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Impact of detector solenoid on the Compact Linear Collider luminosity performance
In order to obtain the necessary luminosity with a reasonable amount of beam power, the Compact Linear Collider (CLIC) design includes an unprecedented collision beam size of {\sigma} = 1 nm vertically and {\sigma} = 45 nm horizontally. Given the small and very flat beams, the luminosity can be sign...
Autores principales: | , , , |
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Lenguaje: | eng |
Publicado: |
2013
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1103/PhysRevSTAB.17.051002 https://dx.doi.org/10.1103/PhysRevSTAB.17.079901 http://cds.cern.ch/record/1634029 |
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author | Inntjore Levinsen, Y. Dalena, Barbara Tomás, Rogelio Schulte, Daniel |
author_facet | Inntjore Levinsen, Y. Dalena, Barbara Tomás, Rogelio Schulte, Daniel |
author_sort | Inntjore Levinsen, Y. |
collection | CERN |
description | In order to obtain the necessary luminosity with a reasonable amount of beam power, the Compact Linear Collider (CLIC) design includes an unprecedented collision beam size of {\sigma} = 1 nm vertically and {\sigma} = 45 nm horizontally. Given the small and very flat beams, the luminosity can be significantly degraded from the impact of the experimental solenoid field in combination with a large crossing angle. Main effects include y-x'-coupling and increase of vertical dispersion. Additionally, Incoherent Synchrotron Radiation (ISR) from the orbit deflection created by the solenoid field, increases the beam emittance. A detailed study of the impact from a realistic solenoid field and the associated correction techniques for the CLIC Final Focus is presented. In particular, the impact of techniques to compensate the beam optics distortions due to the detector solenoid main field and its overlap with the final focus magnets are shown. The unrecoverable luminosity loss due to ISR has been evaluated, and found to be in the range 4-5 % for the solenoid design under study. |
id | cern-1634029 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2013 |
record_format | invenio |
spelling | cern-16340292023-06-29T04:15:50Zdoi:10.1103/PhysRevSTAB.17.051002doi:10.1103/PhysRevSTAB.17.079901http://cds.cern.ch/record/1634029engInntjore Levinsen, Y.Dalena, BarbaraTomás, RogelioSchulte, DanielImpact of detector solenoid on the Compact Linear Collider luminosity performanceAccelerators and Storage RingsIn order to obtain the necessary luminosity with a reasonable amount of beam power, the Compact Linear Collider (CLIC) design includes an unprecedented collision beam size of {\sigma} = 1 nm vertically and {\sigma} = 45 nm horizontally. Given the small and very flat beams, the luminosity can be significantly degraded from the impact of the experimental solenoid field in combination with a large crossing angle. Main effects include y-x'-coupling and increase of vertical dispersion. Additionally, Incoherent Synchrotron Radiation (ISR) from the orbit deflection created by the solenoid field, increases the beam emittance. A detailed study of the impact from a realistic solenoid field and the associated correction techniques for the CLIC Final Focus is presented. In particular, the impact of techniques to compensate the beam optics distortions due to the detector solenoid main field and its overlap with the final focus magnets are shown. The unrecoverable luminosity loss due to ISR has been evaluated, and found to be in the range 4-5 % for the solenoid design under study.<p>In order to obtain the necessary luminosity with a reasonable amount of beam power, the Compact LInear Collider (CLIC) design includes an unprecedented collision beam size of <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi>σ</mml:mi></mml:mrow><mml:mrow><mml:mi>y</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mn>1</mml:mn><mml:mtext> </mml:mtext><mml:mi>nm</mml:mi></mml:mrow></mml:math></inline-formula> vertically and <inline-formula><mml:math display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi>σ</mml:mi></mml:mrow><mml:mrow><mml:mi>x</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mn>45</mml:mn><mml:mtext> </mml:mtext><mml:mi>nm</mml:mi></mml:mrow></mml:math></inline-formula> horizontally. With exceptionally small and flat beams, the luminosity can be significantly degraded due to the combination of the experimental solenoid field and a large crossing angle. The two main effects reducing the luminosity are <inline-formula><mml:math display="inline"><mml:mrow><mml:mi mathvariant="normal">y</mml:mi><mml:mtext>-</mml:mtext><mml:msup><mml:mrow><mml:mi mathvariant="normal">x</mml:mi></mml:mrow><mml:mrow><mml:mo>′</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math></inline-formula>-coupling and an increase of vertical dispersion. Additionally, incoherent synchrotron radiation (ISR) from the orbit deflection created by the solenoid field increases the beam emittance and results in unrecoverable luminosity degradation. A novel approach to evaluate the ISR effect from a realistic solenoid field without knowledge of the full compensation of the geometric aberrations is presented. This approach is confirmed by a detailed study of the correction techniques to compensate the beam optics distortions. The unrecoverable luminosity loss due to ISR for CLIC at 3 TeV has been evaluated, and found to be around 4% to 5% for the solenoid design under study.</p>In order to obtain the necessary luminosity with a reasonable amount of beam power, the Compact Linear Collider (CLIC) design includes an unprecedented collision beam size of {\sigma} = 1 nm vertically and {\sigma} = 45 nm horizontally. Given the small and very flat beams, the luminosity can be significantly degraded from the impact of the experimental solenoid field in combination with a large crossing angle. Main effects include y-x'-coupling and increase of vertical dispersion. Additionally, Incoherent Synchrotron Radiation (ISR) from the orbit deflection created by the solenoid field, increases the beam emittance. A detailed study of the impact from a realistic solenoid field and the associated correction techniques for the CLIC Final Focus is presented. In particular, the impact of techniques to compensate the beam optics distortions due to the detector solenoid main field and its overlap with the final focus magnets are shown. The unrecoverable luminosity loss due to ISR has been evaluated, and found to be in the range 4-5 % for the solenoid design under study.arXiv:1312.1586oai:cds.cern.ch:16340292013-12-05 |
spellingShingle | Accelerators and Storage Rings Inntjore Levinsen, Y. Dalena, Barbara Tomás, Rogelio Schulte, Daniel Impact of detector solenoid on the Compact Linear Collider luminosity performance |
title | Impact of detector solenoid on the Compact Linear Collider luminosity performance |
title_full | Impact of detector solenoid on the Compact Linear Collider luminosity performance |
title_fullStr | Impact of detector solenoid on the Compact Linear Collider luminosity performance |
title_full_unstemmed | Impact of detector solenoid on the Compact Linear Collider luminosity performance |
title_short | Impact of detector solenoid on the Compact Linear Collider luminosity performance |
title_sort | impact of detector solenoid on the compact linear collider luminosity performance |
topic | Accelerators and Storage Rings |
url | https://dx.doi.org/10.1103/PhysRevSTAB.17.051002 https://dx.doi.org/10.1103/PhysRevSTAB.17.079901 http://cds.cern.ch/record/1634029 |
work_keys_str_mv | AT inntjorelevinseny impactofdetectorsolenoidonthecompactlinearcolliderluminosityperformance AT dalenabarbara impactofdetectorsolenoidonthecompactlinearcolliderluminosityperformance AT tomasrogelio impactofdetectorsolenoidonthecompactlinearcolliderluminosityperformance AT schultedaniel impactofdetectorsolenoidonthecompactlinearcolliderluminosityperformance |