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Effect of a resonant excitation on the evolution of the beam emittance and halo population
Collimation with hollow electron beams or lenses (HEL) is currently one of the most promising concepts for active halo control in HL-LHC. In previous studies it has been shown that the halo can be efficiently removed with a hollow electron lens. Equally important as an efficient removal of the halo,...
Autores principales: | , , , , , , , , |
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Lenguaje: | eng |
Publicado: |
2018
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Materias: | |
Acceso en línea: | http://cds.cern.ch/record/2305121 |
_version_ | 1780957496584699904 |
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author | Fitterer, Miriam Stancari, Giulio Valishev, Alexander Bruce, Roderik Redaelli, Stefano Salvachua Ferrando, Belen Maria Valuch, Daniel Valentino, Gianluca Wagner, Joschka |
author_facet | Fitterer, Miriam Stancari, Giulio Valishev, Alexander Bruce, Roderik Redaelli, Stefano Salvachua Ferrando, Belen Maria Valuch, Daniel Valentino, Gianluca Wagner, Joschka |
author_sort | Fitterer, Miriam |
collection | CERN |
description | Collimation with hollow electron beams or lenses (HEL) is currently one of the most promising concepts for active halo control in HL-LHC. In previous studies it has been shown that the halo can be efficiently removed with a hollow electron lens. Equally important as an efficient removal of the halo, is to demonstrate that the core stays unperturbed. In the case of an ideal hollow electron lens without bends, the field at the location of the beam core vanishes and the core thus remains unperturbed. In reality, the field at the beam core does not vanish entirely due to imperfections in the electron beam profile and the electron lens bends necessary to guide the electron in and out of the proton aperture. In particular, in the case of a pulsed operation of the electron lens the non-vanishing residual field induces noise on the proton beam. To identify the most sensitive pulsing patterns for the resonant mode and derive tolerances on the profile imperfections, a first MD (MD1415) was carried out on 24.08.2016 [1] and a second MD on 17.09.2017. In this note we present the results of the second MD (MD2167), which focused on confirming a part of the results of the first MD and testing in addition a resonant excitation for which no effect on the beam core is expected and the effect of random uniform noise in addition. |
id | cern-2305121 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2018 |
record_format | invenio |
spelling | cern-23051212019-09-30T06:29:59Zhttp://cds.cern.ch/record/2305121engFitterer, MiriamStancari, GiulioValishev, AlexanderBruce, RoderikRedaelli, StefanoSalvachua Ferrando, Belen MariaValuch, DanielValentino, GianlucaWagner, JoschkaEffect of a resonant excitation on the evolution of the beam emittance and halo populationAccelerators and Storage RingsCollimation with hollow electron beams or lenses (HEL) is currently one of the most promising concepts for active halo control in HL-LHC. In previous studies it has been shown that the halo can be efficiently removed with a hollow electron lens. Equally important as an efficient removal of the halo, is to demonstrate that the core stays unperturbed. In the case of an ideal hollow electron lens without bends, the field at the location of the beam core vanishes and the core thus remains unperturbed. In reality, the field at the beam core does not vanish entirely due to imperfections in the electron beam profile and the electron lens bends necessary to guide the electron in and out of the proton aperture. In particular, in the case of a pulsed operation of the electron lens the non-vanishing residual field induces noise on the proton beam. To identify the most sensitive pulsing patterns for the resonant mode and derive tolerances on the profile imperfections, a first MD (MD1415) was carried out on 24.08.2016 [1] and a second MD on 17.09.2017. In this note we present the results of the second MD (MD2167), which focused on confirming a part of the results of the first MD and testing in addition a resonant excitation for which no effect on the beam core is expected and the effect of random uniform noise in addition.CERN-ACC-NOTE-2018-0007oai:cds.cern.ch:23051212018-02-20 |
spellingShingle | Accelerators and Storage Rings Fitterer, Miriam Stancari, Giulio Valishev, Alexander Bruce, Roderik Redaelli, Stefano Salvachua Ferrando, Belen Maria Valuch, Daniel Valentino, Gianluca Wagner, Joschka Effect of a resonant excitation on the evolution of the beam emittance and halo population |
title | Effect of a resonant excitation on the evolution of the beam emittance and halo population |
title_full | Effect of a resonant excitation on the evolution of the beam emittance and halo population |
title_fullStr | Effect of a resonant excitation on the evolution of the beam emittance and halo population |
title_full_unstemmed | Effect of a resonant excitation on the evolution of the beam emittance and halo population |
title_short | Effect of a resonant excitation on the evolution of the beam emittance and halo population |
title_sort | effect of a resonant excitation on the evolution of the beam emittance and halo population |
topic | Accelerators and Storage Rings |
url | http://cds.cern.ch/record/2305121 |
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