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Gluon Evolution at small-x : Extending the PT Domain of QCD Dimitri Colferai University of Firenze M. Ciafaloni G.P. Salam A.M. Stasto In collaboration with: { DIS 03 St. Petersburg, 23-27 April 2003
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Outline Definition of the RGI approach Green’s function Extension of PT domain Splitting function
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vs picture BFKLDGLAP ’ ’ ’
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BFKL vs DGLAP kernel in the collinear limit k >> k’ Simplified case: ; Scale change: h’ h G’ G h’ h
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What have we learnt? Position of collinear -poles of evolution kernels depends on s 0 Origin of cubic poles in 1 ( ) : expansion around = 0 of shifted poles ~1/( + /2) Non-singular part A( ) of anomalous dimension gg ( ) A( ) can be taken into account by a subleading kernel in 2 ways: (remember )
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Definition of RG Improved Approach Adapting the procedure for running s and with s 0 = Q 1 Q 2 : resums scale dependent terms of a pure BFKL approach resums exact 1-loop gluon anomalous dimension (note -dependence of A ) includes left-over exact NL BFKL infos This procedure implements kinematical constraints
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Y-evolution of Green’s function Diffusion corrections: Hard Pomeron Scheme A Scheme B fixed running numeric
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Domain of applicability of perturbative QCD
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Resummed splitting function is independent of : important check of RG factorization Evolution eqn. Gluon density High-energy exponent c ( s )
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Conclusions 2 main problems of high-energy perturbative QCD: occurrence of large leading log s contributions and of subleading ones of comparable size and opposite sign increasing importance of wee partons, whence a strong coupling non-perturbative Pomeron regime RGI approach tames both problems: through an understanding and consequent resummation of the most important subleading contributions Subleading corrections and running coupling effects lower high- energy exponents and diffusion/tunneling into NP region We expect a large domain of applicability of PT QCD We have the tools to make reliable physical predictions: *- *, forward jets, Mueller-Navelet jets, …
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