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[PDF] Top 20 Measurement of the centrality dependence of the charged-particle pseudorapidity distribution in proton–lead collisions at $\sqrt{s_{_\text {NN}}} = 5.02$  TeV with the ATLAS detector

Has 10000 "Measurement of the centrality dependence of the charged-particle pseudorapidity distribution in proton–lead collisions at $\sqrt{s_{_\text {NN}}} = 5.02$  TeV with the ATLAS detector" found on our website. Below are the top 20 most common "Measurement of the centrality dependence of the charged-particle pseudorapidity distribution in proton–lead collisions at $\sqrt{s_{_\text {NN}}} = 5.02$  TeV with the ATLAS detector".

Measurement of the centrality dependence of the charged-particle pseudorapidity distribution in proton–lead collisions at $\sqrt{s_{_\text {NN}}} = 5.02$  TeV with the ATLAS detector

Measurement of the centrality dependence of the charged-particle pseudorapidity distribution in proton–lead collisions at $\sqrt{s_{_\text {NN}}} = 5.02$  TeV with the ATLAS detector

... MES of Russia and NRC KI, Russian Feder- ation; JINR; MESTD, Serbia; MSSR, Slovakia; ARRS and MIZŠ, Slovenia; DST /NRF, South Africa; MINECO, Spain; SRC and Wallenberg Foundation, Sweden; SERI, SNSF and Cantons ... 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

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 = ...2. The ATLAS calorimeter system consists of a liquid argon ... 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

Centrality and rapidity dependence of inclusive jet production in $\sqrt{s_\mathrm{NN}} = 5.02$ TeV proton-lead collisions with the ATLAS detector

... 2.76 TeV protonproton collisions are ...measured in datasets corre- sponding to an integrated luminosity of ...recorded with the ATLAS detector ... See full document

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Measurement of long-range pseudorapidity correlations and azimuthal harmonics in $\sqrt{s_{NN}}=5.02$ TeV proton-lead collisions with the ATLAS detector

Measurement of long-range pseudorapidity correlations and azimuthal harmonics in $\sqrt{s_{NN}}=5.02$ TeV proton-lead collisions with the ATLAS detector

... In the offline analysis, p+Pb events are required to have a reconstructed vertex containing at least two associated offline tracks, with its z position satisfying |z vtx | < 150 ... See full document

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Transverse momentum, rapidity, and centrality dependence of inclusive charged-particle production in $\sqrt{s_{NN}}=5.02$ TeV $p$ + Pb collisions measured by the ATLAS experiment

Transverse momentum, rapidity, and centrality dependence of inclusive charged-particle production in $\sqrt{s_{NN}}=5.02$ TeV $p$ + Pb collisions measured by the ATLAS experiment

... is the number of primary charged particles and N Rec Primary is the number of reconstructed tracks that are matched to those charged ...generated particle if that ... See full document

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Measurement of the pseudorapidity and transverse momentum dependence of the elliptic flow of charged particles in lead-lead collisions at $\sqrt{s_{NN}}=2.76$ TeV with the ATLAS detector

Measurement of the pseudorapidity and transverse momentum dependence of the elliptic flow of charged particles in lead-lead collisions at $\sqrt{s_{NN}}=2.76$ TeV with the ATLAS detector

... studied in detail by comparing data to Monte Carlo simulations based on the HIJING event generator [11] and a full GEANT4 [12] simulation of the detector ...[13]. In general ... See full document

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Pseudorapidity distributions of charged hadrons in proton-lead collisions at $\sqrt{s_{_\mathrm{NN}}} =$ 5.02 and 8.16 TeV

Pseudorapidity distributions of charged hadrons in proton-lead collisions at $\sqrt{s_{_\mathrm{NN}}} =$ 5.02 and 8.16 TeV

... 1: The ∆η (a) and ∆φ (b, c) distributions of hit pairs for tracklets in pPb collisions at ...8.16 TeV (squares) and from MC simulations with the E POS and H IJING ... See full document

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Measurement of the correlation between flow harmonics of different order in lead-lead collisions at $\sqrt{s_{NN}}$=2.76 TeV with the ATLAS detector

Measurement of the correlation between flow harmonics of different order in lead-lead collisions at $\sqrt{s_{NN}}$=2.76 TeV with the ATLAS detector

... All of these are well suited for measurements of azimuthal anisotropies over a large pseudorapidity ...subsystems: the inner detector (ID) and the forward calorimeter ...(FCal). ... 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

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 leadlead collisions at √ s NN = ...2.76 TeV are shown using a dataset of approximately 7 µb −1 collected ... See full document

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Measurement of the azimuthal anisotropy for charged particle production in $\sqrt{s_{NN}}=2.76$ TeV lead-lead collisions with the ATLAS detector

Measurement of the azimuthal anisotropy for charged particle production in $\sqrt{s_{NN}}=2.76$ TeV lead-lead collisions with the ATLAS detector

... ideal detector, the combinatorial pair distribu- tion is uniform in ∆φ, and has a nearly triangular shape in ∆η due to the weak dependence of the ... 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

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

... by at least three charged-particle tracks recon- structed in the ...ID. The data were recorded at low instan- taneous luminosity where the probability of ... See full document

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Measurement of the centrality dependence of the charged particle pseudorapidity distribution in lead-lead collisions at $\sqrt{s_{NN}}=2.76$ TeV with the ATLAS detector

Measurement of the centrality dependence of the charged particle pseudorapidity distribution in lead-lead collisions at $\sqrt{s_{NN}}=2.76$ TeV with the ATLAS detector

... for the measurements presented here were collected with a minimum-bias ...coincidence in either the two minimum- bias trigger scintillator (MBTS) detectors, located at ...from ... See full document

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Measurement of the charged-particle multiplicity inside jets from $\sqrt{s}=8$ TeV $pp$ collisions with the ATLAS detector

Measurement of the charged-particle multiplicity inside jets from $\sqrt{s}=8$ TeV $pp$ collisions with the ATLAS detector

... Given the jet p T , the charged particle multiplicity inside jets does not vary significantly with ...that the solution to Eq. 1 reproduces the quark and gluon jet ... See full document

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Measurement of charged-particle event shape variables in $\sqrt{s}=7$ TeV proton-proton interactions with the ATLAS detector

Measurement of charged-particle event shape variables in $\sqrt{s}=7$ TeV proton-proton interactions with the ATLAS detector

... The measurement of charged-particle event shape variables is presented in inclusive inelastic pp collisions at a center-of-mass energy of 7 TeV ... See full document

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Measurement of $WZ$ production in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

Measurement of $WZ$ production in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

... in the direction of the fit parameter σ. The likelihood is maximized over the nuisance parameters for each ...σ. The systematic uncertainties include all sources except ... 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

Measurement of jet fragmentation in Pb+Pb and $pp$ collisions at $\sqrt{s_{NN}} = 5.02$ TeV with the ATLAS detector

... select the Pb+Pb and pp collisions. The first trigger level (L1) is hardware-based and implemented with custom ...electronics. The second level is the software-based high- level ... See full document

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Pseudorapidity distribution of charged hadrons in proton-proton collisions at $\sqrt{s}$ = 13 TeV

Pseudorapidity distribution of charged hadrons in proton-proton collisions at $\sqrt{s}$ = 13 TeV

... analysis of the recorded data is performed with two reconstruction techniques based on hits of charged particles detected by the CMS pixel ...pairs in different layers ... 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

Measurement of $Z$ boson Production in Pb+Pb Collisions at $\sqrt{s_{NN}}=2.76$ TeV with the ATLAS Detector

... studies of heavy ion (HI) collisions carried out by the experiments at the Relativistic Heavy Ion Col- lider (RHIC) at BNL, and the Large Hadron Collider (LHC) at ... See full document

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Measurements of the pseudorapidity dependence of the total transverse energy in proton-proton collisions at $\sqrt{s}=7$ TeV with ATLAS

Measurements of the pseudorapidity dependence of the total transverse energy in proton-proton collisions at $\sqrt{s}=7$ TeV with ATLAS

... acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Aus- tralia; BMWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, Chile; ... See full document

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Pseudorapidity dependence of long-range two-particle correlations in $p$Pb collisions at $\sqrt {s_{NN}}=$ 5.02 TeV

Pseudorapidity dependence of long-range two-particle correlations in $p$Pb collisions at $\sqrt {s_{NN}}=$ 5.02 TeV

... correlation measurement is performed using “trigger” and “associated” par- ticles as described in ...[45]. The trigger particles are defined as charged particles detected within a given p trig ... See full document

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