hijing: A Monte Carlo model for multiple jet production in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>pp</mml:mi></mml:math>,<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>pA</mml:mi></mml:math>, and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>AA</mml:mi></mml:math>collisions

Wang, Xin‐Nian; Gyulassy, Miklós

doi:10.1103/physrevd.44.3501

Cited by 1,756 publications

(1,766 citation statements)

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“…This is done statistically by removing the contribution of muons from π/K weak decays. We obtain the π/K → µ DCA distributions from HIJING [8] simulations using the full STAR Detector configuration. We then use DCA of muons from primary particles and those coming from weak decays of π/K (HIJING simulation) to fit the inclusive muons DCA spectra.…”

Section: Experiments and Analysismentioning

confidence: 99%

Scaling of the charm cross-section and modification of charm p_T spectra at RHIC

Chen

2007

J. Phys. G: Nucl. Part. Phys.

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Section: Experiments and Analysismentioning

confidence: 99%

Scaling of the charm cross-section and modification of charm p_T spectra at RHIC

Chen

2007

J. Phys. G: Nucl. Part. Phys.

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“…The AMPT model [20,21,[25][26][27]] is a hybrid model that uses minijet partons from hard processes and strings from soft processes in the Heavy Ion Jet Interaction Generator (HIJING) model [28] as the initial conditions for modeling heavy-ion collisions at ultra-relativistic energies. The time evolution of resulting minijet partons is described by Zhang's parton cascade (ZPC) [29] model.…”

Section: The Ampt Modelmentioning

confidence: 99%

Anisotropic flow inCu+Aucollisions atsNN=200GeV

Chen

2006

Phys. Rev. C

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The anisotropic flow of charged hadrons in asymmetric Cu + Au collisions at the Relativistic Heavy Ion Collider is studied in a multiphase transport model. Compared with previous results for symmetric Au + Au collisions, charged hadrons produced around midrapidity in asymmetric collisions are found to have a stronger directed flow v 1 and their elliptic flow v 2 is also more sensitive to the parton scattering cross section. Although higher order flows v 3 and v 4 are small at all rapidities, both v 1 and v 2 in these collisions are appreciable and show an asymmetry in forward and backward rapidities.

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“…Hard-scattering processes for Pb+Pb collisions were produced using PYTHIA event generator [16]. To correct Pb+Pb data sample from 2010, hard-scattering events were embedded into events produced by HIJING event generator [17]. To correct Pb+Pb data sample from 2011, real Pb+Pb events recorded for this purpose were used as underlying events.…”

Section: Discussionmentioning

confidence: 99%

Measurement of the charged-hadron spectra and nuclear modification factor in lead–lead collisions with the ATLAS detector

Balek

2016

Nuclear and Particle Physics Proceedings

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The ATLAS experiment at the Large Hadron Collider (LHC) measures charged hadron spectra obtained in 2010 and 2011 lead-lead LHC data taking periods with total integrated statistics of 0.15 nb −1 . The results are compared to the pp spectra of charged hadrons at the same centre-of-mass energy based on the data sample with integrated luminosity of 4.2 pb −1 obtained by the ATLAS experiment in 2011 and 2013. This allows a detailed comparison of the two collision systems in a wide transverse momentum (0.5 < pT < 150 GeV) and pseudorapidity (|η| < 2) ranges in different centrality intervals of Pb+Pb collision. The nuclear modification factor RAA is presented in detail as a function of centrality, pT and η. It shows a distinct pT-dependence with a pronounced minimum at about 7 GeV. Above 60 GeV, it is consistent with a flat, centrality-dependent, value within the uncertainties. The value is 0.55 ± 0.01(stat.) ± 0.04(syst.) in the most central collisions. The RAA is observed to be consistent with flat |η| dependence over the whole transverse momentum range in all centrality classes.

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hijing: A Monte Carlo model for multiple jet production inpp,pA, andAAcollisions

Cited by 1,756 publications

References 73 publications

Scaling of the charm cross-section and modification of charm p_T spectra at RHIC

Scaling of the charm cross-section and modification of charm p_T spectra at RHIC

Anisotropic flow inCu+Aucollisions atsNN=200GeV

Measurement of the charged-hadron spectra and nuclear modification factor in lead–lead collisions with the ATLAS detector

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hijing: A Monte Carlo model for multiple jet production inpp,pA, andAAcollisions

Cited by 1,756 publications

References 73 publications

Scaling of the charm cross-section and modification of charm pT spectra at RHIC

Scaling of the charm cross-section and modification of charm pT spectra at RHIC

Anisotropic flow inCu+Aucollisions atsNN=200GeV

Measurement of the charged-hadron spectra and nuclear modification factor in lead–lead collisions with the ATLAS detector

Contact Info

Product

Resources

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Scaling of the charm cross-section and modification of charm p_T spectra at RHIC

Scaling of the charm cross-section and modification of charm p_T spectra at RHIC