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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Veröffentlicht in: | The European physical journal. C, Particles and fields Particles and fields, 2016-08, Vol.76 (8), p.1, Article 463 |
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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. |
doi_str_mv | 10.1140/epjc/s10052-016-4316-1 |
format | Article |
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-
1
. For such a collider, with a centre-of-mass energy 30 times greater than HERA, parton momentum fractions,
x
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10
-
8
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Q
2
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2
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Q
2
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-
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. 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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.</abstract><cop>Berlin/Heidelberg</cop><pub>Springer Berlin Heidelberg</pub><doi>10.1140/epjc/s10052-016-4316-1</doi><oa>free_for_read</oa></addata></record> |
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source | DOAJ Directory of Open Access Journals; SpringerLink Journals; EZB-FREE-00999 freely available EZB journals; Springer Nature OA Free Journals |
subjects | Astronomy Astrophysics and Cosmology Electrons Elementary Particles Hadrons Heavy Ions Measurement Science and Instrumentation Nuclear Energy Nuclear Physics Particle accelerators Particle collisions Physics Physics and Astronomy Quantum Field Theories Quantum Field Theory Regular Article - Experimental Physics String Theory |
title | VHEeP: a very high energy electron–proton collider |
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