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Photon Reflectivity Distributions from the LHC Beam Screen and their Implications on the Arc Beam Vacuum System
In particle accelerators with intense positively charged bunched beams, an electron cloud may induce beam instabilities and the related beam induced electron multipacting (BIEM), result in an undesired pressure rise and, in a cryogenic machine such as the Large Hadron Collider (LHC), introduce addit...
Autores principales: | , , , , , , , |
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Lenguaje: | eng |
Publicado: |
2003
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1016/j.apsusc.2004.05.271 http://cds.cern.ch/record/639793 |
_version_ | 1780900686653816832 |
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author | Cimino, R Baglin, V Collins, I R Giglia, A Mahne, N Nannarone, S Pasquali, L Pedio, M |
author_facet | Cimino, R Baglin, V Collins, I R Giglia, A Mahne, N Nannarone, S Pasquali, L Pedio, M |
author_sort | Cimino, R |
collection | CERN |
description | In particle accelerators with intense positively charged bunched beams, an electron cloud may induce beam instabilities and the related beam induced electron multipacting (BIEM), result in an undesired pressure rise and, in a cryogenic machine such as the Large Hadron Collider (LHC), introduce addition heat loads. When present, synchrotron radiation (SR) may generate a significant number of photoelectrons, that may play a role in determining the onset and the detailed properties of the electron-cloud related instability. Since electrons are constrained to move along field lines, those created on the accelerator equator in a strong vertical (dipole) field cannot participate in the ecloud build-up. Therefore, for the LHC there has been a continuous effort to find solutions to absorb the photons on the equator. The solution adopted for the LHC dipole beam screens is a saw-tooth structure on the illuminated equator. SR from a bending magnet beamline at ELETTRA, Italy (BEAR) has been used to measure the reflectivities (forward, backscattered and diffuse), for a flat and a saw-tooth structured Cu co-laminated surface using both white light SR, similar to the one emitted by LHC, and monochromatic light. Our data show that the saw-tooth structure does reduce the total reflectivity and modifies the photon energy distribution of the reflected photons. The implications of these results on the LHC arc vacuum system are discussed. |
id | cern-639793 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2003 |
record_format | invenio |
spelling | cern-6397932023-05-31T13:22:14Zdoi:10.1016/j.apsusc.2004.05.271http://cds.cern.ch/record/639793engCimino, RBaglin, VCollins, I RGiglia, AMahne, NNannarone, SPasquali, LPedio, MPhoton Reflectivity Distributions from the LHC Beam Screen and their Implications on the Arc Beam Vacuum SystemAccelerators and Storage RingsIn particle accelerators with intense positively charged bunched beams, an electron cloud may induce beam instabilities and the related beam induced electron multipacting (BIEM), result in an undesired pressure rise and, in a cryogenic machine such as the Large Hadron Collider (LHC), introduce addition heat loads. When present, synchrotron radiation (SR) may generate a significant number of photoelectrons, that may play a role in determining the onset and the detailed properties of the electron-cloud related instability. Since electrons are constrained to move along field lines, those created on the accelerator equator in a strong vertical (dipole) field cannot participate in the ecloud build-up. Therefore, for the LHC there has been a continuous effort to find solutions to absorb the photons on the equator. The solution adopted for the LHC dipole beam screens is a saw-tooth structure on the illuminated equator. SR from a bending magnet beamline at ELETTRA, Italy (BEAR) has been used to measure the reflectivities (forward, backscattered and diffuse), for a flat and a saw-tooth structured Cu co-laminated surface using both white light SR, similar to the one emitted by LHC, and monochromatic light. Our data show that the saw-tooth structure does reduce the total reflectivity and modifies the photon energy distribution of the reflected photons. The implications of these results on the LHC arc vacuum system are discussed.LHC-Project-Report-668CERN-LHC-Project-Report-668oai:cds.cern.ch:6397932003-08-25 |
spellingShingle | Accelerators and Storage Rings Cimino, R Baglin, V Collins, I R Giglia, A Mahne, N Nannarone, S Pasquali, L Pedio, M Photon Reflectivity Distributions from the LHC Beam Screen and their Implications on the Arc Beam Vacuum System |
title | Photon Reflectivity Distributions from the LHC Beam Screen and their Implications on the Arc Beam Vacuum System |
title_full | Photon Reflectivity Distributions from the LHC Beam Screen and their Implications on the Arc Beam Vacuum System |
title_fullStr | Photon Reflectivity Distributions from the LHC Beam Screen and their Implications on the Arc Beam Vacuum System |
title_full_unstemmed | Photon Reflectivity Distributions from the LHC Beam Screen and their Implications on the Arc Beam Vacuum System |
title_short | Photon Reflectivity Distributions from the LHC Beam Screen and their Implications on the Arc Beam Vacuum System |
title_sort | photon reflectivity distributions from the lhc beam screen and their implications on the arc beam vacuum system |
topic | Accelerators and Storage Rings |
url | https://dx.doi.org/10.1016/j.apsusc.2004.05.271 http://cds.cern.ch/record/639793 |
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