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NSTAR 2001 Proceedings of the Workshop on The Physics of Excited Nucleons pot

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  • Organization

  • Foreword

  • CONTENTS

  • Nucleon Resonances in the Quark Model

    • 1 Introduction

    • 2 Effective Degrees of Freedom

    • 3 Confining Interaction

    • 4 Residual Interactions

    • 5 Lattice Results

    • 6 Hybrid Baryons

    • 7 Effects of Decay Channel Couplings

    • 8 Describing Reactions Using the Quark Model

    • 9 Summary

    • Acknowledgments

    • References

  • Quadrupole Strength in the N -> A Transition

    • 1 Introduction

    • 2 Theoretical Developments

    • 3 The Bates y* N -> A Program

    • 4 Future Prospects and Acknowledgments

    • References

  • Pion Electroproduction at ELSA

    • 1 Introduction

    • 2 Neutron Identification

    • 3 First Results

    • References

  • TT0 Electroproduction in the A(1232) Region at MAMI

    • 1 Introduction

    • 2 Results of the p(e e'p)TT0 Experiment

    • 3 Forward and Backward LT-Asymmetry in p(e e'p)TT0

    • 4 Fifth Structure Function in p(e e'p)TT0

    • 5 Summary

    • Acknowledgements

    • References

  • Pion Electroproduction Using CLAS

    • 1 Introduction

    • References

  • Recoil Polarization Measurements in TT0 Electroproduction at the Peak of the A(1232)

    • 1 Introduction

    • 2 Measurement Philosophy: Exploiting Hall A's Tools

    • 3 Specific Measurements for E91-011

    • 4 Accessible Responses and Expected Sensitivity to S1+.

    • 5 Data Analysis - Sample Spectra

    • 6 Conclusions/Outlook

    • Acknowledgments

    • References

  • Chiral Effective Field Theories with Explicit Spin 3/2 Degrees of Freedom - A Status Report

    • 1 Introduction

    • 2 Chiral Calculations and Power Counting

    • 3 Anomalous Magnetic Moments of the Nucleon

    • 4 Isovector Form Factors of the Nucleon

    • 5 Isovector Nucleon-Delta Transition Form Factors

    • 6 Summary

    • Acknowledgments

    • References

  • Dynamical Meson-Baryon Resonances with Chiral Lagrangians

    • 1 Introduction

    • 2 Meson-Baryon Scattering in Coupled Channels

    • 3 Strangeness S = -1 Sector

    • 4 Strangeness S = 0 Sector

    • 5 Strangeness S = -2 Sector

    • 6 Conclusions

    • Acknowledgments

    • References

  • Chiral Lagrangians with Resonances

    • 1 Chiral Symmetry

    • 2 Elastic TTN Scattering and Unitarization

    • 3 Coupled Channel NK Scattering

    • 4 Conclusions

    • Acknowledgments

    • References

  • Pion Photo- and Electroproduction in Dynamical Model

    • 1 Introduction

    • 2 Effective Hamiltonian and Electromagnetic Current

    • 3 Pion Photoproduction and Electroproduction

    • 4 Summary

    • Acknowledgments

    • References

  • Recent Developments in the Dynamical and Unitary Isobar Models for Pion Electromagnetic Production

    • 1 Introduction

    • 2 Formalism

    • 3 Pion Photo- and Electroproduction in the A(1232) Region

    • 4 Threshold TT0 Photoproduction

    • 5 Threshold TT0 Electroproduction

    • 6 Conclusion

    • References

  • Two Pion Production in the Jiilich Model

    • 1 Introduction

    • 2 The Model

    • 3 Results

    • 4 Summary

    • Acknowledgments

    • References

  • Update on Partial-Wave Analysis

    • 1 Overview

    • 2 Near-Threshold Studies

    • 3 Fitting the Full Resonance Region

    • 4 Conclusions and Further Questions

    • Acknowledgments

    • References

  • Nucleon Resonance Properties in Multichannel Approaches

    • 1 Introduction

    • 2 Coupled-channels Analyses

    • 3 Results and Discussion

    • 4 Conclusions and Outlook

    • Acknowledgments

    • References

  • Variation of Hadron Structure with Quark Mass

    • 1 Introduction

    • 2 Electromagnetic Form Factors

    • 3 Structure Functions

    • Acknowledgments

    • References

  • The Role of the Pion in Nucleon Resonance Structure

    • 1 Pion Coupling to Constituent Quarks

    • 2 Model Calculations of Resonance Decay Widths

    • 3 Pion Decays of D-Mesons

    • 4 Conclusion

    • Acknowledgments

    • References

  • Relativistic Quark Models

    • 1 Introduction

    • 2 Relativistic Constituent Quark Models

    • 3 Nucleon Elastic Form Factors and the N - P11(1440) Transition

    • 4 Conclusions

    • References

  • Generalized Polarizabilities in a Constituent Quark Model

    • 1 Introduction

    • 2 Compton Tensor and Low-Energy Theorem

    • 3 Generalized Polarizabilities and their Interpretation

    • 4 Compton Tensor in a Nonrelativistic Framework

    • 5 Generalized Polarizabilities in a Constituent Quark Model

    • 6 Results

    • 7 Summary

    • Acknowledgments

    • References

  • Nucleon Properties in the Perturbative Chiral Quark Model

    • 1 Introduction

    • 2 Perturbative Chiral Quark Model

    • 3 Results

    • Acknowledgments

    • References

  • The Glasgow Pion Photoproduction Partial Wave Analysis 2001

    • 1 Introduction

    • 2 The Analysis

    • 3 Results

    • 4 Conclusions

    • References

  • Residues of the Multipole Amplitudes M3/2 1+ E3/2 1+ at the t-Matrix Pole Found in the Framework of Dispersion Relations

    • 1 Introduction

    • 2 Reducing of Dispersion Relations for M3/2 1+ E3/2 1+ to Integral Equations and the Solution of these Equations

    • References

  • An Isobar Model for n Photo- and Electroproduction on the Nucleon

    • 1 Introduction

    • 2 Isobar Model

    • 3 Results and Discussion

    • Acknowledgments

    • References

  • Detailed Analysis of n Production in Proton-Proton Collisions

    • References

  • Phenomenological Analysis of N* Excitation in Charged Double Pion Production

    • 1 Introduction

    • 2 Model Description

    • 3 Real Photon

    • 4 Virtual Photons

    • References

  • Results on A(1232) Resonance Parameters: A New TTN Partial Wave Analysis

    • 1 Determination of Resonance Parameters from Speed Plots

    • 2 The Background in the P33 Partial Wave

    • 3 An Updated Version of the KH80 Partial Wave Analysis

    • Acknowledgments

    • References

  • Solving the Puzzle of the yp -> TT+TT0n Reaction

    • 1 Introduction

    • 2 Formalism

    • 3 Discussion and Results

    • 4 Summary

    • References

  • The Giessen Model - Vector Meson Production on the Nucleon in a Coupled Channel Approach

    • 1 Introduction

    • 2 The Model

    • 3 Results on (Pseudo)scalar Meson Production

    • 4 Vector Meson Production

    • 5 Outlook

    • 6 Acknowledgments

    • References

  • Multipole Analysis for Pion Photoproduction with MAID and a Dynamical Model

    • References

  • Model Dependence of E2/M1

    • 1 Introduction

    • 2 The Participants and their Models

    • 3 Results

    • Acknowledgments

    • References

  • Eta Photoproduction in a Coupled-Channels Approach

    • 1 Introduction

    • 2 Low-Energy Region: S11(1535) and D13(1520)

    • 3 Intermediate-Energy Region: S11(1650) and D13(1700)

    • Acknowledgments

    • References

  • Electroweak Properties of Baryons in a Covariant Chiral Quark Model

    • References

  • Low Lying qqqqq States in the Baryon Spectrum

    • 1 Introduction

    • 2 The qqqqq System

    • 3 Summary

    • References

  • Parity Doublets from a Relativistic Quark Model

    • References

  • A Dispersion Theoretical Approach to Virtual Compton Scattering off the Proton

    • References

  • Neutron Charge Form Factor and Quadrupole Deformation of the Nucleon

    • References

  • The Ground and Radial Excited States of the Nucleon in a Relativistic Schodinger-Type Model

    • References

  • Vector Meson Photoproduction in the Quark Model

    • 1 Introduction

    • 2 Analysis

    • Acknowledgments

    • References

  • Status of Nucleon Resonances with Masses M < MN + MTT

    • References

  • Spin Structure of the A(1232) and Inelastic Compton Scattering

    • 1 Introduction: The GDH Sum Rule for the A(1232)

    • 2 Photocouplings in NQM: The Role of Spin-Orbit Corrections

    • 3 Differential Cross Section of yN -> yA

    • References

  • Structure of the Roper Resonance from a-Proton and TT-Nucleon Scattering

    • 1 Introduction

    • 2 T-Matrix Description of TT-N and a-p Scattering

    • 3 Comparison with y-N

    • References

  • Structure of the Nucleon Investigated by Compton Scattering

    • References

  • Virtual Compton Scattering at Jefferson Lab: Preliminary Results in the Polarizability Domain at Q2 = 1 and 1.9 GeV2

    • 1 Virtual Compton Scattering

    • 2 Virtual Compton Scattering at Jefferson Laboratory.

    • 3 Preliminary Results for Cross Sections

    • References

  • Measurement of the Cross Section Asymmetry E for yp -> TT0p over the Range Ey = 0.5 - 1.1 GeV

    • 1 Introduction

    • 2 Experiment and Data Analysis

    • 3 Results and Discussion

    • Acknowledgments

    • References

  • Positive Pion Photoproduction and Compton Scattering at GRAAL

    • References

  • Virtual Compton Scattering and Pion Electroproduction in the Nucleon Resonance Region

    • 1 Introduction

    • 2 Experimental Considerations

    • 3 Pion Electroproduction

    • 4 Virtual Compton Scattering (VCS)

    • 5 Conclusion

    • References

  • Single Spin Beam Asymmetry Measurements from Single TT0 Electroproduction in the A(1232) Resonance Region

    • 1 Introduction

    • 2 Data Analysis and Results

    • References

  • The New Crystal Ball Experimental Program

    • 1 Introduction

    • 2 Experimental Considerations

    • 3 Results

    • 4 Acknowledgments

  • Observation of n-Mesic Nuclei in Photoreactions: Results and Perspectives

    • Acknowledgment

    • References

  • Baryon Spectroscopy: Experiments at PNPI

    • 1 Study of TT-p Charge Exchange Scattering in the Region of Low-Lying Pion-Nucleon Resonances

    • 2 Measurement of the Spin Rotation Parameters for TT+p Elastic Scattering in the Second Resonance Region

    • References

  • Measurement of the Cross Section Asymmetry in Deuteron Photodisintegration by Linearly Polarized Photons in the Energy Range Er = 0.8 - 1.6 GeV

    • 1 Introduction

    • 2 Experimental Setup

    • 3 Results and Summary

    • References

  • Nucleon Resonances in Lattice QCD

    • 1 Introduction

    • 2 Method

    • 3 Results and Discussion

    • 4 Conclusion

    • 5 Acknowledgment

    • References

  • Lattice Study of Nucleon Properties with Domain Wall Fermions

    • 1 Introduction

    • 2 Nucleon Excited States

    • 3 Nucleon Matrix Elements

    • 4 Conclusions

    • Acknowledgments

    • References

  • Quark-Hadron Duality: Resonances and the Onset of Scaling

    • 1 Introduction

    • 2 Bloom-Gilman Duality

    • 3 Understanding the Origin of Duality

    • 4 Applications of Local Duality

    • 5 Conclusion

    • References

  • Generalized GDH Sum Rule and Spin-Dependent Electroproduction in the Resonance Region

    • 1 Introduction

    • 2 Generalized GDH Sum Rules

    • 3 JLab E94-010 Experiment

    • 4 GDH with Nearly Real Photons: JLab E97-110

    • 5 Outlook and Summary

    • Acknowledgments

    • References

  • Double Polarization Measurements Using the CLAS at JLab

    • 1 Motivation and Theoretical Description

    • 2 Description of the Experiment

    • 3 Data Analysis and Results

    • Acknowledgments

    • References

  • The Helicity Dependent Excitation Spectrum of the Nucleon and the GDH Sum Rule

    • 1 Experimental Setup

    • 2 Results

    • Acknowledgments

    • References

  • Static Magnetic Moment of the A(1232)

    • 1 Introduction

    • 2 Experimental Setup and Analysis Methods

    • 3 Preliminary Results and Conclusion

    • Acknowledgments

    • References

  • Meson Photoproduction at GRAAL

    • 1 Introduction

    • 2 The Graal Experimental Set-up

    • 3 n Photoproduction

    • 4 TT0 Photoproduction

    • 5 K+ A Photoproduction

    • 6 Acknowledgments

    • References

  • Maximum Likelihood Techniques for PWA of 2-Pion Photoproduction

    • 1 Introduction

    • 2 Analysis Technique

    • 3 Preliminary Tests

    • 4 Conclusion

    • References

  • n Electroproduction with CLAS

    • 1 Introduction

    • 2 Results from First Data Run

    • 3 Prospects and Conclusions

    • 4 Acknowledgements

    • References

  • Kaon Electroproduction and A Polarization Observables Measured with CLAS

    • 1 Introduction

    • 2 Formalism and Kinematics

    • 3 The CLAS Program

    • 4 Results

    • 5 Summary

    • Acknowledgments

    • References

  • Recent Results on Kaon Photoproduction at SAPHIR in the Reactions rp -> K+A and rp ->K+ E0

    • 1 Introduction

    • 2 Cross Sections

    • References

  • Vector Meson Decay of Baryon Resonances

    • 1 Introduction

    • 2 VMD Analysis of the Electromagnetic Resonance Decay

    • 3 The p Meson

    • 4 The w Meson

    • 5 Conclusions

    • 6 Acknowledgments

    • References

  • Higher and Missing Resonances in w Photoproduction

    • Acknowledgments

    • References

  • Photoproduction of Baryon Resonances First Data from the CB-ELSA Experiment

    • 1 Introduction

    • 2 The CB-ELSA Detector

    • 3 First Data

    • 4 Conclusions

    • References

  • Laser-Electron Photon Project at SPring-8

    • 1 Physics Motivation

    • 2 LEPS Facility

    • 3 Detector

    • 4 Results and Prospects

    • References

  • The Baryon Resonance Program at BES

    • 1 Physics motivation

    • 2 Data Status

    • 3 Partial Wave Analyses

    • 4 Future Prospects

    • Acknowledgments

    • References

  • Flavor Symmetry Studies with New Hyperon Data from the Crystal Ball

    • 1 Introduction

    • 2 k-p -> nA

    • 3 TT-p -> TT0TT0n K-p -> TT0TT0A and K-p -> TT0TT0E0

    • 4 Flavor Symmetry and the Masses of the Hyperons

    • 5 Flavor Symmetry and the Search for the Missing Baryon Resonances

    • 6 Summary and Conclusion

    • References

  • Higher Resonances and the Example of Two Pion Electroproduction with the CLAS Detector at Jefferson Lab

    • 1 Physics Issues

    • 2 Kinematics and Observables

    • 3 Theoretical Aspects

    • 4 Data Collection with CLAS

    • 5 Preliminary Data Cross Sections and Physical Analysis

    • 6 Summary and Conclusions

    • References

  • Nucleon Resonances and Mesons in Nuclei

    • 1 Introduction

    • 2 Photoabsorption on Free and Bound Nucleons

    • 3 Properties of Bound Nucleon Resonances

    • 4 Scalar Mesons in the Nuclear Medium

    • 5 Summary

    • References

  • Excitation of Nucleon Resonances

    • 1 Introduction

    • 2 The yNA(1232) Transition - From Precision Experiments to Precision Calculations.

    • 3 The 2nd Resonance Region

    • 4 Missing Baryon Resonances

    • 5 The Nucleon Spin Integral from Small to Large Distances - A Proposal for the Next 5 Years

    • Closing Remarks

    • In Memoriam

    • References

  • Multipole Analysis of a Benchmark Data Set for Pion Photoproduction

    • 1 Overview

    • 2 Multipole Analysis with MAID and a Dynamical Model

    • 3 Multipole Analysis of Pion Photoproduction with Constraints from Fixed-t Dispersion Relations and Unitarity

    • 4 Analysis of Low-Energy Benchmark Data Using Fixed-t Dispersion Relations

    • 5 The Effective Lagrangian Analysis of the Benchmark Dataset

    • 6 Multipole Analysis of the Benchmark Set Covering the First Resonance Region

    • 7 SAID Multipole Analysis of the Benchmark Dataset

    • 8 Conclusions and Future Projects

    • References

  • Appendix

    • Author Index

    • Program of the Workshop

    • List of Participants

Nội dung

NSTAR 2001 Proceedings of the Workshop on . The Physics of Excited Nucleons ^S^*?ft D. Drechsel & L. Tiator World Scientific NSTAR 2001 Proceedings of the Workshop on The Physics of Excited Nucleons [...]... the data 9 Summary The study of nucleon resonances using quark models is more than simply stamp collecting: we are exploring the consequences of QCD for the spectrum and decay of baryons; identifying the important degrees of freedom for the description of the majority of hadrons; and discovering the nature of the properties and interactions of those degrees of freedom Progress hinges on the solution... most of the deformation can be attributed to the asymmetric coupling of the meson cloud to the spin of the nucleon In the spherical quark model of the nucleon, the N — A excitation is a • pure M l {Mx'+ ) transition The resonant quadrupole multipoles E2 {Ex'+ ) and C2 {S1+ ) contain the pertinent information It has become standard practice to quote experimental and theoretical results in terms of the. .. understand the structure of hadrons and the intricate dynamics of their constituents It is the subject of investigations at every medium energy electron accelerator A brief overview of the field is presented, followed by a presentation of the Bates N—>A program 1 Introduction The possibility of nucleon deformation raised more than 20 years ago 1 still remains an open one The presence of resonant quadrupole... model consistent with a chiral model of the nucleon Deficiencies of the models that emerge as a result of the comparison with the data are rectified by re-adjustments of the parameters and/or by modifying the phenomenology This results in an improved understanding 14 of the underlying physics and gradual reduction of the model error For the H(e, e'p)7 channel the new dispersion theory 16 of the Mainz... that the A3/2"(1520) - Al/2~(1405) splitting may also have the same source 6 Hybrid Baryons Identification of hybrid baryons is complicated by the fact that they have the same quantum numbers as conventional three-quark excitations, and so should mix with conventional excitations Their identification is also some- 6 what model dependent, as it relies on the separation of the gluon and quark degrees of. .. theory 16 of the Mainz group, taken in conjunction with the previous work of Vanderhaeghen et al 17 allows to addresses the physics of "deformation" and of nucleon polarizabilities in the region above pion threshold simultaneously Of particular importance to the field is the prediction of the Dynamical Model 18,19 and of Sato and Lee 14 that most of the responses and the REM and RSM exhibit a distinct structure... determination » of the cross section in "parallel kinematics" a0, of the LT-asymmetry, ALT, and response RLT and the measurement of the induced proton polarization Pn Pn is proportional to the R^T response and it would be identically zero in the absence of background It was found 12 to be -0.397 ± 0.055 ± 0.009 which established the importance of the background contributions The coincident cross section in... based on a spectrum-generating algebra 4 describes excited states in terms of collective excitations of string-like objects which carry the quark quantum numbers, with radial excitations arising from rotations and vibrations of these strings As the degrees of freedom are extended, there are more excited states, some of which would be described in other models as excitations of the confining glue The constituent... lighter of the two Su states at 1535 MeV and the small Nr] width for the heavier state at 1650 MeV, which can be explained as due to mixing between the quark-spin-1/2 and 3/2 states caused by the tensor interaction of the strength implied by the contact interaction 10 Although there are also spin-orbit interactions arising from the Thomas precession of the quarks in the confining potential, and there... cancellation of these with the OGE spin-orbit interactions, the spin-orbit interactions which accompany the contact and tensor interactions in the nonrelativistic model cause splittings which are unphysically large A variational calculation in a large basis allows the use of a relativistic kinetic energy and parametrized relativistic corrections to the potentials of the kind expected from examining the OGE . Proceedings of the Workshop on The Physics of Excited Nucleons

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