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Positron Options for the Linac-Ring LHeC
The full physics program of a future Large Hadron electron Collider (LHeC) [1] requires both pe+ and pe− collisions. For a pulsed 140-GeV or an ERL-based 60-GeV Linac-Ring LHeC this implies a challenging rate of, respectively, about 1.8 × 1015 or 4.4 × 1016 e+/s at the collision point, which is abou...
Autores principales: | , , , , , , , , , , , |
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Lenguaje: | eng |
Publicado: |
2012
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Acceso en línea: | http://cds.cern.ch/record/1459907 |
_version_ | 1780925208075436032 |
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author | Zimmermann, F Brüning, O S Papaphilippou, Y Schulte, D Sievers, P Rinolfi, L Variola, A Zomer, F Braun, H H Yakimenko, V Bulyak, E V Klein, M |
author_facet | Zimmermann, F Brüning, O S Papaphilippou, Y Schulte, D Sievers, P Rinolfi, L Variola, A Zomer, F Braun, H H Yakimenko, V Bulyak, E V Klein, M |
author_sort | Zimmermann, F |
collection | CERN |
description | The full physics program of a future Large Hadron electron Collider (LHeC) [1] requires both pe+ and pe− collisions. For a pulsed 140-GeV or an ERL-based 60-GeV Linac-Ring LHeC this implies a challenging rate of, respectively, about 1.8 × 1015 or 4.4 × 1016 e+/s at the collision point, which is about 300 or 7000 times the rate previously obtained, at the SLAC Linear Collider (SLC). We consider providing this e+ rate through a combination of measures: (1) Reducing the required production rate from the e+ target through colliding e+ (and the LHC protons) several times before deceleration, by reusing the e+ over several acceleration/deceleration cycles, and by cooling them, e.g., with a compact tri-ring scheme or a conventional damping ring in the SPS tunnel. (2) Using an advanced target, e.g., W-granules, rotating wheel, slicedrod converter, or liquid metal jet, for converting gamma rays to e+. (3) Selecting the most powerful of several proposed gamma sources, namely Compton ERL, Compton storage ring, coherent pair production in a strong laser, or high-field undulator radiation from the high-energy lepton beam. We sketch some of these concepts, present example parameters; estimate the electrical power required, andmention open questions. |
id | cern-1459907 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2012 |
record_format | invenio |
spelling | cern-14599072022-08-17T13:26:23Zhttp://cds.cern.ch/record/1459907engZimmermann, FBrüning, O SPapaphilippou, YSchulte, DSievers, PRinolfi, LVariola, AZomer, FBraun, H HYakimenko, VBulyak, E VKlein, MPositron Options for the Linac-Ring LHeCAccelerators and Storage RingsThe full physics program of a future Large Hadron electron Collider (LHeC) [1] requires both pe+ and pe− collisions. For a pulsed 140-GeV or an ERL-based 60-GeV Linac-Ring LHeC this implies a challenging rate of, respectively, about 1.8 × 1015 or 4.4 × 1016 e+/s at the collision point, which is about 300 or 7000 times the rate previously obtained, at the SLAC Linear Collider (SLC). We consider providing this e+ rate through a combination of measures: (1) Reducing the required production rate from the e+ target through colliding e+ (and the LHC protons) several times before deceleration, by reusing the e+ over several acceleration/deceleration cycles, and by cooling them, e.g., with a compact tri-ring scheme or a conventional damping ring in the SPS tunnel. (2) Using an advanced target, e.g., W-granules, rotating wheel, slicedrod converter, or liquid metal jet, for converting gamma rays to e+. (3) Selecting the most powerful of several proposed gamma sources, namely Compton ERL, Compton storage ring, coherent pair production in a strong laser, or high-field undulator radiation from the high-energy lepton beam. We sketch some of these concepts, present example parameters; estimate the electrical power required, andmention open questions.CERN-ATS-2012-135oai:cds.cern.ch:14599072012-05-20 |
spellingShingle | Accelerators and Storage Rings Zimmermann, F Brüning, O S Papaphilippou, Y Schulte, D Sievers, P Rinolfi, L Variola, A Zomer, F Braun, H H Yakimenko, V Bulyak, E V Klein, M Positron Options for the Linac-Ring LHeC |
title | Positron Options for the Linac-Ring LHeC |
title_full | Positron Options for the Linac-Ring LHeC |
title_fullStr | Positron Options for the Linac-Ring LHeC |
title_full_unstemmed | Positron Options for the Linac-Ring LHeC |
title_short | Positron Options for the Linac-Ring LHeC |
title_sort | positron options for the linac-ring lhec |
topic | Accelerators and Storage Rings |
url | http://cds.cern.ch/record/1459907 |
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