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A. N. Khorramian 3 July 2006 - QCD06, Montpellier
A. N. Khorramian 3 July 2006 - QCD06, Montpellier
A. N. Khorramian 3 July 2006 - QCD06, Montpellier
A. N. Khorramian 3 July 2006 - QCD06, Montpellier
A. N. Khorramian 3 July 2006 - QCD06, Montpellier
A. N. Khorramian 3 July 2006 - QCD06, Montpellier
A. N. Khorramian 3 July 2006 - QCD06, Montpellier
A. N. Khorramian 3 July 2006 - QCD06, Montpellier
A. N. Khorramian 3 July 2006 - QCD06, Montpellier
A. N. Khorramian 3 July 2006 - QCD06, Montpellier
A. N. Khorramian 3 July 2006 - QCD06, Montpellier
A. N. Khorramian 3 July 2006 - QCD06, Montpellier
A. N. Khorramian 3 July 2006 - QCD06, Montpellier
A. N. Khorramian 3 July 2006 - QCD06, Montpellier
A. N. Khorramian 3 July 2006 - QCD06, Montpellier
A. N. Khorramian 3 July 2006 - QCD06, Montpellier
A. N. Khorramian 3 July 2006 - QCD06, Montpellier
A. N. Khorramian 3 July 2006 - QCD06, Montpellier
A. N. Khorramian 3 July 2006 - QCD06, Montpellier
A. N. Khorramian 3 July 2006 - QCD06, Montpellier
A. N. Khorramian 3 July 2006 - QCD06, Montpellier
A. N. Khorramian 3 July 2006 - QCD06, Montpellier
A. N. Khorramian 3 July 2006 - QCD06, Montpellier
A. N. Khorramian 3 July 2006 - QCD06, Montpellier
A. N. Khorramian 3 July 2006 - QCD06, Montpellier
A. N. Khorramian 3 July 2006 - QCD06, Montpellier
A. N. Khorramian 3 July 2006 - QCD06, Montpellier
A. N. Khorramian 3 July 2006 - QCD06, Montpellier
A. N. Khorramian 3 July 2006 - QCD06, Montpellier
A. N. Khorramian 3 July 2006 - QCD06, Montpellier
Conclusion • PDFs can not be calculated from theory and are obtained from fits to data. • In this work valence quark distributions is derived from xF3 data by using NLO logarithmic expansions . • After calculating parton distributions at scale of Q0, valence quark densities and Non-singlet structure function are available. • The results of the Non-singlet structure function are in good agreement with other theoretical model and CCFR experimental data.