Odderon effects in the differential cross-sections at Tevatron and LHC energies
Abstract In the present paper, we extend the Froissaron-Maximal Odderon (FMO) approach at t different from 0. Our extended FMO approach gives an excellent description of the 3266 experimental points considered in a wide range of energies and momentum transferred. We show that the very interesting TO...
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Online Access: | http://link.springer.com/article/10.1140/epjc/s10052-019-6954-6 |
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doaj-6e7e6fdbfab848a2a7a231d084bc640b2020-11-25T03:10:56ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522019-05-0179611410.1140/epjc/s10052-019-6954-6Odderon effects in the differential cross-sections at Tevatron and LHC energiesEvgenij Martynov0Basarab Nicolescu1Bogolyubov Institute for Theoretical PhysicsFaculty of European Studies, Babes-Bolyai UniversityAbstract In the present paper, we extend the Froissaron-Maximal Odderon (FMO) approach at t different from 0. Our extended FMO approach gives an excellent description of the 3266 experimental points considered in a wide range of energies and momentum transferred. We show that the very interesting TOTEM results for proton–proton differential cross-section in the range 2.76–13 TeV, together with the Tevatron data for antiproton–proton at 1.8 and 1.96 TeV give further experimental evidence for the existence of the Odderon. One spectacular theoretical result is the fact that the difference in the dip-bump region between $${\bar{p}}p$$ p¯p and pp differential cross-sections is diminishing with increasing energies and for very high energies (say 100 TeV), the difference between $${\bar{p}}p$$ p¯p and pp in the dip-bump region is changing its sign: pp becomes bigger than $${\bar{p}}p$$ p¯p at |t| about 1 GeV$$^2$$ 2 . This is a typical Odderon effect. Another important – phenomenological – result of our approach is that the slope in pp scattering has a different behavior in t than the slope in $${\bar{p}}p$$ p¯p scattering. This is also a clear Odderon effect.http://link.springer.com/article/10.1140/epjc/s10052-019-6954-6 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Evgenij Martynov Basarab Nicolescu |
spellingShingle |
Evgenij Martynov Basarab Nicolescu Odderon effects in the differential cross-sections at Tevatron and LHC energies European Physical Journal C: Particles and Fields |
author_facet |
Evgenij Martynov Basarab Nicolescu |
author_sort |
Evgenij Martynov |
title |
Odderon effects in the differential cross-sections at Tevatron and LHC energies |
title_short |
Odderon effects in the differential cross-sections at Tevatron and LHC energies |
title_full |
Odderon effects in the differential cross-sections at Tevatron and LHC energies |
title_fullStr |
Odderon effects in the differential cross-sections at Tevatron and LHC energies |
title_full_unstemmed |
Odderon effects in the differential cross-sections at Tevatron and LHC energies |
title_sort |
odderon effects in the differential cross-sections at tevatron and lhc energies |
publisher |
SpringerOpen |
series |
European Physical Journal C: Particles and Fields |
issn |
1434-6044 1434-6052 |
publishDate |
2019-05-01 |
description |
Abstract In the present paper, we extend the Froissaron-Maximal Odderon (FMO) approach at t different from 0. Our extended FMO approach gives an excellent description of the 3266 experimental points considered in a wide range of energies and momentum transferred. We show that the very interesting TOTEM results for proton–proton differential cross-section in the range 2.76–13 TeV, together with the Tevatron data for antiproton–proton at 1.8 and 1.96 TeV give further experimental evidence for the existence of the Odderon. One spectacular theoretical result is the fact that the difference in the dip-bump region between $${\bar{p}}p$$ p¯p and pp differential cross-sections is diminishing with increasing energies and for very high energies (say 100 TeV), the difference between $${\bar{p}}p$$ p¯p and pp in the dip-bump region is changing its sign: pp becomes bigger than $${\bar{p}}p$$ p¯p at |t| about 1 GeV$$^2$$ 2 . This is a typical Odderon effect. Another important – phenomenological – result of our approach is that the slope in pp scattering has a different behavior in t than the slope in $${\bar{p}}p$$ p¯p scattering. This is also a clear Odderon effect. |
url |
http://link.springer.com/article/10.1140/epjc/s10052-019-6954-6 |
work_keys_str_mv |
AT evgenijmartynov odderoneffectsinthedifferentialcrosssectionsattevatronandlhcenergies AT basarabnicolescu odderoneffectsinthedifferentialcrosssectionsattevatronandlhcenergies |
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1724656311542480896 |