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Transformer ratio saturation in a beam-driven wakefield accelerator
We show that for beam-driven wakefield acceleration, the linearly ramped, equally spaced train of bunches typically considered to optimise the transformer ratio only works for flat-top bunches. Through theory and simulation, we explain that this behaviour is due to the unique properties of the plasm...
Autores principales: | , , |
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Lenguaje: | eng |
Publicado: |
AIP
2015
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1063/1.4938038 http://cds.cern.ch/record/2710804 |
_version_ | 1780965186189918208 |
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author | Farmer, J P Martorelli, R Pukhov, A |
author_facet | Farmer, J P Martorelli, R Pukhov, A |
author_sort | Farmer, J P |
collection | CERN |
description | We show that for beam-driven wakefield acceleration, the linearly ramped, equally spaced train of bunches typically considered to optimise the transformer ratio only works for flat-top bunches. Through theory and simulation, we explain that this behaviour is due to the unique properties of the plasma response to a flat-top density profile. Calculations of the optimal scaling for a train of Gaussian bunches show diminishing returns with increasing bunch number, tending towards saturation. For a periodic bunch train, a transformer ratio of 23 was achieved for 50 bunches, rising to 40 for a fully optimised beam. |
id | oai-inspirehep.net-1633713 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2015 |
publisher | AIP |
record_format | invenio |
spelling | oai-inspirehep.net-16337132020-02-24T09:50:54Zdoi:10.1063/1.4938038http://cds.cern.ch/record/2710804engFarmer, J PMartorelli, RPukhov, ATransformer ratio saturation in a beam-driven wakefield acceleratorAccelerators and Storage RingsAccelerators and Storage RingsWe show that for beam-driven wakefield acceleration, the linearly ramped, equally spaced train of bunches typically considered to optimise the transformer ratio only works for flat-top bunches. Through theory and simulation, we explain that this behaviour is due to the unique properties of the plasma response to a flat-top density profile. Calculations of the optimal scaling for a train of Gaussian bunches show diminishing returns with increasing bunch number, tending towards saturation. For a periodic bunch train, a transformer ratio of 23 was achieved for 50 bunches, rising to 40 for a fully optimised beam.AIPoai:inspirehep.net:16337132015 |
spellingShingle | Accelerators and Storage Rings Accelerators and Storage Rings Farmer, J P Martorelli, R Pukhov, A Transformer ratio saturation in a beam-driven wakefield accelerator |
title | Transformer ratio saturation in a beam-driven wakefield accelerator |
title_full | Transformer ratio saturation in a beam-driven wakefield accelerator |
title_fullStr | Transformer ratio saturation in a beam-driven wakefield accelerator |
title_full_unstemmed | Transformer ratio saturation in a beam-driven wakefield accelerator |
title_short | Transformer ratio saturation in a beam-driven wakefield accelerator |
title_sort | transformer ratio saturation in a beam-driven wakefield accelerator |
topic | Accelerators and Storage Rings Accelerators and Storage Rings |
url | https://dx.doi.org/10.1063/1.4938038 http://cds.cern.ch/record/2710804 |
work_keys_str_mv | AT farmerjp transformerratiosaturationinabeamdrivenwakefieldaccelerator AT martorellir transformerratiosaturationinabeamdrivenwakefieldaccelerator AT pukhova transformerratiosaturationinabeamdrivenwakefieldaccelerator |