We discuss the quantitative consequences of the resummation of the small-x contributions to the anomalous dimensions beyond next-to-leading order in alpha_s and up to next order in ln(1/x) (NLx) in a framework based on the renormalization group equations. We find large and negative effects leading to negative values for the {\sf total} splitting function P_{gg}(x,alpha_s) already for x \lsim 0.01 at Q^2 \simeq 20 GeV^2. Terms less singular than those under consideration turn out to be quantitatively as important and need to be included. We derive the effects of the conformal part of the NLx contributions to the anomalous dimensions and discuss the exponent omega describing the s^omega behavior of inclusive cross sections
AbstractWe analyze the iterative structure of unfactorized partonic structure functions in the large...
The status of the resummation of small x contributions to the unpolarized and polarized deep inelast...
We numerically analyse the evolution of the flavor non-singlet $g_{1}$ structure function taking int...
We discuss the quantitative consequences of the resummation of the small-x contributions to the anom...
We report the results of including resummed splitting functions in the QCD evolution equations at sm...
The impact of the resummed next-to-leading logarithmic small-$x$ contributions to the anomalous dime...
The impact of the resummed next-to-leading logarithmic small-$x$ contributions to the anomalous dime...
The impact of the resummed next-to-leading logarithmic small-x contributions to the anomalous dimens...
A brief overview is presented of recent developments concerning resummed small-x evolution, based up...
AbstractThis remark is part of an ongoing project to simplify the structure of the multi-loop anomal...
The double logarithmic terms $\alpha_{s} \ln^{2}x $ are important to predict precisely the small $x$...
After a brief introduction to low-x QCD and to resummation approaches, I illustrate the predictions ...
AbstractThe modified evolution equation for parton distributions of Dokshitzer, Marchesini and Salam...
We summarize our recent results on small x resummation in full QCD with n_f quark flavours and discu...
I review the k-factorization method to combine the high-energy behaviour in QCD with the renormaliza...
AbstractWe analyze the iterative structure of unfactorized partonic structure functions in the large...
The status of the resummation of small x contributions to the unpolarized and polarized deep inelast...
We numerically analyse the evolution of the flavor non-singlet $g_{1}$ structure function taking int...
We discuss the quantitative consequences of the resummation of the small-x contributions to the anom...
We report the results of including resummed splitting functions in the QCD evolution equations at sm...
The impact of the resummed next-to-leading logarithmic small-$x$ contributions to the anomalous dime...
The impact of the resummed next-to-leading logarithmic small-$x$ contributions to the anomalous dime...
The impact of the resummed next-to-leading logarithmic small-x contributions to the anomalous dimens...
A brief overview is presented of recent developments concerning resummed small-x evolution, based up...
AbstractThis remark is part of an ongoing project to simplify the structure of the multi-loop anomal...
The double logarithmic terms $\alpha_{s} \ln^{2}x $ are important to predict precisely the small $x$...
After a brief introduction to low-x QCD and to resummation approaches, I illustrate the predictions ...
AbstractThe modified evolution equation for parton distributions of Dokshitzer, Marchesini and Salam...
We summarize our recent results on small x resummation in full QCD with n_f quark flavours and discu...
I review the k-factorization method to combine the high-energy behaviour in QCD with the renormaliza...
AbstractWe analyze the iterative structure of unfactorized partonic structure functions in the large...
The status of the resummation of small x contributions to the unpolarized and polarized deep inelast...
We numerically analyse the evolution of the flavor non-singlet $g_{1}$ structure function taking int...