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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Main Authors: Evgenij Martynov, Basarab Nicolescu
Format: Article
Language:English
Published: SpringerOpen 2019-05-01
Series:European Physical Journal C: Particles and Fields
Online Access:http://link.springer.com/article/10.1140/epjc/s10052-019-6954-6
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spelling 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
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AT basarabnicolescu odderoneffectsinthedifferentialcrosssectionsattevatronandlhcenergies
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