{"paper":{"title":"Simulations and measurements of beam loss patterns at the CERN Large Hadron Collider","license":"http://creativecommons.org/licenses/by/3.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"physics.acc-ph","authors_text":"A. Ferrari, A. Marsili, A. Mereghetti, A. Rossi, B. Salvachua, C. Bracco, C. Tambasco, D. Deboy, D. Mirarchi, D. Wollmann, E. Quaranta, E. Skordis, F. Cerutti, G. Robert-Demolaize, G. Valentino, L. Lari, M. Brugger, M. Cauchi, R. Bruce, R.W. Assmann, S. Redaelli, T. Weiler, V. Boccone, V. Vlachoudis","submitted_at":"2014-09-10T15:51:09Z","abstract_excerpt":"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"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.3123","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"}