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VHEeP: A very high energy electron-proton collider
Based on current CERN infrastructure, an electron–proton collider is proposed at a centre-of-mass energy of about 9 TeV. A 7 TeV LHC bunch is used as the proton driver to create a plasma wakefield which then accelerates electrons to 3 TeV, these then colliding with the other 7 TeV LHC proton beam. A...
Autores principales: | , |
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Lenguaje: | eng |
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2016
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1140/epjc/s10052-016-4316-1 http://cds.cern.ch/record/2157995 |
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author | Caldwell, A. Wing, M. |
author_facet | Caldwell, A. Wing, M. |
author_sort | Caldwell, A. |
collection | CERN |
description | Based on current CERN infrastructure, an electron–proton collider is proposed at a centre-of-mass energy of about 9 TeV. A 7 TeV LHC bunch is used as the proton driver to create a plasma wakefield which then accelerates electrons to 3 TeV, these then colliding with the other 7 TeV LHC proton beam. Although of very high energy, the collider has a modest projected integrated luminosity of 10–100 pb$^{-1}$ . For such a collider, with a centre-of-mass energy 30 times greater than HERA, parton momentum fractions, x, down to about $10^{-8}$ are accessible for photon virtualities, $Q^2$ , of 1 GeV$^2$ . The energy dependence of hadronic cross sections at high energies, such as the total photon–proton cross section, which has synergy with cosmic-ray physics, can be measured and QCD and the structure of matter better understood in a region where the effects are completely unknown. Searches at high $Q^2$ for physics beyond the Standard Model will be possible, in particular the significantly increased sensitivity to the production of leptoquarks. These and other physics highlights of a very high energy electron–proton collider are outlined. |
id | cern-2157995 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2016 |
record_format | invenio |
spelling | cern-21579952021-11-13T11:58:29Zdoi:10.1140/epjc/s10052-016-4316-1http://cds.cern.ch/record/2157995engCaldwell, A.Wing, M.VHEeP: A very high energy electron-proton colliderhep-phParticle Physics - Phenomenologyhep-exParticle Physics - ExperimentBased on current CERN infrastructure, an electron–proton collider is proposed at a centre-of-mass energy of about 9 TeV. A 7 TeV LHC bunch is used as the proton driver to create a plasma wakefield which then accelerates electrons to 3 TeV, these then colliding with the other 7 TeV LHC proton beam. Although of very high energy, the collider has a modest projected integrated luminosity of 10–100 pb$^{-1}$ . For such a collider, with a centre-of-mass energy 30 times greater than HERA, parton momentum fractions, x, down to about $10^{-8}$ are accessible for photon virtualities, $Q^2$ , of 1 GeV$^2$ . The energy dependence of hadronic cross sections at high energies, such as the total photon–proton cross section, which has synergy with cosmic-ray physics, can be measured and QCD and the structure of matter better understood in a region where the effects are completely unknown. Searches at high $Q^2$ for physics beyond the Standard Model will be possible, in particular the significantly increased sensitivity to the production of leptoquarks. These and other physics highlights of a very high energy electron–proton collider are outlined.Based on current CERN infrastructure, an electron--proton collider is proposed at a centre-of-mass energy of about 9 TeV. A 7 TeV LHC bunch is used as the proton driver to create a plasma wakefield which then accelerates electrons to 3\,TeV, these then colliding with the other 7 TeV LHC proton beam. Although of very high energy, the collider has a modest projected integrated luminosity of $10-100$ pb$^{-1}$. For such a collider, with a centre-of-mass energy 30 times greater than HERA, parton momentum fractions, $x$, down to about $10^{-8}$ are accessible for photon virtualities, $Q^2$, of 1 GeV$^2$. The energy dependence of hadronic cross sections at high energies, such as the the total photon--proton cross section, which has synergy with cosmic-ray physics, can be measured and QCD and the structure of matter better understood in a region where the effects are completely unknown. Searches at high $Q^2$ for physics beyond the Standard Model will be possible, in particular the significantly increased sensitivity to the production of leptoquarks. These and other physics highlights of a very high energy electron--proton collider are outlined.arXiv:1606.00783oai:cds.cern.ch:21579952016-06-02 |
spellingShingle | hep-ph Particle Physics - Phenomenology hep-ex Particle Physics - Experiment Caldwell, A. Wing, M. VHEeP: A very high energy electron-proton collider |
title | VHEeP: A very high energy electron-proton collider |
title_full | VHEeP: A very high energy electron-proton collider |
title_fullStr | VHEeP: A very high energy electron-proton collider |
title_full_unstemmed | VHEeP: A very high energy electron-proton collider |
title_short | VHEeP: A very high energy electron-proton collider |
title_sort | vheep: a very high energy electron-proton collider |
topic | hep-ph Particle Physics - Phenomenology hep-ex Particle Physics - Experiment |
url | https://dx.doi.org/10.1140/epjc/s10052-016-4316-1 http://cds.cern.ch/record/2157995 |
work_keys_str_mv | AT caldwella vheepaveryhighenergyelectronprotoncollider AT wingm vheepaveryhighenergyelectronprotoncollider |