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DGLAP

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Parent: ZEUS (experiment) Hop 5
Expansion Funnel Raw 67 → Dedup 0 → NER 0 → Enqueued 0
1. Extracted67
2. After dedup0 (None)
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DGLAP
NameDGLAP
FieldParticle physics
Introduced1970s
Derived fromQuantum chromodynamics
Key peopleVladimir Gribov, Lev Lipatov, Yuri Dokshitzer, Georgi Altarelli, Guido Parisi
Influenced byRichard Feynman, Murray Gell-Mann, Kenneth Wilson

DGLAP DGLAP denotes a set of evolution equations central to perturbative Quantum Chromodynamics and high-energy particle physics. Derived in the early 1970s by five authors whose initials form the acronym, the formalism relates scale dependence of parton distributions measured in processes at colliders such as the Large Hadron Collider and the Stanford Linear Accelerator Center. Its predictive power underlies global analyses by collaborations like CTEQ, NNPDF, and MSTW, and informs theoretical work connected to the European Organization for Nuclear Research and the Fermi National Accelerator Laboratory.

Introduction

The DGLAP framework was developed by Yuri Dokshitzer, Vladimir Gribov, Lev Lipatov, Georgi Altarelli, and Guido Parisi to describe how parton distribution functions change with a hard scale such as the momentum transfer in deep inelastic scattering experiments at facilities like DESY and the CERN SPS. It connects short-distance calculations in Quantum Chromodynamics with experimental observables from experiments like HERA and the Tevatron. The equations are integral-differential relations used extensively by global fit groups including HERAPDF and MMHT to extract parton densities for use in predicting cross sections for processes measured by collaborations such as ATLAS and CMS.

Theoretical Basis

DGLAP is rooted in renormalization group concepts developed by Kenneth Wilson and perturbative techniques advanced by Richard Feynman and Murray Gell-Mann. It exploits factorization theorems formalized by researchers at institutions such as SLAC National Accelerator Laboratory and Brookhaven National Laboratory to separate long-distance parton structure from short-distance hard scattering kernels computed using Feynman rules. The formal derivation uses operator product expansion methods related to work by Kenneth Wilson and anomalous dimensions introduced in studies by Alexander Polyakov and Gerard 't Hooft. The strong coupling running is governed by the beta function of Quantum Chromodynamics computed by David Gross, Frank Wilczek, and H. David Politzer.

Splitting Functions and Evolution Equations

Key ingredients are the splitting functions, derived perturbatively via diagrams evaluated in gauges used by practitioners at SLAC and CERN. Leading-order splitting kernels were computed by Georgi Altarelli and Guido Parisi, with next-to-leading and higher-order corrections provided by teams associated with Moscow State University, University of Oxford, and University of Cambridge. Splitting functions encode probabilities for parton branchings such as quark-to-quark, quark-to-gluon, and gluon-to-gluon transitions measured in experiments run by ZEUS and H1. The integro-differential evolution equations relate parton distribution functions at one scale to those at another, analogous to renormalization group flows studied by Kenneth Wilson and spectral analyses by Miguel Virasoro.

Solutions and Methods

Solutions use Mellin moment techniques developed in analytic work at Princeton University and numerical methods refined at Los Alamos National Laboratory. Techniques include diagonalization in flavor and singlet-nonsinglet bases used by groups at University of Chicago and expansion in orthogonal polynomials as applied by researchers at University of Milan. Fixed-order solutions employ perturbative matching conditions with heavy-flavor schemes developed by collaborations at DESY and CERN. All-order resummation approaches that address small-x or large-x limits owe conceptual debt to work by Lev Lipatov and methods used in the Regge theory community including Vladimir Gribov.

Applications in High-Energy Physics

DGLAP-evolved parton distributions are essential inputs for theoretical predictions tested by major experiments including ATLAS, CMS, LHCb, ALICE, CDF, and D0. They enable precision determinations of cross sections for Higgs boson production studied by teams at CERN and electroweak measurements performed by collaborations at LEP and SLC. Parton evolution affects backgrounds in searches for beyond-Standard-Model signals pursued by groups at Fermilab and influences interpretations of heavy-ion collision data collected by RHIC and ALICE. Global fits using DGLAP underpin determinations of the strong coupling constant alpha_s cited in reviews by institutions such as the Particle Data Group.

Numerical Implementation and Parton Distribution Fits

Practical usage requires numerical evolution codes maintained by collaborations like LHAPDF, APFEL, and groups at CERN and DESY. Global analyses by CTEQ-TEA, NNPDF, MMHT, HERAPDF, and others combine DGLAP evolution with diverse datasets from HERA, Tevatron, and the LHC to extract quark and gluon distributions. Statistical and systematic treatments employ methods developed at CERN and universities such as University of Oxford and Università di Torino. Benchmarks and comparisons among fits are coordinated at workshops organized by ICHEP and specialized schools hosted by CERN and SLAC.

Extensions and Generalizations

Extensions of the original formalism include transverse-momentum-dependent evolution studied by researchers at Brookhaven National Laboratory and Jefferson Lab, small-x resummation frameworks related to the BFKL equation developed by Lipatov and collaborators, and matched schemes combining DGLAP with threshold resummation pursued by teams at University of Freiburg and Princeton University. Generalizations to polarized parton distributions were advanced by groups at CERN and DESY and are used in spin physics programs at RHIC. Ongoing theoretical developments connect DGLAP evolution to nonperturbative models explored at Institute for Nuclear Research (Moscow) and lattice studies performed by collaborations at Brookhaven National Laboratory and Jefferson Lab.

Category:Quantum chromodynamics