Abstract

We study parton-branching solutions of QCD evolution equations and present a method to construct both collinear and transverse momentum dependent (TMD) parton densities from this approach. We work with next-to-leading-order (NLO) accuracy in the strong coupling. Using the unitarity picture in terms of resolvable and non-resolvable branchings, we analyze the role of the soft-gluon resolution scale in the evolution equations. For longitudinal momentum distributions, we find agreement of our numerical calculations with existing evolution programs at the level of better than 1% over a range of five orders of magnitude both in evolution scale and in longitudinal momentum fraction. We make predictions for the evolution of transverse momentum distributions. We perform fits to the high-precision deep inelastic scattering (DIS) structure function measurements, and we present a set of NLO TMD distributions based on the parton branching approach.

Highlights

  • Deep inelastic scattering (DIS) data [34, 35], and used in a parton shower calculation [18] to make predictions for W -boson + jets hadro-production, which can be compared with LHC experimental measurements [36, 37]

  • We study parton-branching solutions of QCD evolution equations and present a method to construct both collinear and transverse momentum dependent (TMD) parton densities from this approach

  • We have shown that a consistent set of TMD parton distributions, valid over a large range in x, k⊥ and μ can be determined from a parton branching solution of QCD evolution equations, as long as the soft gluon region is treated appropriately, e.g. by applying angular ordering conditions

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Summary

Unitarity approach to QCD evolution equations

We give the main elements of the parton-branching approach to the evolution equations. We introduce a soft-gluon resolution scale into the renormalization group evolution equations, and describe resolvable and non-resolvable emissions. We discuss the relationship of our results with the angular-ordered, coherent branching [70,71,72,73] and the behavior of the endpoint z → 1 region in transverse momentum distributions [74, 75]. We construct an iterative Monte Carlo solution of the evolution equations, and apply it to the case of collinear and TMD parton densities

The renormalization group evolution
Expansion in powers of αs
Resolvable and non-resolvable emissions
Momentum sum rule
Sudakov form factor
Solution of the evolution equation applying a Monte Carlo method
Transverse momentum distributions and ordering variables
Numerical parton-branching solution at NLO
Fit to precision DIS data
TMD densities
Conclusions
Findings
A The two-loop R coefficients
Full Text
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