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[PDF] Top 20 Measurement of charged-particle spectra in Pb+Pb collisions at $\sqrt{{s}_\mathsf{{NN}}} = 2.76$ TeV with the ATLAS detector at the LHC

Has 10000 "Measurement of charged-particle spectra in Pb+Pb collisions at $\sqrt{{s}_\mathsf{{NN}}} = 2.76$ TeV with the ATLAS detector at the LHC" found on our website. Below are the top 20 most common "Measurement of charged-particle spectra in Pb+Pb collisions at $\sqrt{{s}_\mathsf{{NN}}} = 2.76$ TeV with the ATLAS detector at the LHC".

Measurement of charged-particle spectra in Pb+Pb collisions at $\sqrt{{s}_\mathsf{{NN}}} = 2.76$ TeV with the ATLAS detector at the LHC

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

57

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

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

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Measurement of the production and lepton charge asymmetry of $W$ bosons in Pb+Pb collisions at $\mathbf {\sqrt{\mathbf {s}_{\mathrm {\mathbf {NN}}}}=2.76\;TeV}$ with the ATLAS detector

Measurement of the production and lepton charge asymmetry of $W$ bosons in Pb+Pb collisions at $\mathbf {\sqrt{\mathbf {s}_{\mathrm {\mathbf {NN}}}}=2.76\;TeV}$ with the ATLAS detector

... N.A. Styles 42 , D. Su 144 , J. Su 124 , R. Subramaniam 78 , A. Succurro 12 , Y. Sugaya 117 , C. Suhr 107 , M. Suk 127 , V.V. Sulin 95 , S. Sultansoy 4c , T. Sumida 67 , S. Sun 57 , X. Sun 33a , J.E. ... See full document

33

Measurement of the elliptic anisotropy of charged particles produced in PbPb collisions at $\sqrt{s}_{NN}$=2.76 TeV

Measurement of the elliptic anisotropy of charged particles produced in PbPb collisions at $\sqrt{s}_{NN}$=2.76 TeV

... measure the azimuthal correlations of the particles produced in heavy- ion collisions in relation to the initial geometry of the ...Originally, the ... See full document

63

$Z$ boson production in $p+$Pb collisions at $\sqrt{s_{NN}}=5.02$ TeV measured with the ATLAS detector

$Z$ 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 ats NN = ...5.02 TeV, produced from a 4 TeV proton beam and a 1.57 TeV per nucleon lead ...beam. The ... See full document

36

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

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

24

Measurements of the Nuclear Modification Factor for Jets in Pb+Pb Collisions at $\sqrt{s_{\mathrm{NN}}}=2.76$ TeV with the ATLAS Detector

Measurements of the Nuclear Modification Factor for Jets in Pb+Pb Collisions at $\sqrt{s_{\mathrm{NN}}}=2.76$ TeV with the ATLAS Detector

... resulting in the phenomenon of “jet quenching.” The partonic energy loss can be probed through measurements of the suppression of jet production ...rates. The ... See full document

20

Measurement of charged-particle distributions sensitive to the underlying event in $ \sqrt{s}=13 $ TeV proton-proton collisions with the ATLAS detector at the LHC

Measurement of charged-particle distributions sensitive to the underlying event in $ \sqrt{s}=13 $ TeV proton-proton collisions with the ATLAS detector at the LHC

... observables the models describe the underlying-event data to better than 5% ...level of variation is far greater than the experimental uncertainty of the measurements, and there ... See full document

40

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

... A. Loginov 177 , C.W. Loh 169 , T. Lohse 16 , K. Lohwasser 48 , M. Lokajicek 126 , V.P. Lombardo 5 , J.D. Long 88 , R.E. Long 71 , L. Lopes 125a , D. Lopez Mateos 57 , B. Lopez Paredes 140 , J. Lorenz 99 , N. Lorenzo ... See full document

46

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 single-particle ... See full document

47

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

... This measurement uses the dataset of pp collisions recorded by the ATLAS detector in 2012, corre- sponding to an integrated luminosity of ...−1 at a ... See full document

35

Measurement of the Inelastic Proton-Proton Cross Section at $\sqrt{s} = 13$  TeV with the ATLAS Detector at the LHC

Measurement of the Inelastic Proton-Proton Cross Section at $\sqrt{s} = 13$  TeV with the ATLAS Detector at the LHC

... Sources of background include interactions between the beam and residual gas in the beam pipe; inter- actions between the beam and collimators upstream of the ... See full document

30

Measurement of inclusive two-particle angular correlations in pp collisions with the ATLAS detector at the LHC

Measurement of inclusive two-particle angular correlations in pp collisions with the ATLAS detector at the LHC

... functions in ∆η and ∆φ have been measured using charged particles with p T > 100 MeV and |η| < ...by the ATLAS detector at the LHC from proton-proton ... See full document

47

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

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

... 2.76 TeV pp collisions at the LHC. The measurements are performed over the transverse momentum range of 4 < p T < 14 ...from in-flight pion and kaon ... See full document

55

Measurement of the ${B}^{\pm}$ Meson Nuclear Modification Factor in Pb-Pb Collisions at $\sqrt{{s}_{NN}}=5.02\text{ }\text{ }\mathrm{TeV}$

Measurement of the ${B}^{\pm}$ Meson Nuclear Modification Factor in Pb-Pb Collisions at $\sqrt{{s}_{NN}}=5.02\text{ }\text{ }\mathrm{TeV}$

... collected with the same trigger during the pp and PbPb data taking, requiring the presence of two muon candidates, with no explicit momentum ...For the offline anal- ysis, ... See full document

30

Measurement of event-shape observables in $Z \rightarrow \ell ^{+} \ell ^{-}$ events in $pp$ collisions at $\sqrt{s}=$ 7 TeV with the ATLAS detector at the LHC

Measurement of event-shape observables in $Z \rightarrow \ell ^{+} \ell ^{-}$ events in $pp$ collisions at $\sqrt{s}=$ 7 TeV with the ATLAS detector at the LHC

... Since the UE is dominated by low-scale strong-force interactions, in which the strong coupling strength diverges and perturbative methods of quantum chromodynamics (QCD) lose predictivity, it ... See full document

53

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

... detector at the LHC. These measurements provide insight into the jet quenching process in the quark–gluon plasma created in the aftermath of ... See full document

56

Measurement of inclusive jet charged-particle fragmentation functions in Pb+Pb collisions at $\sqrt{s_{NN}}=2.76$ TeV with the ATLAS detector

Measurement of inclusive jet charged-particle fragmentation functions in Pb+Pb collisions at $\sqrt{s_{NN}}=2.76$ TeV with the ATLAS detector

... energies of calorimeter cells within the tower ...estimate. The UE energy was subtracted from each calorimeter cell within the towers included in the reconstructed ...jet. ... See full document

32

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 = ...Run 2. The ATLAS calorimeter system consists of a ... See full document

50

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

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

... E. von Toerne 23 , V. Vorobel 131 , K. Vorobev 100 , M. Vos 170 , R. Voss 32 , J.H. Vossebeld 77 , N. Vranjes 14 , M. Vranjes Milosavljevic 14 , V. Vrba 130 , M. Vreeswijk 109 , R. Vuillermet 32 , I. Vukotic 33 , P. ... See full document

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