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Linac and damping ring designs for the FCC-ee
We report the design of the pre-injector chain for the Future Circular e$^+$e$^−$ Collider (FCC-ee) system. The electron beam from a low-emittance RF gun is accelerated by an S-band linac up to 6 GeV. A damping ring at 1.54 GeV is required for emittance cooling of the positron beam. The intermediate...
Autores principales: | , , , , , , , , , , , , , , , , , |
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Lenguaje: | eng |
Publicado: |
2019
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.18429/JACoW-IPAC2019-MOPMP002 http://cds.cern.ch/record/2696111 |
_version_ | 1780964187961294848 |
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author | Ogur, Salim Barnyakov, Alexey Chaikovska, Iryna Chehab, Robert Furukawa, Kazuro Iida, Naoko Kamitani, Takuya Levichev, Alexey Martyshkin, Pavel Miyahara, Fusashi Nikiforov, Danila Oide, Katsunobu Ozcan, Erkcan Papaphilippou, Yannis Polozov, Sergey Rinolfi, Louis Yaman, Fatih Zimmermann, Frank |
author_facet | Ogur, Salim Barnyakov, Alexey Chaikovska, Iryna Chehab, Robert Furukawa, Kazuro Iida, Naoko Kamitani, Takuya Levichev, Alexey Martyshkin, Pavel Miyahara, Fusashi Nikiforov, Danila Oide, Katsunobu Ozcan, Erkcan Papaphilippou, Yannis Polozov, Sergey Rinolfi, Louis Yaman, Fatih Zimmermann, Frank |
author_sort | Ogur, Salim |
collection | CERN |
description | We report the design of the pre-injector chain for the Future Circular e$^+$e$^−$ Collider (FCC-ee) system. The electron beam from a low-emittance RF gun is accelerated by an S-band linac up to 6 GeV. A damping ring at 1.54 GeV is required for emittance cooling of the positron beam. The intermediate energy step from the exit of the S-band linac at 6 GeV to the 20 GeV injection energy of the top-up booster can be provided by the modified Super Proton Synchrotron (SPS), serving as a pre-booster ring (PBR). An alternative option to reach 20 GeV energy would be to extend the S-band linac with a C- or X-band linac. An overall cost optimisation will determine the choice of the final configuration. Beam loss and emittance dilution in the linac due to space charge effects, wakefields, and misalignment of accelerator components can be mitigated by RF phasing and orbit steering. Start-to-end simulations examine the beam transport through the linac up to either 6 GeV or 20 GeV. The results indicate large design margins. Simulations of the beam dynamics in the damping ring (DR) demonstrate a sufficiently large momentum acceptance. Effects of intrabeam scattering and electron cloud instability in the DR are also studied. |
id | oai-inspirehep.net-1743390 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2019 |
record_format | invenio |
spelling | oai-inspirehep.net-17433902020-09-28T09:48:01Zdoi:10.18429/JACoW-IPAC2019-MOPMP002http://cds.cern.ch/record/2696111engOgur, SalimBarnyakov, AlexeyChaikovska, IrynaChehab, RobertFurukawa, KazuroIida, NaokoKamitani, TakuyaLevichev, AlexeyMartyshkin, PavelMiyahara, FusashiNikiforov, DanilaOide, KatsunobuOzcan, ErkcanPapaphilippou, YannisPolozov, SergeyRinolfi, LouisYaman, FatihZimmermann, FrankLinac and damping ring designs for the FCC-eeAccelerators and Storage RingsWe report the design of the pre-injector chain for the Future Circular e$^+$e$^−$ Collider (FCC-ee) system. The electron beam from a low-emittance RF gun is accelerated by an S-band linac up to 6 GeV. A damping ring at 1.54 GeV is required for emittance cooling of the positron beam. The intermediate energy step from the exit of the S-band linac at 6 GeV to the 20 GeV injection energy of the top-up booster can be provided by the modified Super Proton Synchrotron (SPS), serving as a pre-booster ring (PBR). An alternative option to reach 20 GeV energy would be to extend the S-band linac with a C- or X-band linac. An overall cost optimisation will determine the choice of the final configuration. Beam loss and emittance dilution in the linac due to space charge effects, wakefields, and misalignment of accelerator components can be mitigated by RF phasing and orbit steering. Start-to-end simulations examine the beam transport through the linac up to either 6 GeV or 20 GeV. The results indicate large design margins. Simulations of the beam dynamics in the damping ring (DR) demonstrate a sufficiently large momentum acceptance. Effects of intrabeam scattering and electron cloud instability in the DR are also studied.CERN-ACC-2019-073oai:inspirehep.net:17433902019 |
spellingShingle | Accelerators and Storage Rings Ogur, Salim Barnyakov, Alexey Chaikovska, Iryna Chehab, Robert Furukawa, Kazuro Iida, Naoko Kamitani, Takuya Levichev, Alexey Martyshkin, Pavel Miyahara, Fusashi Nikiforov, Danila Oide, Katsunobu Ozcan, Erkcan Papaphilippou, Yannis Polozov, Sergey Rinolfi, Louis Yaman, Fatih Zimmermann, Frank Linac and damping ring designs for the FCC-ee |
title | Linac and damping ring designs for the FCC-ee |
title_full | Linac and damping ring designs for the FCC-ee |
title_fullStr | Linac and damping ring designs for the FCC-ee |
title_full_unstemmed | Linac and damping ring designs for the FCC-ee |
title_short | Linac and damping ring designs for the FCC-ee |
title_sort | linac and damping ring designs for the fcc-ee |
topic | Accelerators and Storage Rings |
url | https://dx.doi.org/10.18429/JACoW-IPAC2019-MOPMP002 http://cds.cern.ch/record/2696111 |
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