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...
Ausführliche Beschreibung

Gespeichert in:

Autor*in:	Martynov, Evgenij [verfasserIn] Nicolescu, Basarab [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2019

Übergeordnetes Werk:	Enthalten in: The European physical journal - Berlin : Springer, 1998, 79(2019), 6 vom: 30. Mai
Übergeordnetes Werk:	volume:79 ; year:2019 ; number:6 ; day:30 ; month:05

Links:	Volltext

DOI / URN:	10.1140/epjc/s10052-019-6954-6

Katalog-ID:	SPR008381186

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520			\|a 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 %${\bar{p}}p%$ and pp differential cross-sections is diminishing with increasing energies and for very high energies (say 100 TeV), the difference between %${\bar{p}}p%$ and pp in the dip-bump region is changing its sign: pp becomes bigger than %${\bar{p}}p%$ at \|t\| about 1 GeV%$^2%$. 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 %${\bar{p}}p%$ scattering. This is also a clear Odderon effect.
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matchkey_str	article:14346052:2019----::deoefcsnhdfeetacosetostea
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allfields	10.1140/epjc/s10052-019-6954-6 doi (DE-627)SPR008381186 (SPR)s10052-019-6954-6-e DE-627 ger DE-627 rakwb eng 530 ASE 33.50 bkl Martynov, Evgenij verfasserin aut Odderon effects in the differential cross-sections at Tevatron and LHC energies 2019 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier 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 %${\bar{p}}p%$ and pp differential cross-sections is diminishing with increasing energies and for very high energies (say 100 TeV), the difference between %${\bar{p}}p%$ and pp in the dip-bump region is changing its sign: pp becomes bigger than %${\bar{p}}p%$ at \|t\| about 1 GeV%$^2%$. 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 %${\bar{p}}p%$ scattering. This is also a clear Odderon effect. Nicolescu, Basarab verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 79(2019), 6 vom: 30. Mai (DE-627)253722934 (DE-600)1459069-4 1434-6052 nnns volume:79 year:2019 number:6 day:30 month:05 https://dx.doi.org/10.1140/epjc/s10052-019-6954-6 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2031 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2119 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 33.50 ASE AR 79 2019 6 30 05
spelling	10.1140/epjc/s10052-019-6954-6 doi (DE-627)SPR008381186 (SPR)s10052-019-6954-6-e DE-627 ger DE-627 rakwb eng 530 ASE 33.50 bkl Martynov, Evgenij verfasserin aut Odderon effects in the differential cross-sections at Tevatron and LHC energies 2019 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier 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 %${\bar{p}}p%$ and pp differential cross-sections is diminishing with increasing energies and for very high energies (say 100 TeV), the difference between %${\bar{p}}p%$ and pp in the dip-bump region is changing its sign: pp becomes bigger than %${\bar{p}}p%$ at \|t\| about 1 GeV%$^2%$. 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 %${\bar{p}}p%$ scattering. This is also a clear Odderon effect. Nicolescu, Basarab verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 79(2019), 6 vom: 30. Mai (DE-627)253722934 (DE-600)1459069-4 1434-6052 nnns volume:79 year:2019 number:6 day:30 month:05 https://dx.doi.org/10.1140/epjc/s10052-019-6954-6 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2031 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2119 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 33.50 ASE AR 79 2019 6 30 05
allfields_unstemmed	10.1140/epjc/s10052-019-6954-6 doi (DE-627)SPR008381186 (SPR)s10052-019-6954-6-e DE-627 ger DE-627 rakwb eng 530 ASE 33.50 bkl Martynov, Evgenij verfasserin aut Odderon effects in the differential cross-sections at Tevatron and LHC energies 2019 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier 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 %${\bar{p}}p%$ and pp differential cross-sections is diminishing with increasing energies and for very high energies (say 100 TeV), the difference between %${\bar{p}}p%$ and pp in the dip-bump region is changing its sign: pp becomes bigger than %${\bar{p}}p%$ at \|t\| about 1 GeV%$^2%$. 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 %${\bar{p}}p%$ scattering. This is also a clear Odderon effect. Nicolescu, Basarab verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 79(2019), 6 vom: 30. Mai (DE-627)253722934 (DE-600)1459069-4 1434-6052 nnns volume:79 year:2019 number:6 day:30 month:05 https://dx.doi.org/10.1140/epjc/s10052-019-6954-6 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2031 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2119 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 33.50 ASE AR 79 2019 6 30 05
allfieldsGer	10.1140/epjc/s10052-019-6954-6 doi (DE-627)SPR008381186 (SPR)s10052-019-6954-6-e DE-627 ger DE-627 rakwb eng 530 ASE 33.50 bkl Martynov, Evgenij verfasserin aut Odderon effects in the differential cross-sections at Tevatron and LHC energies 2019 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier 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 %${\bar{p}}p%$ and pp differential cross-sections is diminishing with increasing energies and for very high energies (say 100 TeV), the difference between %${\bar{p}}p%$ and pp in the dip-bump region is changing its sign: pp becomes bigger than %${\bar{p}}p%$ at \|t\| about 1 GeV%$^2%$. 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 %${\bar{p}}p%$ scattering. This is also a clear Odderon effect. Nicolescu, Basarab verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 79(2019), 6 vom: 30. Mai (DE-627)253722934 (DE-600)1459069-4 1434-6052 nnns volume:79 year:2019 number:6 day:30 month:05 https://dx.doi.org/10.1140/epjc/s10052-019-6954-6 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2031 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2119 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 33.50 ASE AR 79 2019 6 30 05
allfieldsSound	10.1140/epjc/s10052-019-6954-6 doi (DE-627)SPR008381186 (SPR)s10052-019-6954-6-e DE-627 ger DE-627 rakwb eng 530 ASE 33.50 bkl Martynov, Evgenij verfasserin aut Odderon effects in the differential cross-sections at Tevatron and LHC energies 2019 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier 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 %${\bar{p}}p%$ and pp differential cross-sections is diminishing with increasing energies and for very high energies (say 100 TeV), the difference between %${\bar{p}}p%$ and pp in the dip-bump region is changing its sign: pp becomes bigger than %${\bar{p}}p%$ at \|t\| about 1 GeV%$^2%$. 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 %${\bar{p}}p%$ scattering. This is also a clear Odderon effect. Nicolescu, Basarab verfasserin aut Enthalten in The European physical journal Berlin : Springer, 1998 79(2019), 6 vom: 30. Mai (DE-627)253722934 (DE-600)1459069-4 1434-6052 nnns volume:79 year:2019 number:6 day:30 month:05 https://dx.doi.org/10.1140/epjc/s10052-019-6954-6 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2031 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2119 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 33.50 ASE AR 79 2019 6 30 05
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author	Martynov, Evgenij
spellingShingle	Martynov, Evgenij ddc 530 bkl 33.50 Odderon effects in the differential cross-sections at Tevatron and LHC energies
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topic_title	530 ASE 33.50 bkl Odderon effects in the differential cross-sections at Tevatron and LHC energies
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title	Odderon effects in the differential cross-sections at Tevatron and LHC energies
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title_full	Odderon effects in the differential cross-sections at Tevatron and LHC energies
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title_sort	odderon effects in the differential cross-sections at tevatron and lhc energies
title_auth	Odderon effects in the differential cross-sections at Tevatron and LHC energies
abstract	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 %${\bar{p}}p%$ and pp differential cross-sections is diminishing with increasing energies and for very high energies (say 100 TeV), the difference between %${\bar{p}}p%$ and pp in the dip-bump region is changing its sign: pp becomes bigger than %${\bar{p}}p%$ at \|t\| about 1 GeV%$^2%$. 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 %${\bar{p}}p%$ scattering. This is also a clear Odderon effect.
abstractGer	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 %${\bar{p}}p%$ and pp differential cross-sections is diminishing with increasing energies and for very high energies (say 100 TeV), the difference between %${\bar{p}}p%$ and pp in the dip-bump region is changing its sign: pp becomes bigger than %${\bar{p}}p%$ at \|t\| about 1 GeV%$^2%$. 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 %${\bar{p}}p%$ scattering. This is also a clear Odderon effect.
abstract_unstemmed	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 %${\bar{p}}p%$ and pp differential cross-sections is diminishing with increasing energies and for very high energies (say 100 TeV), the difference between %${\bar{p}}p%$ and pp in the dip-bump region is changing its sign: pp becomes bigger than %${\bar{p}}p%$ at \|t\| about 1 GeV%$^2%$. 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 %${\bar{p}}p%$ scattering. This is also a clear Odderon effect.
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title_short	Odderon effects in the differential cross-sections at Tevatron and LHC energies
url	https://dx.doi.org/10.1140/epjc/s10052-019-6954-6
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up_date	2024-07-03T20:34:26.744Z
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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 %${\bar{p}}p%$ and pp differential cross-sections is diminishing with increasing energies and for very high energies (say 100 TeV), the difference between %${\bar{p}}p%$ and pp in the dip-bump region is changing its sign: pp becomes bigger than %${\bar{p}}p%$ at \|t\| about 1 GeV%$^2%$. 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 %${\bar{p}}p%$ scattering. This is also a clear Odderon effect.</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Nicolescu, Basarab</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">The European physical journal</subfield><subfield code="d">Berlin : Springer, 1998</subfield><subfield code="g">79(2019), 6 vom: 30. 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Odderon effects in the differential cross-sections at Tevatron and LHC energies

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