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The Tuning Algorithm of the LHC 400 MHz Superconducting Cavities

The LHC Superconducting 400 MHz cavities are of the single-cell type, equipped with a movable coupler allowing for a range of loaded Q from 20000 to 180000. Their mechanical tuner has a range of 250 kHz with a 25 Hz resolution. The LHC bunch spacing is 25 ns but the filling pattern exhibits various...

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Autor principal: Baudrenghien, P
Lenguaje:eng
Publicado: 2007
Materias:
Acceso en línea:http://cds.cern.ch/record/1014303
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author Baudrenghien, P
author_facet Baudrenghien, P
author_sort Baudrenghien, P
collection CERN
description The LHC Superconducting 400 MHz cavities are of the single-cell type, equipped with a movable coupler allowing for a range of loaded Q from 20000 to 180000. Their mechanical tuner has a range of 250 kHz with a 25 Hz resolution. The LHC bunch spacing is 25 ns but the filling pattern exhibits various gaps free of particles and of different length. Consequently the RF beam current at 400 MHz is also modulated. The largest gap has a length of 3s to accommodate for the rise-time of the beam dump kicker. It will always be kept free of particles. With the strong RF feedback the decay time of the cavity field is between one and two s, much smaller than the revolution period (90 s). Hence two steady state situations are encountered during one turn: The klystron power toggles between beam and no-beam values as the RF feedback keeps the field constant. The tuner position is set to keep the klystron power equal in both cases (Half Detuning). This note presents the tuning algorithm that sets and keeps the tuner at this optimal position.
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spelling cern-10143032019-09-30T06:29:59Zhttp://cds.cern.ch/record/1014303engBaudrenghien, PThe Tuning Algorithm of the LHC 400 MHz Superconducting CavitiesAccelerators and Storage RingsThe LHC Superconducting 400 MHz cavities are of the single-cell type, equipped with a movable coupler allowing for a range of loaded Q from 20000 to 180000. Their mechanical tuner has a range of 250 kHz with a 25 Hz resolution. The LHC bunch spacing is 25 ns but the filling pattern exhibits various gaps free of particles and of different length. Consequently the RF beam current at 400 MHz is also modulated. The largest gap has a length of 3s to accommodate for the rise-time of the beam dump kicker. It will always be kept free of particles. With the strong RF feedback the decay time of the cavity field is between one and two s, much smaller than the revolution period (90 s). Hence two steady state situations are encountered during one turn: The klystron power toggles between beam and no-beam values as the RF feedback keeps the field constant. The tuner position is set to keep the klystron power equal in both cases (Half Detuning). This note presents the tuning algorithm that sets and keeps the tuner at this optimal position.AB-Note-2007-011CERN-AB-Note-2007-011oai:cds.cern.ch:10143032007-02-05
spellingShingle Accelerators and Storage Rings
Baudrenghien, P
The Tuning Algorithm of the LHC 400 MHz Superconducting Cavities
title The Tuning Algorithm of the LHC 400 MHz Superconducting Cavities
title_full The Tuning Algorithm of the LHC 400 MHz Superconducting Cavities
title_fullStr The Tuning Algorithm of the LHC 400 MHz Superconducting Cavities
title_full_unstemmed The Tuning Algorithm of the LHC 400 MHz Superconducting Cavities
title_short The Tuning Algorithm of the LHC 400 MHz Superconducting Cavities
title_sort tuning algorithm of the lhc 400 mhz superconducting cavities
topic Accelerators and Storage Rings
url http://cds.cern.ch/record/1014303
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