in order to quantify potential limitations in terms of cleaning efficiency, ultimately optimising the collider capabilities. Particle tracking simulations combined with shower simulations represent a powerful tool for quantifying the power deposition in magnets next to the cleaning insertion. In this study, we benchmark the simulation models against beam loss monitor measurements from magnet quench tests (QT) with 6.5 TeV proton and 6.37Z TeV Pb ion beams. In addition, we investigate the effect of possible imperfections on the collimation leakage and the power deposition in magnets.


7th Int. Particle Accelerator Conf. (IPAC'16), Busan, Korea, May 8-13, 2016 | 2016

Simulation of Heavy-Ion Beam Losses with the SixTrack-FLUKA Active Coupling

Pascal Dominik Hermes; Roderik Bruce; F. Cerutti; A. Ferrari; John M. Jowett; Anton Lechner; Alessio Mereghetti; Daniele Mirarchi; Pablo G. Ortega; Stefano Redaelli; Belen Salvachua; Eleftherios Skordis; Gianluca Valentino; Vasilis Vlachoudis

The LHC heavy-ion program aims to further increase the stored ion beam energy, putting high demands on the LHC collimation system. Accurate simulations of the ion collimation efficiency are crucial to validate the feasibility of new proposed configurations and beam parameters. In this paper we present a generalized framework of the SixTrackFLUKA coupling to simulate the fragmentation of heavyions in the collimators and their motion in the LHC lattice. We compare heavy-ion loss maps simulated on the basis of this framework with the loss distributions measured during heavy-ion operation in 2011 and 2015.


7th Int. Particle Accelerator Conf. (IPAC'16), Busan, Korea, May 8-13, 2016 | 2016

Validation of Off-momentum Cleaning Performance of the LHC Collimation System

Belen Salvachua; P. Baudrenghien; Roderik Bruce; Hector Garcia; Pascal Dominik Hermes; Stephen Jackson; Michael Jaussi; Regina Kwee-Hinzmann; Alessio Mereghetti; Daniele Mirarchi; Stefano Redaelli; Helga Timko; Gianluca Valentino; Alessandra Valloni

The LHC collimation system is designed to provide effective cleaning against losses coming from off-momentum particles, either due to un-captured beam or to an unexpected RF frequency change. For this reason the LHC is equipped with a hierarchy of collimators in IR3: primary, secondary and absorber collimators. After every collimator alignment or change of machine configuration, the off-momentum cleaning efficiency is validated with loss maps at low intensity. We describe here the improved technique used in 2015 to generate such loss maps without completely dumping the beam into the collimators. The achieved performance of the collimation system for momentum cleaning is reviewed.


international conference on supercomputing | 2014

Overview of the FLUKA code

G. Battistoni; Till Boehlen; F. Cerutti; Pik Wai Chin; Luigi Salvatore Esposito; A. Fassò; A. Ferrari; Alessio Mereghetti; Pablo G. Ortega; Johannes Ranft; S. Roesler; P. Sala; Vasilis Vlachoudis


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2013

Sources of machine-induced background in the ATLAS and CMS detectors at the CERN Large Hadron Collider

Roderik Bruce; R. Assmann; V. Boccone; Giuseppe Bregliozzi; H. Burkhardt; F. Cerutti; A. Ferrari; M. Huhtinen; Anton Lechner; Y. Levinsen; Alessio Mereghetti; N.V. Mokhov; I.S. Tropin; V. Vlachoudis


Archive | 2013

SIXTRACK-FLUKA ACTIVE COUPLING FOR THE UPGRADE OF THE SPS SCRAPERS

Alessio Mereghetti; F. Cerutti; R. De Maria; B. Goddard; V. Kain; M. Meddahi; Ö.Mete; Yannis Papaphilippou; D.Pastor Sinuela; Vasilis Vlachoudis


arXiv: Accelerator Physics | 2013

Progress with the Upgrade of the SPS for the HL-LHC Era

B. Goddard; Theodoros Argyropoulos; Hannes Bartosik; W. Bartmann; T Bohl; F. Caspers; K. Cornelis; H.Damerau; L.N.Drøsdal; L. Ducimetière; R. Garoby; M. Gourber-Pace; Wolfgang Höfle; Giovanni Iadarola; L. Jensen; V. Kain; R. Losito; M. Meddahi; Alessio Mereghetti; V. Mertens; E. Montesinos; J. E. Müller; Yannis Papaphilippou; G. Rumolo; Benoit Salvant; E.N.Shaposhnikova; M.Taborelli; H. Timko; F. Velotti; E. Gianfelice-Wendt

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