Nucleon Resonance Electroexcitation Amplitudes and Emergent Hadron Mass
Understanding the strong interaction dynamics that govern the emergence of hadron mass (EHM) represents a challenging open problem in the Standard Model. In this paper we describe new opportunities for gaining insight into EHM from results on nucleon resonance ($N^\ast$) electroexcitation amplitudes...
Gespeichert in:
Hauptverfasser: | , , , |
---|---|
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext bestellen |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
Zusammenfassung: | Understanding the strong interaction dynamics that govern the emergence of
hadron mass (EHM) represents a challenging open problem in the Standard Model.
In this paper we describe new opportunities for gaining insight into EHM from
results on nucleon resonance ($N^\ast$) electroexcitation amplitudes (i.e.
$\gamma_vpN^\ast$ electrocouplings) in the mass range up to 1.8\,GeV for
virtual photon four-momentum squared (i.e. photon virtualities $Q^2$) up to
7.5\,GeV$^2$ available from exclusive meson electroproduction data acquired
during the 6-GeV era of experiments at Jefferson Laboratory (JLab). These
results, combined with achievements in the use of continuum Schwinger function
methods (CSMs), offer new opportunities for charting the momentum dependence of
the dressed quark mass from results on the $Q^2$-evolution of the
$\gamma_vpN^\ast$ electrocouplings. A successful description of the
$\Delta(1232)3/2^+$ and $N(1440)1/2^+$ electrocouplings has been achieved using
CSMs with, in both cases, common momentum-dependent mass functions for the
dressed quarks, for the gluons, and the same momentum-dependent strong
coupling. Parameter-free CSM predictions for the electrocouplings of the
$\Delta(1600)3/2^+$ became available in 2019. The experimental results obtained
in the first half of 2022 have confirmed the CSM predictions. We also discuss
prospects for these studies during the 12-GeV era at JLab using the CLAS12
detector, with experiments that are currently in progress, and canvass the
physics motivation for continued studies in this area with a possible increase
of the JLab electron beam energy up to 22\,GeV. |
---|---|
DOI: | 10.48550/arxiv.2301.07777 |