BFKL next-to-next-to-leading order

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BFKL at next-to-leading order

This is a summary of the contributions on the next-to-leading order corrections to the BFKL equation which were presented to the ‘Small-x and Diffraction’ working group at the 1998 Durham Workshop on HERA Physics. The original BFKL equation [1] allowed the computation of elastic scattering amplitudes in the Regge limit to leading logarithmic (LO) accuracy, i.e. all terms ∼ (αs ln s)n are summed...

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An introduction to leading and next-to-leading BFKL

Some twenty-five years ago Balitsky, Fadin, Kuraev and Lipatov (BFKL) set out to determine the high-energy behaviour of the scattering of hadronic objects within perturbative QCD. They found terms going as (αs ln s) n, where s is the squared centre-of-mass energy. Since ln s is large it can compensate the smallness of ᾱs and thus it was necessary to sum this whole series of leading logarithmic ...

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ژورنال

عنوان ژورنال: Nuclear Physics B

سال: 2007

ISSN: 0550-3213

DOI: 10.1016/j.nuclphysb.2007.05.024