Abstract

In this contribution we discuss recent results in light quark baryon spectroscopy involving CLAS data and higher level analysis results from the partial wave analysis by the Bonn-Gatchina group. New baryon states were discovered largely based on the open strangeness production channels $\gamma p \to K^+ \Lambda$ and $\gamma p \to K^+ \Sigma^0$. The data illustrate the great potential of the kaon-hyperon channel in the discovery of higher mass baryon resonances in s-channel production. Other channels with discovery potential, such as $\gamma p \to p \omega$ and $\gamma p \to \phi p$ are also discussed. In the second part I will demonstrate on data the sensitivity of meson electroproduction to expose the active degrees of freedom underlying resonance transitions as a function of the probed distance scale. For several of the prominent excited states in the lower mass range the short distance behavior is described by a core of three dressed-quarks with running quark mass, and meson-baryon contributions make up significant parts of the excitation strength at large distances. Finally, an outlook is given of baryon resonance physics at the 12 GeV CEBAF electron accelerator.

Highlights

  • Dramatic events occurred in the evolution of the microsecond old universe that had tremendous implication for the further development of the universe to the state it is in today

  • The energy available at the CEBAF electron accelerator as well as at ELSA and MAMI are well matched to study the details of this transition in searching for "missing" baryon states and in probing the momentum-dependent light-quark mass in the Q-dependence of the resonance transition amplitudes

  • The N∗ program pursued by the CLAS collaboration has made very significant contributions towards improving our understanding of strong QCD by charting the kinematic landscape of the excited light-quark baryon states, which led to revealing of many new excited states

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Summary

Introduction

Dramatic events occurred in the evolution of the microsecond old universe that had tremendous implication for the further development of the universe to the state it is in today. Of ≈ 1 fm, i.e. protons, neutrons, and other baryons In course of this process, elementary, nearly massless quarks acquire dynamical mass due to the coupling to the dressed gluons, and the fact that chiral symmetry is broken dynamically [1]. This transition is not a simple first order phase transition, but a "cross over" between two phases. The presence of the full complement of excited baryons, the acquisition of dynamical mass by light quarks, and the transition from unconfined quarks to confinement are intricately related and are at the core of the problems we are trying to solve in hadron physics today. We do have all the tools at our disposal to study the individual excited states in relative isolation, and to probe the quark mass versus the momentum or distance scale, and to search for so far undiscovered baryon states

Establishing the light quark baryon spectrum
Hyperon photoproduction
Vector meson photoproduction
Electroexcitation of light-quark baryon resonances
Solving the Roper puzzle
Light-cone charge transition densities
Summary & Outlook
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