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Baryons as relativistic three-quark bound states

5 Pith papers cite this work. Polarity classification is still indexing.

5 Pith papers citing it
abstract

We review the spectrum and electromagnetic properties of baryons described as relativistic three-quark bound states within QCD. The composite nature of baryons results in a rich excitation spectrum, whilst leading to highly non-trivial structural properties explored by the coupling to external (electromagnetic and other) currents. Both present many unsolved problems despite decades of experimental and theoretical research. We discuss the progress in these fields from a theoretical perspective, focusing on nonperturbative QCD as encoded in the functional approach via Dyson-Schwinger and Bethe-Salpeter equations. We give a systematic overview as to how results are obtained in this framework and explain technical connections to lattice QCD. We also discuss the mutual relations to the quark model, which still serves as a reference to distinguish 'expected' from 'unexpected' physics. We confront recent results on the spectrum of non-strange and strange baryons, their form factors and the issues of two-photon processes and Compton scattering determined in the Dyson-Schwinger framework with those of lattice QCD and the available experimental data. The general aim is to identify the underlying physical mechanisms behind the plethora of observable phenomena in terms of the underlying quark and gluon degrees of freedom.

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hep-ph 5

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UNVERDICTED 5

representative citing papers

All-loop four-quark Bethe-Salpeter kernel

hep-ph · 2026-05-06 · unverdicted · novelty 7.0

The all-loop bare perturbative part of the four-quark Bethe-Salpeter kernel is computed analytically in the large-Nf limit of massless QCD.

Effects of Final State Interactions on Landau Singularities

hep-ph · 2024-07-25 · unverdicted · novelty 5.0

Triangle singularities mimicking resonances are analyzed in the presence of final-state rescattering using Landau equations and a scattering formalism enforcing two- and three-body unitarity.

Light-front mass operator with dressed quarks

hep-ph · 2026-04-24 · unverdicted · novelty 5.0

An effective dressed light-front mass operator for quarks is constructed from a lattice-inspired propagator and applied to compute pion TMDs, PDFs, and distribution amplitudes.

Lepton anomalous magnetic moments: Theory

hep-ph · 2025-12-20 · unverdicted · novelty 2.0

The paper provides an overview of theoretical calculations for lepton anomalous magnetic moments arising from quantum corrections in the Standard Model.

citing papers explorer

Showing 5 of 5 citing papers.

  • All-loop four-quark Bethe-Salpeter kernel hep-ph · 2026-05-06 · unverdicted · none · ref 76

    The all-loop bare perturbative part of the four-quark Bethe-Salpeter kernel is computed analytically in the large-Nf limit of massless QCD.

  • Chiral symmetry restoration effects onto the meson spectrum from a Dyson-Schwinger and Bethe-Salpeter approach hep-ph · 2026-02-19 · unverdicted · none · ref 8 · internal anchor

    Varying interaction strength in DSE/BSE models produces meson degeneracies whose domains shrink with model realism, linked to quark propagator pole locations and possible chiral spin symmetry.

  • Effects of Final State Interactions on Landau Singularities hep-ph · 2024-07-25 · unverdicted · none · ref 14 · internal anchor

    Triangle singularities mimicking resonances are analyzed in the presence of final-state rescattering using Landau equations and a scattering formalism enforcing two- and three-body unitarity.

  • Light-front mass operator with dressed quarks hep-ph · 2026-04-24 · unverdicted · none · ref 1

    An effective dressed light-front mass operator for quarks is constructed from a lattice-inspired propagator and applied to compute pion TMDs, PDFs, and distribution amplitudes.

  • Lepton anomalous magnetic moments: Theory hep-ph · 2025-12-20 · unverdicted · none · ref 272 · internal anchor

    The paper provides an overview of theoretical calculations for lepton anomalous magnetic moments arising from quantum corrections in the Standard Model.