| Foreword | 5 |
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| Contents | 7 |
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| List of Participants | 10 |
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| Sponsors | 15 |
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| I Introductory talks | 16 |
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| Today's view on strangeness | 17 |
| Strange and gluonic contributions to the nucleon spin | 25 |
| II Form factors and two- photon effects | 29 |
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| Electromagnetic form factors of the nucleon | 30 |
| Two photon effects in electron scattering | 35 |
| Single spin asymmetries in elastic electron- nucleon scattering | 40 |
| Transverse single spin asymmetry in elastic electron- proton scattering | 44 |
| Transverse spin asymmetry at the A4 experiment | 46 |
| Normal beam spin asymmetries during the G° forward angle measurement | 50 |
| Ill Weak form factors of the nucleon | 52 |
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| III- 1 PV experiment | 52 |
| The axial form factor of the nucleon | 53 |
| Parity violating electron scattering at the MAM I facility in Mainz | 57 |
| Updated results from the SAMPLE experiment | 61 |
| The next generation HAPPEX experiments | 65 |
| The GO experiment: Parity violation in e- N elastic scattering | 69 |
| Study of the parity violation in the ^( 1232) region | 74 |
| Don't forget to measure As | 75 |
| III- 2 Theory | 79 |
| Getting to grips with hadrons | 80 |
| Systematic uncertainties in the precise determination of the strangeness magnetic moment of the nucleon | 86 |
| Current status of parton charge symmetry | 92 |
| Pion- nucleon interaction and the strangeness content of the nucleon | 96 |
| Strange form factors of the nucleon in the chiral quark- soliton model | 100 |
| Strange form factors and Chiral Perturbation Theory | 104 |
| Time- like compton scattering and the Bethe- Heitler process | 108 |
| Corrections to the nuclear axial vector coupling in a nuclear medium | 110 |
| Strangeness- conserving effective weak chiral Lagrangian | 111 |
| IV Experimental techniques in PV electron scattering | 112 |
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| IV-1 Beam asymmetry | 112 |
| Overview of laser systematics | 113 |
| Beam optics for electron scattering parity- violation experiments | 119 |
| GO beam quality and multiple linear regression corrections | 123 |
| IV-2 Polarimetry | 125 |
| M0ller polarimetry with atomic hydrogen targets | 126 |
| Progress report on the A4 Compton backscattering polarimeter | 130 |
| The transmission Compton polarimeter of the A4 experiment | 132 |
| Stabilization system of the laser system of the A4 Compton backscattering polarimeter | 134 |
| Electron beam line design of A4 Compton backscattering polarimeter | 135 |
| IV-3 Detection | 136 |
| Background substraction in parity violation experiments | 137 |
| Redesign of the A4 calorimeter for the measurement at backward angles | 141 |
| Performance of the G° superconducting magnet system | 142 |
| Cherenkov counter for the G° backward angle measurements | 143 |
| A bin- per- bin dead- time control technique for time- of- flight measurements in the G° experiment: The differential buddy | 144 |
| V Hadronic structure... and more | 145 |
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| V- 1 Test of the SM at low energy | 145 |
| A precise measurement of sin2Ow at low Q2 in M0ller scattering | 146 |
| Qweak: A precision measurement of the proton's weak charge | 150 |
| The Qweak tracking system | 154 |
| Neutral currents and strangeness of the nucleon from the NuTeV experiment | 156 |
| V-2 PV in nuclear systems | 160 |
| Parity violation in astrophysics | 161 |
| Parity violation in nuclear systems | 165 |
| Parity violation in nuclear systems | 169 |
| Parity violating asymmetry in y + d - n + p at low energy | 173 |
| \/-3 Neutrino beam | 175 |
| Precision physics at a neutrino factory | 176 |
| The MINERvA experiment at FNAL | 180 |
| VI Concluding talks | 181 |
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| Frontiers of polarized electron scattering experiments | 182 |
| Parity- violation with electrons: Theoretical perspectives | 187 |
| Workshop summary | 195 |
