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Production of Low-Energy Antiprotons
The production, collection and deceleration of antiprotons is reviewed with the aim of establishing guidelines for the design of a simple yet efficient source of stopped antiprotons. A high-energy (20-100 GeV) high-intensity (~ 1013 protons/pulse) proton accelerator is needed to produce antiprotons...
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Lenguaje: | eng |
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1996
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Acceso en línea: | http://cds.cern.ch/record/311679 |
_version_ | 1780890115086745600 |
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author | Möhl, D |
author_facet | Möhl, D |
author_sort | Möhl, D |
collection | CERN |
description | The production, collection and deceleration of antiprotons is reviewed with the aim of establishing guidelines for the design of a simple yet efficient source of stopped antiprotons. A high-energy (20-100 GeV) high-intensity (~ 1013 protons/pulse) proton accelerator is needed to produce antiprotons in copious numbers. A 'passive' conversion-target consisting of a thin iridium rod embedded in graphite, and a magnetic-horn type lens to collect the antiproton flux from the target represent a good compromise between yield and reliability. To transport the flux to low energy a large-acceptance cooling and deceleration ring working up to an energy equal to one-eighth to one-tenth of the primary proton energy is required. Stochastic cooling (at high energy) and electron cooling (at lower energy) are indispensable for providing low-energy beams of useful density. |
id | cern-311679 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 1996 |
record_format | invenio |
spelling | cern-3116792021-11-11T09:52:21Zhttp://cds.cern.ch/record/311679engMöhl, DProduction of Low-Energy AntiprotonsAccelerators and Storage RingsThe production, collection and deceleration of antiprotons is reviewed with the aim of establishing guidelines for the design of a simple yet efficient source of stopped antiprotons. A high-energy (20-100 GeV) high-intensity (~ 1013 protons/pulse) proton accelerator is needed to produce antiprotons in copious numbers. A 'passive' conversion-target consisting of a thin iridium rod embedded in graphite, and a magnetic-horn type lens to collect the antiproton flux from the target represent a good compromise between yield and reliability. To transport the flux to low energy a large-acceptance cooling and deceleration ring working up to an energy equal to one-eighth to one-tenth of the primary proton energy is required. Stochastic cooling (at high energy) and electron cooling (at lower energy) are indispensable for providing low-energy beams of useful density.CERN-PS-96-034-DIoai:cds.cern.ch:3116791996-09-17 |
spellingShingle | Accelerators and Storage Rings Möhl, D Production of Low-Energy Antiprotons |
title | Production of Low-Energy Antiprotons |
title_full | Production of Low-Energy Antiprotons |
title_fullStr | Production of Low-Energy Antiprotons |
title_full_unstemmed | Production of Low-Energy Antiprotons |
title_short | Production of Low-Energy Antiprotons |
title_sort | production of low-energy antiprotons |
topic | Accelerators and Storage Rings |
url | http://cds.cern.ch/record/311679 |
work_keys_str_mv | AT mohld productionoflowenergyantiprotons |