We present a detailed QCD analysis of nucleon structure functions x F 3 ( x , Q 2 ) , based on Laplace transforms and the Jacobi polynomials approach. The analysis corresponds to the next-to-leading order and next-to-next-to-leading order approximations of perturbative QCD. The Laplace transform technique, as an exact analytical solution, is used for the solution of nonsinglet Dokshitzer-Gribov-Lipatov-Altarelli-Parisi evolution equations at low- and large-x values. The extracted results are used as input to obtain the x and Q 2 evolution of x F 3 ( x,Q2) structure functions using the Jacobi polynomials approach. In our work, the values of the typical QCD scale Λ ( n f)MS and the strong coupling constant α s (M2Z) are...
An exact expression for the leading-order (LO) gluon distribution function G(x,Q 2)=xg(x,Q 2) from t...
We apply analytic perturbation theory to the QCD analysis of the xF3 structure function data of the ...
We report [1] on the first calculation of the structure function g1 in polarised deep-inelastic scat...
We present a detailed QCD analysis of nucleon structure functions x F 3 ( x , Q 2 ) , bas...
We present a detailed QCD analysis of nucleon structure functions xF3(x,Q2), based on Laplace transf...
The next-to-next-to-leading order (NNLO) non-singlet QCD analysis of the experimental data of the CC...
An analytical solution based on the Laplace transformation technique for the Dokshitzer-Gribov-Lipat...
An analytical solution based on the Laplace transformation technique for the Dokshitzer-Gribov-Lipat...
We present a first QCD analysis of next-to-next-leading-order (NNLO) contributions of the spindepend...
We summarize recent results on the evolution of unpolarized parton densities and deep-inelastic stru...
We present the results of the leading order (LO) and next-to-leading order (NLO) QCD analysis of exp...
We present the new framework based on BFKL and DGLAP evolution equations in which the leading ln(Q&q...
We present the next-to-next-to-leading order (NNLO) contributions to the main splitting functions fo...
We report on a high statistics quenched lattice QCD calculation of the deep-inelastic structure func...
We apply analytic perturbation theory to the QCD analysis of the xF3 structure function data of the ...
An exact expression for the leading-order (LO) gluon distribution function G(x,Q 2)=xg(x,Q 2) from t...
We apply analytic perturbation theory to the QCD analysis of the xF3 structure function data of the ...
We report [1] on the first calculation of the structure function g1 in polarised deep-inelastic scat...
We present a detailed QCD analysis of nucleon structure functions x F 3 ( x , Q 2 ) , bas...
We present a detailed QCD analysis of nucleon structure functions xF3(x,Q2), based on Laplace transf...
The next-to-next-to-leading order (NNLO) non-singlet QCD analysis of the experimental data of the CC...
An analytical solution based on the Laplace transformation technique for the Dokshitzer-Gribov-Lipat...
An analytical solution based on the Laplace transformation technique for the Dokshitzer-Gribov-Lipat...
We present a first QCD analysis of next-to-next-leading-order (NNLO) contributions of the spindepend...
We summarize recent results on the evolution of unpolarized parton densities and deep-inelastic stru...
We present the results of the leading order (LO) and next-to-leading order (NLO) QCD analysis of exp...
We present the new framework based on BFKL and DGLAP evolution equations in which the leading ln(Q&q...
We present the next-to-next-to-leading order (NNLO) contributions to the main splitting functions fo...
We report on a high statistics quenched lattice QCD calculation of the deep-inelastic structure func...
We apply analytic perturbation theory to the QCD analysis of the xF3 structure function data of the ...
An exact expression for the leading-order (LO) gluon distribution function G(x,Q 2)=xg(x,Q 2) from t...
We apply analytic perturbation theory to the QCD analysis of the xF3 structure function data of the ...
We report [1] on the first calculation of the structure function g1 in polarised deep-inelastic scat...