Soft emissions and the equivalence of BFKL and CCFM final states

This article demonstrates that the BFKL and CCFM equations, despite their different physical content, lead to equivalent results for any final-state observable at leading single-logarithmic order. A novel and fundamental element is the treatment also of the soft (z->1 divergent) part of the splitting function in the CCFM equation.

lepton nucleon: deep inelastic scattering
quantum chromodynamics
jet: leptoproduction
gluon: emission
Lipatov equation
kinematics: phase space

References(43)

Figures(0)

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