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QCD theory overview
High Energy Physics - Phenomenology · Submitted 24 Dec 2020
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim The review covers topics like Improved Transverse Momentum Dependent Factorization, $k_T$ dependent splitting functions, Transversal Momentum Dependent parton shower, non-Gaussian broadening of jet traversing quark gluon plasma.
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The abstract, sentence by sentence
In this review I am going to present biased by personal experience review of QCD. The review covers topics like Improved Transverse Momentum Dependent Factorization, $k_T$ dependent splitting functions, Transversal Momentum Dependent parton shower, non-Gaussian broadening of jet traversing quark gluon plasma.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | In this review I am going to present biased by personal experience review of QCD. | contribution 0.48 | 0.30 | 0.04 | asserted 0.87 |
| s1 | The review covers topics like Improved Transverse Momentum Dependent Factorization, $k_T$ dependent splitting functions, Transversal Momentum Dependent parton shower, non-Gaussian broadening of jet traversing quark gluon plasma. | contribution 0.94 | 0.13 | 0.07 | asserted 0.98 |
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The paper
Original abstract
In this review I am going to present biased by personal experience review of QCD. The review covers topics like Improved Transverse Momentum Dependent Factorization, $k_T$ dependent splitting functions, Transversal Momentum Dependent parton shower, non-Gaussian broadening of jet traversing quark gluon plasma.
Human review
How the literature uses it
What this paper does with the arXiv papers it cites
What it cites · 72 sentences without a confident label
Builds on 6 papers
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The computation of the gluon-to-gluon splitting $P_gg$ required a further modification of the formalism used in [ref] which was recently achieved in [ref] .
Transverse-momentum-dependent quark splitting functions in $k_T$-factorization: real contributions · Transverse Momentum Dependent splitting functions · 0.92
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The computation of the gluon-to-gluon splitting $P_gg$ required a further modification of the formalism used in [ref] which was recently achieved in [ref] .
TMD splitting functions in kT factorization: the real contribution to the gluon-to-gluon splitting · Transverse Momentum Dependent splitting functions · 0.92
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The computation of the gluon-to-gluon splitting $P_gg$ required a further modification of the formalism used in [ref] which was recently achieved in [ref] .
High-Energy Factorization and Small-X Deep Inelastic Scattering Beyond Leading Order · Transverse Momentum Dependent splitting functions · 0.92
Uses the method or tool of 7 papers
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Here I will describe application of TMD parton densities, TMD parton showers [ref] [Very recently new very successful approach to obtain TMD pdfs called Parton Branching method has been developed [ref] .] and off-shell matrix elements obtained from [ref] to dijets calculations.
NLO prescription for unintegrated parton distributions · Monte Carlo with Transverse Momentum Dependent shower · 0.98
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Here I will describe application of TMD parton densities, TMD parton showers [ref] [Very recently new very successful approach to obtain TMD pdfs called Parton Branching method has been developed [ref] .] and off-shell matrix elements obtained from [ref] to dijets calculations.
KaTie: for parton-level event generation with k_T-dependent initial states · Monte Carlo with Transverse Momentum Dependent shower · 0.98
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Here I will describe application of TMD parton densities, TMD parton showers [ref] [Very recently new very successful approach to obtain TMD pdfs called Parton Branching method has been developed [ref] .] and off-shell matrix elements obtained from [ref] to dijets calculations.
Collinear and TMD parton densities from fits to precision DIS measurements in the parton branching method · Monte Carlo with Transverse Momentum Dependent shower · 0.98
Uses data or values from 1 paper
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The points with error bars represent experimental data from Ref. [ref] .
Dijet azimuthal correlations and conditional yields in $pp$ and $p$+Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV with the ATLAS detector · Factorization for forward dijet production · 0.83
Compares with 4 papers
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Fig. [ref] shows predictions for the azimuthal de-correlation $Δϕ$ for high dijets for different regions of $^leading$ using TMD parton densities with off-shell matrix elements, parton shower and hadronization in comparison with measurements at $√(s) = 7$ TeV in pp collisions at the LHC [ref] .
Dijet Azimuthal Decorrelations in pp Collisions at sqrt(s) = 7 TeV · Monte Carlo with Transverse Momentum Dependent shower · 0.96
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Thus, Eq. ([ref]) shows the same kind of suppression for the emission of highly energetic gluons due to interferences as the approach by Baier Dokshitzer Mueller Peigné, Schiff, and Zakharov (BDMPS-Z) [ref] .
Fully quantum treatment of the Landau--Pomeranchuk--Migdal effect in QED and QCD · Non-Gaussian broadening in jet quenching · 0.98
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Thus, Eq. ([ref]) shows the same kind of suppression for the emission of highly energetic gluons due to interferences as the approach by Baier Dokshitzer Mueller Peigné, Schiff, and Zakharov (BDMPS-Z) [ref] .
Radiative energy loss and $p_{\perp}$-broadening of high energy partons in nuclei · Non-Gaussian broadening in jet quenching · 0.98
Cites as support 3 papers
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It has been shown in Refs. [ref] that inclusion of Sudakov logarithms is necessary in order to describe the LHC jet data at small $x$ but yet before the saturation regime.
Small-$x$ dynamics in forward-central dijet decorrelations at the LHC · Factorization for forward dijet production · 0.99
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It has been shown in Refs. [ref] that inclusion of Sudakov logarithms is necessary in order to describe the LHC jet data at small $x$ but yet before the saturation regime.
Resummation effects in forward production of Z0+jet at LHC · Factorization for forward dijet production · 0.99
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This effect can be significant even at large transverse momenta, as has been discussed and shown explicitly in [ref] .
Collinearity approximations and kinematic shifts in partonic shower algorithms · Monte Carlo with Transverse Momentum Dependent shower · 1.00
Cites as background 4 papers
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The quantities $Φ_^ag→cd^_(i)$ are the TMD gluon distributions introduced in Ref. [ref] and parametrize a dense state of the nucleus or the proton in terms of small-$x$ gluons, see Ref. [ref] for an overview.
TMD gluon distributions at small x in the CGC theory · Factorization for forward dijet production · 0.86
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The quantities $Φ_^ag→cd^_(i)$ are the TMD gluon distributions introduced in Ref. [ref] and parametrize a dense state of the nucleus or the proton in terms of small-$x$ gluons, see Ref. [ref] for an overview.
Improved TMD factorization for forward dijet production in dilute-dense hadronic collisions · Factorization for forward dijet production · 0.86
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The behaviour of dense systems of partons when $x$ becomes small is predicted by Quantum Chromodynamics (QCD) and leads to non-linear evolution equations known as B-JIMWLK equations (for review see [ref] ), which can be derived within the Color Glass Condensate (CGC) theory.
The Color Glass Condensate · Factorization for forward dijet production · 0.96
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