<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi mathvariant="italic">Z</mml:mi></mml:math>boson production in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi>p</mml:mi><mml:mo>+</mml:mo><mml:mi>Pb</mml:mi></mml:mrow></mml:math>collisions at<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:msqrt><mml:msub><mml:mi>s</mml:mi><mml:mi mathvariant="italic">NN</mml:mi></mml:msub></mml:msqrt><mml:mo>=</mml:mo><mml:mn>5.02</mml:mn></mml:mrow></mml:mat

Abulaiti, Y.; Akerstedt, H.; Åsman, B.; Bendtz, K.; Bertoli, G.; Bylund, O. Bessidskaia; Böhm, C.; Clément, C.; Cribbs, W. A.; Hellman, S.; Jon‐And, K.; Khandanyan, H.; Kim, Heyon; Klimek, P.; Lundberg, O.; Milstead, D. A.; Moa, T.; Molander, S.; Pani, P.; Petridis, A.; Pluciński, P.; Pöttgen, Ruth; Rossetti, V.; Shcherbakova, A.; Silverstein, S. B.; Sjölin, J.; Strandberg, S.; Tylmad, M.; Ughetto, M.

doi:10.1103/physrevc.92.044915

Cited by 78 publications

(107 citation statements)

References 43 publications

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“…4. Again, the HYDJET++ model predicts a steeper slope of v 3 -v 4 correlation than the experimental data [32]. Similarly to the case of the v 2 -v 4 correlation, the AMPT model reproduces the…”

Section: Resultsmentioning

confidence: 59%

“…This introduces the like shape of the correlation. However, the boomerang turn is much sharper than the one seen in the ATLAS data [32] (see the zoomed plot in the Fig. 2).…”

Section: Resultsmentioning

confidence: 71%

“…2. In contrast to the v 2 , higher order Fourier harmonics v n (n = 3, 4) have a weak centrality dependence and in peripheral collisions they decrease faster than in central collisions as measured by ATLAS [32]. This introduces the like shape of the correlation.…”

Section: Resultsmentioning

confidence: 93%

“…Centrality dependencies of the Fourier harmonics v 2 , v 3 and v 4 from PbPb collisions at √ s NN = 2.76 TeV simulated by the HYDJET++ and AMPT models are shown in Fig. 1 together with the experimental data from the ATLAS Collaboration [32]. In both models, the elliptic v 2 harmonic exhibits a strong centrality dependence, while the v 3 and v 4 have a weak centrality dependence.…”

Section: Resultsmentioning

confidence: 98%

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Correlations between azimuthal anisotropy Fourier harmonics in PbPb collisions at sNN=2.76 TeV in the HYDJET++ model and in the multiphase tran

Dordevic¹,

Milošević

Nađđerđ³

et al. 2020

Phys. Rev. C

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Correlations between azimuthal anisotropy Fourier harmonics v n (n = 2, 3, 4) are studied using the events from PbPb collisions at √ s NN = 2.76 TeV generated by the HYDJET++ and AMPT models, and compared to the corresponding experimental results obtained by the ATLAS Collaboration. The Fourier harmonics v n are measured over a wide centrality range using the two-particle azimuthal correlation method. The slopes of the v 2 -v 3 correlation from both models are in a good agreement with the ATLAS data. The HYDJET++ model predicts a stronger slope for the v 2 -v 4and v 3 -v 4 correlations than the ones experimentally measured, while the results from the AMPT model are in a rather good agreement with the experimental results. In contrast to the HYD-JET++ predictions, the AMPT model predicts a boomerang-like shape in the structure of the correlations as found in the experimental data.

show abstract

Section: Resultsmentioning

confidence: 59%

“…This introduces the like shape of the correlation. However, the boomerang turn is much sharper than the one seen in the ATLAS data [32] (see the zoomed plot in the Fig. 2).…”

Section: Resultsmentioning

confidence: 71%

Section: Resultsmentioning

confidence: 93%

Section: Resultsmentioning

confidence: 98%

See 2 more Smart Citations

Correlations between azimuthal anisotropy Fourier harmonics in PbPb collisions at sNN=2.76 TeV in the HYDJET++ model and in the multiphase tran

Dordevic¹,

Milošević

Nađđerđ³

et al. 2020

Phys. Rev. C

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show abstract

“…The DSSZ analysis not only uses the l ± /µ−DIS data sets and p+A DY data sets, but also firstly includes the inclusive pion production in the deutron and gold collisions at PHENIX to constrain the nuclear gluon PDF. The EPPS16 [35] is the extension of the previous EPS09 [36] with the additional experimental data from proton-lead collisions at LHC [37][38][39] for the first time. It offers a less biased and flavor-dependent fitting analysis for nuclear PDFs.…”

Section: Introductionmentioning

confidence: 99%

Probing cold nuclear matter effects with the productions of isolated- ${\gamma} $ and ${\gamma} $+jet in p+Pb collisions at ${\sqrt{{s}_{{NN}}}}= $ 8.16 TeV

Ma¹,

Dai²,

Zhang³

2019

Chinese Phys. C

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We investigate the cold nuclear matter (CNM) effects on the productions of the isolated prompt photon and γ+jet in proton-lead collisions at 8.16 TeV under the next-to-leading order (NLO) perturbative quantum chromodynamics calculations with four parametrizations for nuclear parton distribution functions (nPDFs), i.e. DSSZ, EPPS16, nCTEQ15, nIMParton. Our theoretical calculations provide good descriptions of pp baseline in the ATLAS collaboration and make predictions for future experimental results at p+Pb collisions. We calculate the dependence of the nuclear modification factor of isolated prompt photon on transverse momentum p γ T and pseudo-rapidity η γ at very forward and backward rapidity regions, and demonstrate that the forward-to-backward yield asymmetries Y asym pPb as a function of p γ T with different nPDFs parametrizations have diverse behaviors. Furthermore, the nuclear modification factor of isolated-γ+jet R γJet pPb as a function of γ+jet's pseudo-rapidity ηγJet = 1 2 (ηγ + ηJet) at different average transverse momentum p avg T = 1 2 (p γ T + p Jet T ) has been discussed, which can facilitate a tomography study of CNM effects with precise locations in a rather wide kinematic region by varying the transverse momenta and rapidities of both isolated photon and jet in p+A collisions.

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W and Z boson production in p-Pb collisions at s N N = 5.02 $$ \sqrt{s_{\mathrm{NN}}}=5.02 $$ TeV

Adam¹,

Adamová²,

Aggarwal³

et al. 2017

J. High Energ. Phys.

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The W and Z boson production was measured via the muonic decay channel in proton-lead collisions at √ s NN = 5.02 TeV at the Large Hadron Collider with the ALICE detector. The measurement covers backward (−4.46 < y cms < −2.96) and forward (2.03 < y cms < 3.53) rapidity regions, corresponding to Pb-going and p-going directions, respectively. The Z-boson production cross section, with dimuon invariant mass of 60 < m µµ < 120 GeV/c 2 and muon transverse momentum (p µ T ) larger than 20 GeV/c, is measured. The production cross section and charge asymmetry of muons from W-boson decays with p µ T > 10 GeV/c are determined. The results are compared to theoretical calculations both with and without including the nuclear modification of the parton distribution functions. The W-boson production is also studied as a function of the collision centrality: the cross section of muons from W-boson decays is found to scale with the average number of binary nucleon-nucleon collisions within uncertainties.

show abstract

Zboson production inp+Pbcollisions atsNN=5.02

Cited by 78 publications

References 43 publications

Correlations between azimuthal anisotropy Fourier harmonics in PbPb collisions at sNN=2.76 TeV in the HYDJET++ model and in the multiphase tran

Correlations between azimuthal anisotropy Fourier harmonics in PbPb collisions at sNN=2.76 TeV in the HYDJET++ model and in the multiphase tran

Probing cold nuclear matter effects with the productions of isolated- ${\gamma} $ and ${\gamma} $+jet in p+Pb collisions at ${\sqrt{{s}_{{NN}}}}= $ 8.16 TeV

W and Z boson production in p-Pb collisions at s N N = 5.02 $$ \sqrt{s_{\mathrm{NN}}}=5.02 $$ TeV

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