Published December 17, 2003 | Version v1
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Contributions to the G0 experiment on parity violation: calculation and simulation of radiative corrections and background study

Description

In the framework of quantum chromodynamics, the nucleon is made of three valence quarks surrounded by a sea of gluons and quark-antiquark pairs. Only the only lightest quarks (u,d, and s) contribute significantly to the nucleon properties. In the G0 experiment we use the property of weak interaction to violate parity symmetry, in order to determine separately the contributions of the three types of quarks to nucleon form factors.The experiment, which takes place at Thomas Jefferson Laboratory (USA) aims at measuring parity violation asymmetry in electron-proton scattering. By doing several measurements at different momentum squared of the exchanged photons and for different kinematics will permit to determine separately strange quarks electric and magnetic contributions to nucleon form factors. To extract an asymmetry with small errors it is necessary to correct all the beam parameters and to have high enough counting rates in detectors. A special electronics was developed to treat information coming from 16 scintillator pairs for each of the 8 sectors of the G0 spectrometer. A complete calculation of radiative corrections has been done and Monte Carlo simulations with the GEANT program has permitted to determine the shape of the experimental spectra including inelastic background. This work will allow to do a comparison between experimental data and theoretical calculations based on the standard model. (author)

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Additional details

Additional titles

Original title (French)
Contribution a l'experience G0 de violation de la parite: calcul et simulation des corrections radiatives et etude du bruit de fond

Publishing Information

Imprint Pagination
185 p.
Report number
FRNC-TH--14531

Optional Information

Notes
66 refs.; Available from the INIS Liaison Officer for France, see the INIS website for current contact and E-mail addresses
Secondary number(s)
IPNO-T--04-01