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Nuclear modification of high-p_T hadron spectra in p+A collisions at LHC
Nuclear Theory · Submitted 9 Apr 2012
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim They are shown to modify the partonic flavor content of final jets and momentum spectra of final hadrons in p+A collisions at the Large Hadron Collider.
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The abstract, sentence by sentence
Multiple parton scatterings in high-energy p+A collisions involve multi-parton correlation inside the projectile and color coherence of multiple jets which will lead to nuclear modification of final hadron spectra relative to that in p+p collisions. Such modification of final hadron spectra in p+A collisions is studied within HIJING 2.1 model which includes initial parton shadowing, transverse momentum broadening, parton flavor and momentum correlation inside the projectile through flavor and momentum conservation and fragmentation of multiple jets. They are shown to modify the partonic flavor content of final jets and momentum spectra of final hadrons in p+A collisions at the Large Hadron Collider.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Multiple parton scatterings in high-energy p+A collisions involve multi-parton correlation inside the projectile and color coherence of multiple jets which will lead to nuclear modification of final hadron spectra relative to that in p+p collisions. | background 0.99 | 0.10 | 0.40 | hedged possibility 0.56 |
| s1 | Such modification of final hadron spectra in p+A collisions is studied within HIJING 2.1 model which includes initial parton shadowing, transverse momentum broadening, parton flavor and momentum correlation inside the projectile through flavor and momentum conservation and fragmentation of multiple jets. | method 0.93 | 0.70 | 0.10 | asserted 1.00 |
| s2 | They are shown to modify the partonic flavor content of final jets and momentum spectra of final hadrons in p+A collisions at the Large Hadron Collider. | result 0.99 | 0.79 | 0.62 | asserted 1.00 |
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The paper
Original abstract
Multiple parton scatterings in high-energy p+A collisions involve multi-parton correlation inside the projectile and color coherence of multiple jets which will lead to nuclear modification of final hadron spectra relative to that in p+p collisions. Such modification of final hadron spectra in p+A collisions is studied within HIJING 2.1 model which includes initial parton shadowing, transverse momentum broadening, parton flavor and momentum correlation inside the projectile through flavor and momentum conservation and fragmentation of multiple jets. They are shown to modify the partonic flavor content of final jets and momentum spectra of final hadrons in p+A collisions at the Large Hadron Collider.
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References
How the literature uses it
21 arXiv papers cite this in 31 sentences
Papers citing it · 15 sentences without a confident label
Builds on it 1 paper
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We also extropolate our calculation to LHC energy and give the prediction of $dN_ch/dη$ for $p+Pb$ at $√(s)=4.4$ TeV [ref] .
Suppression of high $p_T$ hadron spectra in $p+A$ collisions · Introduction · 0.91
Uses its method or tool 4 papers
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We will first use HIJING Monte Carlo model [ref] to study the intrinsic dihadron correlations in p+p and A+A collisions from minijets without final state interaction.
Relics of Minijets amid Anisotropic Flows in High-energy Heavy-ion Collisions · Introduction · 1.00
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The HIJING 2.1 generator [ref] is employed to estimate the systematic uncertainty (Section [ref]).
Production of muons from heavy-flavour hadron decays in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV · Analysis strategy · 1.00
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Examples employed here include $𝙷𝙸𝙹𝙸𝙽𝙶$ [ref] , $𝙷𝙸𝙹𝙸𝙽𝙶𝙱𝙱$ [ref] and $𝙰𝙼𝙿𝚃$ [ref] .
Predictions for $p+$Pb Collisions at $\sqrt{s_{NN}} = 5$ TeV: Comparison with Data · Charged particles · 0.96
Compares with it 4 papers
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A comparison of the model calculations with the data shows that most of the models that include shadowing [ref] or saturation [ref] predict the measured multiplicity values to within 20% (see also Tab. [ref]).
Pseudorapidity density of charged particles in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV · Introduction · 1.00
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Phenomenological models like HIJING [ref] , EPOS LHC [ref] and EPOS 3 [ref] reproduce the data better for the Pb-going side than for the proton-going side.
ALICE results on system-size dependence of charged-particle multiplicity density in p-Pb, Pb-Pb and Xe-Xe collisions · Results and discussion · 0.96
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The prediction from the HIJING 2.1 model [ref] describes, with shadowing, the trend seen in the data, although it seems that, with the present shadowing parameter $s_g$, the model underpredicts the data.
Transverse momentum distribution and nuclear modification factor of charged particles in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV · Introduction · 0.94
Cites it as background 3 papers
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The two-component models [ref] combine perturbative QCD processes with soft interactions, and include nuclear modification of the initial parton distributions.
Pseudorapidity density of charged particles in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV · Introduction · 0.88
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Among these effects, an important role is played by transverse momentum ($k_T$) broadening of initial- and final-state partons [ref] , and by the modification of the parton distributions functions in bound nucleons compared to those of free nucleons, leading in particular to a reduction of parton densities (shadowing) at small parton fractional momentum $x$ [ref] .
Inclusive photon production at forward rapidities in pp and p$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV · Introduction · 0.98
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There are also calculations and predictions for the nuclear modification factor in Monte Carlo models such as HIJING [ref] .
Nuclear modification of high transverse momentum particle production in p+A collisions at RHIC and LHC · Introduction · 0.94
What it cites · 1 sentence without a confident label
Compares with 2 papers
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The final hadron spectra at large $p_T$ are however significantly suppressed due to the Lund string fragmentation of multiple parton systems (solid and dashed curves in the lower panel) leaving no room for additional suppression by jet quenching as compared to experimental data from ALICE [ref] and CMS [ref] .
Suppression of charged particle production at large transverse momentum in central Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV · Introduction · 0.96
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Shown in Fig. [ref] are HIJING 2.1 results on rapidity distributions of charged hadrons in minimum-biased $d+Au$ (upper panel) and $p+Pb$ (lower panel) collisions (solid) at $√(s)_NN=200$ GeV and 5.0 TeV, respectively, as compared to $d+Au$ data from the STAR experiment [ref] .
Charged particle distributions and nuclear modification at high rapidities in d+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV · Introduction · 0.96
Cites as support 4 papers
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Recent studies show that multiple parton scatterings inside a quark-gluon plasma can in fact change the the color flow of the jet parton shower from that in vacuum [ref] .
Decoherence and energy loss in QCD cascades in nuclear collisions · Introduction · 0.97
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Recent studies show that multiple parton scatterings inside a quark-gluon plasma can in fact change the the color flow of the jet parton shower from that in vacuum [ref] .
Antiangular Ordering of Gluon Radiation in QCD Media · Introduction · 0.97
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Recent studies show that multiple parton scatterings inside a quark-gluon plasma can in fact change the the color flow of the jet parton shower from that in vacuum [ref] .
Interference effects in medium-induced gluon radiation · Introduction · 0.97
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