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Improvement of PLL algorithm for the LEP Q-meter

The PLL (Phase Locked Loop) has two modes: search mode and locking mode. The mode is determined by how far apart the internal frequency is from the external frequency. When the internal - and exter nal frequencies are close, the PLL is in locking mode. While locking on the external frequency, the PL...

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Autor principal: Berrig, O E
Lenguaje:eng
Publicado: 1998
Materias:
Acceso en línea:http://cds.cern.ch/record/702445
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author Berrig, O E
author_facet Berrig, O E
author_sort Berrig, O E
collection CERN
description The PLL (Phase Locked Loop) has two modes: search mode and locking mode. The mode is determined by how far apart the internal frequency is from the external frequency. When the internal - and exter nal frequencies are close, the PLL is in locking mode. While locking on the external frequency, the PLL can largely be expressed as a linear term superimposed with a small "noise" term. We can t herefore calculate a transfer function that will completely describe the performance of the PLL apart from the precision, which is determined by the noise term. Two ideas are presented on how to re duce the noise term. The first idea is to compensate the noise term with an equal value of opposite sign. This completely removes the noise when the PLL locks on a steady frequency. Unfortunately it can not be used for the LEP Q-meter which is plagued by the presence of satellite frequencies. For other equipment with cleaner spectra, the method can improve their precision dramatically. T he second idea reduces the noise level with a factor 2 but limits the locking range. This will be tested out on the LEP Q-meter.
id cern-702445
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1998
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spelling cern-7024452023-05-11T12:03:24Zhttp://cds.cern.ch/record/702445engBerrig, O EImprovement of PLL algorithm for the LEP Q-meterAccelerators and Storage RingsThe PLL (Phase Locked Loop) has two modes: search mode and locking mode. The mode is determined by how far apart the internal frequency is from the external frequency. When the internal - and exter nal frequencies are close, the PLL is in locking mode. While locking on the external frequency, the PLL can largely be expressed as a linear term superimposed with a small "noise" term. We can t herefore calculate a transfer function that will completely describe the performance of the PLL apart from the precision, which is determined by the noise term. Two ideas are presented on how to re duce the noise term. The first idea is to compensate the noise term with an equal value of opposite sign. This completely removes the noise when the PLL locks on a steady frequency. Unfortunately it can not be used for the LEP Q-meter which is plagued by the presence of satellite frequencies. For other equipment with cleaner spectra, the method can improve their precision dramatically. T he second idea reduces the noise level with a factor 2 but limits the locking range. This will be tested out on the LEP Q-meter.SL-Note-98-024-BIoai:cds.cern.ch:7024451998-04-09
spellingShingle Accelerators and Storage Rings
Berrig, O E
Improvement of PLL algorithm for the LEP Q-meter
title Improvement of PLL algorithm for the LEP Q-meter
title_full Improvement of PLL algorithm for the LEP Q-meter
title_fullStr Improvement of PLL algorithm for the LEP Q-meter
title_full_unstemmed Improvement of PLL algorithm for the LEP Q-meter
title_short Improvement of PLL algorithm for the LEP Q-meter
title_sort improvement of pll algorithm for the lep q-meter
topic Accelerators and Storage Rings
url http://cds.cern.ch/record/702445
work_keys_str_mv AT berrigoe improvementofpllalgorithmforthelepqmeter