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Double-parton scattering contribution to production of jet pairs with large rapidity separation at the LHC
High Energy Physics - Phenomenology · Submitted 11 Mar 2014
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Relative contribution of DPS is growing at large rapidity distance between jets.
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The abstract, sentence by sentence
We discuss production of four-jet final state $pp \rightarrow j j j j X$ in proton-proton collisions at the LHC through the mechanism of double-parton scattering (DPS) in the context of jets with large rapidity separation. The DPS contributions are calculated within the so-called factorized Ansatz and each step of DPS is calculated in the LO collinear approximation. The LO pQCD calculations are shown to give a reasonably good descritption of recent CMS and ATLAS data on inclusive jet production and therefore this formalism can be used to reliably estimate the DPS effects. Relative contribution of DPS is growing at large rapidity distance between jets. This is consistent with our experience from previous studies of double-parton scattering effects in the case of open and hidden charm production. The calculated differential cross sections as a function of rapidity distance between the most remote in rapidity jets are compared with recent results of LL and NLL BFKL calculations for Mueller-Navelet (MN) jet production at $\sqrt{s} = 7$ TeV. The DPS contribution to widely rapidity separated jet production is carefully studied for the present energy $\sqrt{s}$ = 7 TeV and also at the nominal LHC energy $\sqrt{s}$ = 14 TeV and in different ranges of jet transverse momenta. The differential cross section as a function of dijet transverse momenta as well as two-dimensional ($p_{T}(y_{min})\times p_{T}(y_{max})$)-plane correlations for DPS mechanism are also presented. Some ideas how the DPS effects could be studied in the case of double dijet production are suggested.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We discuss production of four-jet final state $pp \rightarrow j j j j X$ in proton-proton collisions at the LHC through the mechanism of double-parton scattering (DPS) in the context of jets with large rapidity separation. | contribution 0.95 | 0.54 | 0.07 | asserted 0.78 |
| s1 | The DPS contributions are calculated within the so-called factorized Ansatz and each step of DPS is calculated in the LO collinear approximation. | method 1.00 | 0.88 | 0.03 | asserted 1.00 |
| s2 | The LO pQCD calculations are shown to give a reasonably good descritption of recent CMS and ATLAS data on inclusive jet production and therefore this formalism can be used to reliably estimate the DPS effects. | interpretation 0.60 | 0.77 | 0.08 | asserted 0.94 |
| s3 | Relative contribution of DPS is growing at large rapidity distance between jets. | result 0.99 | 0.84 | 0.56 | asserted 1.00 |
| s4 | This is consistent with our experience from previous studies of double-parton scattering effects in the case of open and hidden charm production. | interpretation 0.72 | 0.24 | 0.09 | hedged possibility 0.85 |
| s5 | The calculated differential cross sections as a function of rapidity distance between the most remote in rapidity jets are compared with recent results of LL and NLL BFKL calculations for Mueller-Navelet (MN) jet production at $\sqrt{s} = 7$ TeV. | contribution 0.68 | 0.66 | 0.07 | asserted 0.97 |
| s6 | The DPS contribution to widely rapidity separated jet production is carefully studied for the present energy $\sqrt{s}$ = 7 TeV and also at the nominal LHC energy $\sqrt{s}$ = 14 TeV and in different ranges of jet transverse momenta. | contribution 0.98 | 0.93 | 0.10 | asserted 0.99 |
| s7 | The differential cross section as a function of dijet transverse momenta as well as two-dimensional ($p_{T}(y_{min})\times p_{T}(y_{max})$)-plane correlations for DPS mechanism are also presented. | result 0.53 | 0.91 | 0.05 | asserted 0.99 |
| s8 | Some ideas how the DPS effects could be studied in the case of double dijet production are suggested. | future work 0.99 | 0.34 | 0.04 | hedged possibility 0.97 |
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The paper
Original abstract
We discuss production of four-jet final state $pp \rightarrow j j j j X$ in proton-proton collisions at the LHC through the mechanism of double-parton scattering (DPS) in the context of jets with large rapidity separation. The DPS contributions are calculated within the so-called factorized Ansatz and each step of DPS is calculated in the LO collinear approximation. The LO pQCD calculations are shown to give a reasonably good descritption of recent CMS and ATLAS data on inclusive jet production and therefore this formalism can be used to reliably estimate the DPS effects. Relative contribution of DPS is growing at large rapidity distance between jets. This is consistent with our experience from previous studies of double-parton scattering effects in the case of open and hidden charm production. The calculated differential cross sections as a function of rapidity distance between the most remote in rapidity jets are compared with recent results of LL and NLL BFKL calculations for Mueller-Navelet (MN) jet production at $\sqrt{s} = 7$ TeV. The DPS contribution to widely rapidity separated jet production is carefully studied for the present energy $\sqrt{s}$ = 7 TeV and also at the nominal LHC energy $\sqrt{s}$ = 14 TeV and in different ranges of jet transverse momenta. The differential cross section as a function of dijet transverse momenta as well as two-dimensional ($p_{T}(y_{min})\times p_{T}(y_{max})$)-plane correlations for DPS mechanism are also presented. Some ideas how the DPS effects could be studied in the case of double dijet production are suggested.
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How the literature uses it
14 arXiv papers cite this in 19 sentences
Papers whose main result relates to this one's
States the same result 2 papers
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We show that the relative (with respect to SPS dijets and to the BFKL Mueller-Navelet (MN) jets) contribution of DPS is growing at large rapidity distance between jets.
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We show that the relative contribution of DPS is growing with respect to standard single-parton scattering (SPS) production of dijets and to the BFKL Mueller-Navelet (MN) jet mechanism at large rapidity distance between jets.
Papers citing it · 14 sentences without a confident label
Uses its method or tool 1 paper
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This simplified leading-order approach was used in our first estimate of DPS differential cross sections for jets widely separated in rapidity [ref] .
Double parton scattering at high energies · Four-jet production in DPS · 0.80
Cites it as background 4 papers
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Another observable discussed in Ref. [ref] is the distribution in transverse momentum of the most remote jets.
Searching for and exploring double-parton scattering effects in four-jet production at the LHC · First results · 0.82
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The case of double-parton scattering is usually described within the framework of the standard collinear perturbative QCD by means of the double parton distribution functions (DPDFs) [ref] .
Numerical analysis of the unintegrated double gluon distribution · Introduction · 0.96
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The double-parton scattering contribution to the Mueller–Navelet jet production was considered in Refs. [ref] , using different approaches.
High-energy resummation in semi-hard processes at the LHC · Outlook · 0.89
What it cites · 28 sentences without a confident label
Uses data or values from 2 papers
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Experimental data from the Tevatron [ref] and the LHC [ref] provide an estimate of $σ_eff$ in the denominator of formula ([ref]).
Observation of $J/\psi$ pair production in pp collisions at $\sqrt{s}=7 TeV$ · Basic formalism · 0.99
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Experimental data from the Tevatron [ref] and the LHC [ref] provide an estimate of $σ_eff$ in the denominator of formula ([ref]).
Observation of double charm production involving open charm in pp collisions at $\sqrt{s}$=7 TeV · Basic formalism · 0.99
Compares with 3 papers
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In Fig. [ref] we compare our calculation with the CMS data [ref] .
Measurement of the Inclusive Jet Cross Section in pp Collisions at sqrt(s) = 7 TeV · Numerical Results · 0.97
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The ($p_1t,p_2t$) distribution for the DPS mechanism is rather different than similar distributions for dijet SPS [ref] and MN jets [ref] .
Dijet correlations at RHIC, leading-order $k_t$-factorization approach versus next-to-leading order collinear approach · Numerical Results · 0.97
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For comparison we show also results for the LL and NLL BFKL calculation for MN jet from Ref. [ref] .
Confronting Mueller-Navelet jets in NLL BFKL with LHC experiments at 7 TeV · Numerical Results · 1.00
Cites as background 3 papers
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The dijet azimuthal correlations were also studied in collinear next-to-leading order approximation [ref] .
Jet-jet and hadron-jet correlations in hadro- and electro-production · Introduction · 0.85
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A detailed analysis of $σ_eff$ based on various experimental data can be found in Refs. [ref] .
Extracting sigma_effective from the CDF gamma+3jets measurement · Basic formalism · 0.95
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A detailed analysis of $σ_eff$ based on various experimental data can be found in Refs. [ref] .
Constraining MPI models using sigma_effective and recent Tevatron and LHC Underlying Event data · Basic formalism · 0.95
Discussion
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