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Performance of the Crowbar of the LHC High Power RF System

The counter-rotating proton beams in the Large Hadron Collider (LHC) are captured and accelerated to their final energies by two identical 400 MHz Radio Frequency (RF) systems. The RF power source required for each beam comprises eight 300 kW klystrons. The output power of each klystron is fed via a...

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Detalles Bibliográficos
Autores principales: Ravidà, G, Brunner, O, Valuch, D
Lenguaje:eng
Publicado: 2012
Materias:
Acceso en línea:http://cds.cern.ch/record/1460942
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author Ravidà, G
Brunner, O
Valuch, D
author_facet Ravidà, G
Brunner, O
Valuch, D
author_sort Ravidà, G
collection CERN
description The counter-rotating proton beams in the Large Hadron Collider (LHC) are captured and accelerated to their final energies by two identical 400 MHz Radio Frequency (RF) systems. The RF power source required for each beam comprises eight 300 kW klystrons. The output power of each klystron is fed via a circulator and a waveguide line to the input coupler of a single-cell superconducting (SC) cavity. Each unit of four klystrons is powered by a -100kV/40A AC/DC power converter. A fast protection system (crowbar) protects the four klystrons in each of these units. Although the LHC RF system has shown has very good performance, operational experience has shown that the five-gap double-ended thyratrons used in the crowbar system suffer, from time to time, from auto-firing, which result in beam dumps. This paper presents the recent results obtained with an alternative solution based on solid state thyristors. Comparative measurements with the thyratron are shown.
id cern-1460942
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2012
record_format invenio
spelling cern-14609422022-08-17T13:28:52Zhttp://cds.cern.ch/record/1460942engRavidà, GBrunner, OValuch, DPerformance of the Crowbar of the LHC High Power RF SystemAccelerators and Storage RingsThe counter-rotating proton beams in the Large Hadron Collider (LHC) are captured and accelerated to their final energies by two identical 400 MHz Radio Frequency (RF) systems. The RF power source required for each beam comprises eight 300 kW klystrons. The output power of each klystron is fed via a circulator and a waveguide line to the input coupler of a single-cell superconducting (SC) cavity. Each unit of four klystrons is powered by a -100kV/40A AC/DC power converter. A fast protection system (crowbar) protects the four klystrons in each of these units. Although the LHC RF system has shown has very good performance, operational experience has shown that the five-gap double-ended thyratrons used in the crowbar system suffer, from time to time, from auto-firing, which result in beam dumps. This paper presents the recent results obtained with an alternative solution based on solid state thyristors. Comparative measurements with the thyratron are shown.CERN-ATS-2012-149oai:cds.cern.ch:14609422012-04-01
spellingShingle Accelerators and Storage Rings
Ravidà, G
Brunner, O
Valuch, D
Performance of the Crowbar of the LHC High Power RF System
title Performance of the Crowbar of the LHC High Power RF System
title_full Performance of the Crowbar of the LHC High Power RF System
title_fullStr Performance of the Crowbar of the LHC High Power RF System
title_full_unstemmed Performance of the Crowbar of the LHC High Power RF System
title_short Performance of the Crowbar of the LHC High Power RF System
title_sort performance of the crowbar of the lhc high power rf system
topic Accelerators and Storage Rings
url http://cds.cern.ch/record/1460942
work_keys_str_mv AT ravidag performanceofthecrowbarofthelhchighpowerrfsystem
AT brunnero performanceofthecrowbarofthelhchighpowerrfsystem
AT valuchd performanceofthecrowbarofthelhchighpowerrfsystem