8–13 Jun 2025
America/Winnipeg timezone
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Probing Hadron Structure through $e ~ + ~ p ~ \to ~ e^{'} ~ + ~ \pi^{+} ~ + ~ \Delta^{0}$ reaction at Jefferson Lab

10 Jun 2025, 11:45
15m
Oral not-in-competition (Graduate Student) / Orale non-compétitive (Étudiant(e) du 2e ou 3e cycle) Nuclear Physics / Physique nucléaire (DNP-DPN) (DNP) T1-6 Hadrons | Hadrons (DPN)

Speaker

Ali Usman

Description

The internal structure of hadrons is incompletely understood, as the intrinsic properties of hadrons (e.g. mass, spin) cannot yet be fully understood within a QCD framework. Generalized Parton Distributions (GPDs) provide information about the three dimensional structure of hadrons. The pion is a good candidate for hadron structure studies, due to its relatively simple structure and its experimental accessibility. Experimental Hall C at Jefferson Lab is a unique facility that can host high precision studies of exclusive pion electroproduction reactions. The cross-section of this reaction is dictated by the longitudinal and transverse polarizations of the virtual photon. Considering the recoil system in such a reaction, the ground state nucleon in the $p(e,e^{'} \pi^{+})n$ reaction has been studied in detail but little is known about the nucleon-to-resonance ($N \to \Delta$) transition reaction $p(e,e^{'} \pi^{+})\Delta^{0}$. This reaction provides access to the transition GPDs. The 12 GeV upgrade at Jefferson Lab provides a unique opportunity to study the higher resonance of pion electroproduction reaction $p(e,e^{'} \pi^{+})\Delta^{0}$ at wide range of kinematics ($Q^{2}, ~ W$ and $-t$). This talk will present the first measurement of the beam spin asymmetry and cross-section ratio ($\sigma_{LT^{'}}/\sigma_{0}$) from the Kaon-LT Experiment. These are compared with the ground state reaction. The comparison of two reactions will be invaluable for our understanding of hadron GPDs.

Keyword-1 Hadron Structure
Keyword-2 QCD

Author

Ali Usman

Presentation materials

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