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Suppression of high $p_T$ hadron spectra in $p+A$ collisions
Nuclear Theory · Submitted 30 Jul 2012
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Multi-parton flavor and momentum correlation inside the projectile are incorporated through flavor and momentum conservation which are shown to modify the flavor content and momentum spectra of final partons and most importantly lead to suppression of large $p_{T}$ hadron spectra in $p+A$ collisions at both RHIC and LHC energies.
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The abstract, sentence by sentence
Multiple hard and semi-hard parton scatterings in high-energy $p+A$ collisions involve multi-parton correlation in both momentum and flavor inside the projectile proton which will lead to modification of the final hadron spectra relative to that in $p+p$ collisions. Such modification of final hadron transverse momentum spectra in $p+A$ collisions is studied within HIJING 2.1 Monte Carlo model which includes nuclear shadowing of the initial parton distributions and transverse momentum broadening. Multi-parton flavor and momentum correlation inside the projectile are incorporated through flavor and momentum conservation which are shown to modify the flavor content and momentum spectra of final partons and most importantly lead to suppression of large $p_{T}$ hadron spectra in $p+A$ collisions at both RHIC and LHC energies.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Multiple hard and semi-hard parton scatterings in high-energy $p+A$ collisions involve multi-parton correlation in both momentum and flavor inside the projectile proton which will lead to modification of the final hadron spectra relative to that in $p+p$ collisions. | background 0.96 | 0.14 | 0.10 | asserted 0.58 |
| s1 | Such modification of final hadron transverse momentum spectra in $p+A$ collisions is studied within HIJING 2.1 Monte Carlo model which includes nuclear shadowing of the initial parton distributions and transverse momentum broadening. | method 0.96 | 0.74 | 0.05 | asserted 0.98 |
| s2 | Multi-parton flavor and momentum correlation inside the projectile are incorporated through flavor and momentum conservation which are shown to modify the flavor content and momentum spectra of final partons and most importantly lead to suppression of large $p_{T}$ hadron spectra in $p+A$ collisions at both RHIC and LHC energies. | result 0.96 | 0.85 | 0.92 | asserted 1.00 |
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Original abstract
Multiple hard and semi-hard parton scatterings in high-energy $p+A$ collisions involve multi-parton correlation in both momentum and flavor inside the projectile proton which will lead to modification of the final hadron spectra relative to that in $p+p$ collisions. Such modification of final hadron transverse momentum spectra in $p+A$ collisions is studied within HIJING 2.1 Monte Carlo model which includes nuclear shadowing of the initial parton distributions and transverse momentum broadening. Multi-parton flavor and momentum correlation inside the projectile are incorporated through flavor and momentum conservation which are shown to modify the flavor content and momentum spectra of final partons and most importantly lead to suppression of large $p_{T}$ hadron spectra in $p+A$ collisions at both RHIC and LHC energies.
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References
How the literature uses it
2 arXiv papers cite this in 2 sentences
What it cites · 2 sentences without a confident label
Builds on 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] .
Nuclear modification of high-p_T hadron spectra in p+A collisions at LHC · Introduction · 0.91
Uses the method or tool of 1 paper
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HIJING2.0 [ref] employes the factorized form of parton distributions in nuclei [ref] [equation] where $R_a^A(x,Q^2,b)$ is the impact-parameter-dependent nuclear modification factor.
Hadron production in p+p, p+Pb, and Pb+Pb collisions with the HIJING 2.0 model at energies available at the CERN Large Hadron Collider · Introduction · 0.87
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