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Adjustment of a double drift harmonic buncher and bunch shape measurements
The longitudinal beam matching of the new 50 MeV linac is achieved with a double drift harmonic buncher. For optimum bunching efficiency the RF phase difference between the two cavities should be known and controlled to about 1 degrees (at 202.56 MHz). The adjustment of the RF levels and phases is b...
Autores principales: | , , |
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Lenguaje: | eng |
Publicado: |
1976
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Materias: | |
Acceso en línea: | http://cds.cern.ch/record/873817 |
_version_ | 1780907723604361216 |
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author | Knott, J Warner, D Weiss, M |
author_facet | Knott, J Warner, D Weiss, M |
author_sort | Knott, J |
collection | CERN |
description | The longitudinal beam matching of the new 50 MeV linac is achieved with a double drift harmonic buncher. For optimum bunching efficiency the RF phase difference between the two cavities should be known and controlled to about 1 degrees (at 202.56 MHz). The adjustment of the RF levels and phases is based on observations of the bunch form via a broad-band probe connected to a travelling wave oscilloscope. The time base is tightly locked to the RF by a specially developed circuit allowing a systematic study of different bunching conditions. A comparison is made between some preliminary measurements and the waveforms predicted by a simplified theory. (3 refs). |
id | cern-873817 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 1976 |
record_format | invenio |
spelling | cern-8738172019-09-30T06:29:59Zhttp://cds.cern.ch/record/873817engKnott, JWarner, DWeiss, MAdjustment of a double drift harmonic buncher and bunch shape measurementsNuclear PhysicsThe longitudinal beam matching of the new 50 MeV linac is achieved with a double drift harmonic buncher. For optimum bunching efficiency the RF phase difference between the two cavities should be known and controlled to about 1 degrees (at 202.56 MHz). The adjustment of the RF levels and phases is based on observations of the bunch form via a broad-band probe connected to a travelling wave oscilloscope. The time base is tightly locked to the RF by a specially developed circuit allowing a systematic study of different bunching conditions. A comparison is made between some preliminary measurements and the waveforms predicted by a simplified theory. (3 refs).oai:cds.cern.ch:8738171976 |
spellingShingle | Nuclear Physics Knott, J Warner, D Weiss, M Adjustment of a double drift harmonic buncher and bunch shape measurements |
title | Adjustment of a double drift harmonic buncher and bunch shape measurements |
title_full | Adjustment of a double drift harmonic buncher and bunch shape measurements |
title_fullStr | Adjustment of a double drift harmonic buncher and bunch shape measurements |
title_full_unstemmed | Adjustment of a double drift harmonic buncher and bunch shape measurements |
title_short | Adjustment of a double drift harmonic buncher and bunch shape measurements |
title_sort | adjustment of a double drift harmonic buncher and bunch shape measurements |
topic | Nuclear Physics |
url | http://cds.cern.ch/record/873817 |
work_keys_str_mv | AT knottj adjustmentofadoubledriftharmonicbuncherandbunchshapemeasurements AT warnerd adjustmentofadoubledriftharmonicbuncherandbunchshapemeasurements AT weissm adjustmentofadoubledriftharmonicbuncherandbunchshapemeasurements |