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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...

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Detalles Bibliográficos
Autores principales: Caldwell, A., Wing, M.
Lenguaje:eng
Publicado: 2016
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.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2016
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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