Observation of two zeros of the real amplitude in pp scattering at LHC energies

Abstract Elastic scattering of charged hadrons is described by the combination of nuclear and Coulomb amplitudes. It is well know that at the very forward range the nuclear real and Coulomb parts interplay a crucial role in the determination of the magnitude of the real part at $$|t|=0$$ | t | = 0 ....

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Main Author: Anderson Kendi Kohara
Format: Article
Language:English
Published: SpringerOpen 2023-02-01
Series:European Physical Journal C: Particles and Fields
Online Access:https://doi.org/10.1140/epjc/s10052-023-11286-4
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author Anderson Kendi Kohara
author_facet Anderson Kendi Kohara
author_sort Anderson Kendi Kohara
collection DOAJ
description Abstract Elastic scattering of charged hadrons is described by the combination of nuclear and Coulomb amplitudes. It is well know that at the very forward range the nuclear real and Coulomb parts interplay a crucial role in the determination of the magnitude of the real part at $$|t|=0$$ | t | = 0 . However, beyond $$|t|=0$$ | t | = 0 the real and imaginary nuclear amplitudes have different t dependencies and we show that at LHC energies the zeros formed by the combination $$T_C(t)+T_R^N(s,t)=0$$ T C ( t ) + T R N ( s , t ) = 0 in pp process can be potentially observed when the background due to the imaginary part is removed. This observation constrains the real part at this forward range.
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spelling doaj.art-16fc7fd1648b4d9fb7fca2297d6db9fa2023-04-03T05:37:35ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60522023-02-018321410.1140/epjc/s10052-023-11286-4Observation of two zeros of the real amplitude in pp scattering at LHC energiesAnderson Kendi Kohara0Faculty of Physics and Applied Computer Science, AGH University of Science and TechnologyAbstract Elastic scattering of charged hadrons is described by the combination of nuclear and Coulomb amplitudes. It is well know that at the very forward range the nuclear real and Coulomb parts interplay a crucial role in the determination of the magnitude of the real part at $$|t|=0$$ | t | = 0 . However, beyond $$|t|=0$$ | t | = 0 the real and imaginary nuclear amplitudes have different t dependencies and we show that at LHC energies the zeros formed by the combination $$T_C(t)+T_R^N(s,t)=0$$ T C ( t ) + T R N ( s , t ) = 0 in pp process can be potentially observed when the background due to the imaginary part is removed. This observation constrains the real part at this forward range.https://doi.org/10.1140/epjc/s10052-023-11286-4
spellingShingle Anderson Kendi Kohara
Observation of two zeros of the real amplitude in pp scattering at LHC energies
European Physical Journal C: Particles and Fields
title Observation of two zeros of the real amplitude in pp scattering at LHC energies
title_full Observation of two zeros of the real amplitude in pp scattering at LHC energies
title_fullStr Observation of two zeros of the real amplitude in pp scattering at LHC energies
title_full_unstemmed Observation of two zeros of the real amplitude in pp scattering at LHC energies
title_short Observation of two zeros of the real amplitude in pp scattering at LHC energies
title_sort observation of two zeros of the real amplitude in pp scattering at lhc energies
url https://doi.org/10.1140/epjc/s10052-023-11286-4
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