[PDF] Top 20 Measurement of event-plane correlations in $\sqrt{s_{NN}}=2.76$ TeV lead-lead collisions with the ATLAS detector
Has 10000 "Measurement of event-plane correlations in $\sqrt{s_{NN}}=2.76$ TeV lead-lead collisions with the ATLAS detector" found on our website. Below are the top 20 most common "Measurement of event-plane correlations in $\sqrt{s_{NN}}=2.76$ TeV lead-lead collisions with the ATLAS detector".
Measurement of event-plane correlations in $\sqrt{s_{NN}}=2.76$ TeV lead-lead collisions with the ATLAS detector
... acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWF and FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, ... See full document
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Measurement of jet $p_{\mathrm{T}}$ correlations in Pb+Pb and $pp$ collisions at $\sqrt{s_{\mathrm{NN}}}=$ 2.76 TeV with the ATLAS detector
... ing the matter produced in ultra-relativistic heavy-ion ...collisions. In these collisions, a hot medium of deconfined colour charges is produced, known as the quark–gluon ... See full document
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Measurement of the azimuthal anisotropy of charged particles produced in $\sqrt{s_{_\text {NN}}}$ = 5.02 TeV Pb+Pb collisions with the ATLAS detector
... ]. The MBTS system detects charged particles over ...side of the detector, positioned at z = ...Run 2. The ATLAS calorimeter system consists of a liquid argon (LAr) ... See full document
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Measurement of flow harmonics with multi-particle cumulants in Pb+Pb collisions at $\sqrt{s_{\mathrm {NN}}}=2.76$ TeV with the ATLAS detector
... measurements of the azimuthal anisotropy in lead–lead collisions at √ s NN = ...2.76 TeV are shown using a dataset of approximately 7 µb −1 collected at ... See full document
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Measurement of inclusive jet charged-particle fragmentation functions in Pb+Pb collisions at $\sqrt{s_{NN}}=2.76$ TeV with the ATLAS detector
... acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWFW and FWF, Austria; ANAS, Azerbai- jan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CON- ... See full document
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Measurement of jet fragmentation in Pb+Pb and $pp$ collisions at $\sqrt{s_{NN}} = 5.02$ TeV with the ATLAS detector
... contribution of reconstructed tracks which are not be matched to a generated primary particle in the MC samples of pp collision events produced without data overlay, along with ... See full document
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Measurement of $Z$ boson Production in Pb+Pb Collisions at $\sqrt{s_{NN}}=2.76$ TeV with the ATLAS Detector
... by the high-level trigger (HLT). The L1 muon algorithm also identified regions of interest (RoI) within the detector to be investigated by the ...HLT. In the HLT, ... See full document
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Centrality, rapidity and transverse momentum dependence of isolated prompt photon production in lead-lead collisions at $\sqrt{s_{\mathrm{NN}}} = 2.76$ TeV measured with the ATLAS detector
... performed. The first reweights the contributions from up and down valence quarks to account for the neutrons in the colliding lead nuclei, but with no attempt at modeling ... See full document
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Centrality and rapidity dependence of inclusive jet production in $\sqrt{s_\mathrm{NN}} = 5.02$ TeV proton-lead collisions with the ATLAS detector
... C. Di Donato 103a,103b , A. Di Girolamo 30 , B. Di Girolamo 30 , A. Di Mattia 153 , B. Di Micco 135a,135b , R. Di Nardo 47 , A. Di Simone 48 , R. Di Sipio 20a,20b , D. Di Valentino 29 , F.A. Dias 46 , M.A. Diaz 32a , ... See full document
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Measurement of longitudinal flow decorrelations in Pb+Pb collisions at $\sqrt{s_{\text {NN}}}=2.76$ and 5.02 TeV with the ATLAS detector
... D.E. Ferreira de Lima 60b , A. Ferrer 170 , D. Ferrere 52 , C. Ferretti 92 , F. Fiedler 86 , A. Filipˇciˇc 78 , M. Filipuzzi 45 , F. Filthaut 108 , M. Fincke-Keeler 172 , K.D. Finelli 24 , M.C.N. Fiolhais 128a,128c,r , ... See full document
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Studies of azimuthal dihadron correlations in ultra-central PbPb collisions at $\sqrt{s_{NN}} =$ 2.76 TeV
... extraction of η/s from the anisotropy data is crucial for investigating the transport prop- erties of the hot and dense medium created in heavy-ion collisions in ... See full document
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Measurement of the suppression and azimuthal anisotropy of muons from heavy-flavor decays in Pb+Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 2.76$ TeV with the ATLAS detector
... E. Valdes Santurio 43a,43b , M. Valente 52 , S. Valentinetti 23b,23a , A. Valero 172 , L. Valéry 44 , R.A. Vallance 21 , A. Vallier 5 , J.A. Valls Ferrer 172 , T.R. Van Daalen 14 , W. Van Den Wollenberg 118 , H. Van der ... See full document
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Measurement of jet fragmentation in PbPb and pp collisions at $\sqrt{s_{NN}}=2.76$ TeV
... background. The full difference between the two background subtraction methods is quoted conservatively as the uncertainty in the fragmentation function due to background sub- ...to ... See full document
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Measurement of the azimuthal anisotropy of neutral pions in PbPb collisions at $\sqrt{s_{NN}}=2.76$ TeV
... subtracting the combinatorial background from the π 0 candidate invariant mass ...distribution. The combinatorial background is estimated and subtracted using an event mixing technique, which ... See full document
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Measurements of the Nuclear Modification Factor for Jets in Pb+Pb Collisions at $\sqrt{s_{\mathrm{NN}}}=2.76$ TeV with the ATLAS Detector
... ues of the jet rapidity [ 14 ]. Thus measurements of jet suppression for jets in different intervals of rapidity pro- vide complementary information about the energy ...and ... See full document
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Measurement of charged-particle spectra in Pb+Pb collisions at $\sqrt{{s}_\mathsf{{NN}}} = 2.76$ TeV with the ATLAS detector at the LHC
... presented in this paper were performed using the ATLAS inner de- tector (ID), calorimeter, muon spectrometer, and the high-level trigger and data acquisition systems ...[19]. The ID ... See full document
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Measurement of the Azimuthal Angle Dependence of Inclusive Jet Yields in Pb+Pb Collisions at $\sqrt{s_{NN}}=$ 2.76 TeV with the ATLAS detector
... produced with the PYTHIA event generator [31] ver- sion ...using the AUET2B tune [32] and overlaid on minimum-bias Pb+Pb collisions recorded by ...procedure, the MC sample con- ... See full document
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$Z$ boson production in $p+$Pb collisions at $\sqrt{s_{NN}}=5.02$ TeV measured with the ATLAS detector
... uses the 2013 ATLAS p +Pb collision data at √ s NN = 5.02 TeV, produced from a 4 TeV proton beam and a ...1.57 TeV per nucleon lead beam. The asymmetric energy ... See full document
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Measurement of jet fragmentation in Pb+Pb and $pp$ collisions at $\sqrt{{s_\mathrm{NN}}} = 2.76$ TeV with the ATLAS detector at the LHC
... M. Ishino 157 , M. Ishitsuka 159 , C. Issever 122 , S. Istin 20a , F. Ito 164 , J.M. Iturbe Ponce 87 , R. Iuppa 162a,162b , H. Iwasaki 69 , J.M. Izen 44 , V. Izzo 106a , S. Jabbar 3 , P. Jackson 1 , V. Jain 2 , ... See full document
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Measurement of the centrality and pseudorapidity dependence of the integrated elliptic flow in lead-lead collisions at $\sqrt{s_{\mathrm {NN}}}=2.76$ TeV with the ATLAS detector
... (MC) event samples were used to deter- mine the tracking efficiencies and the rates of fake ...tracks. The HIJING event generator [25] was used to produce minimum-bias Pb+Pb ... See full document
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