The quark beam function at NNLL

DOI10.1007/JHEP09(2010)005zbMath1291.81397arXiv1002.2213OpenAlexW2024904055MaRDI QIDQ2251082

Frank J. Tackmann, Iain W. Stewart, Wouter J. Waalewijn

Publication date: 10 July 2014

Published in: Journal of High Energy Physics (Search for Journal in Brave)

Full work available at URL: https://arxiv.org/abs/1002.2213

zbMATH Keywords

renormalization groupQCDNLO computationshadronic colliders

Mathematics Subject Classification ID

Nuclear physics (81V35) Strong interaction, including quantum chromodynamics (81V05) Perturbative methods of renormalization applied to problems in quantum field theory (81T15) Renormalization group methods applied to problems in quantum field theory (81T17)

Related Items (10)

An effective field theory for forward scattering and factorization violation ⋮ Beam functions for \(N\)-jettiness at \(\mathrm{N^3LO}\) in perturbative QCD ⋮ Next-to-next-to-leading order \(N\)-jettiness soft function for one massive colored particle production at hadron colliders ⋮ Resummation of transverse momentum distributions in distribution space ⋮ Parton fragmentation within an identified jet at NNLL ⋮ Non-global structure of the \(\mathcal{O}\left( {\alpha_s^2} \right) \) dijet soft function ⋮ Proper factorization theorems in high-energy scattering near the endpoint ⋮ Coulomb gluons will generally destroy coherence ⋮ Factorization connecting continuum \& lattice TMDs ⋮ The infrared structure of perturbative gauge theories

Cites Work

• The three-loop splitting functions in QCD: the non-singlet case
• Reparameterization invariance for collinear operators
• Invariant operators in collinear effective theory

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