[PDF] Top 20 Measurement of forward-backward multiplicity correlations in lead-lead, proton-lead, and proton-proton collisions with the ATLAS detector
Has 10000 "Measurement of forward-backward multiplicity correlations in lead-lead, proton-lead, and proton-proton collisions with the ATLAS detector" found on our website. Below are the top 20 most common "Measurement of forward-backward multiplicity correlations in lead-lead, proton-lead, and proton-proton collisions with the ATLAS detector".
Measurement of forward-backward multiplicity correlations in lead-lead, proton-lead, and proton-proton collisions with the ATLAS detector
... MOST and NSFC, China; COLCIENCIAS, Colombia; MSMT CR, MPO CR and VSC CR, Czech Republic; DNRF and DNSRC, Denmark; IN2P3-CNRS, CEA-DSM/IRFU, France; GNSF, Georgia; BMBF, HGF, and MPG, Germany; ... See full document
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Measurement of jet fragmentation in 5.02 TeV proton-lead and proton-proton collisions with the ATLAS detector
... acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWFW and FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, ... See full document
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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
... dependence of the mean charged-particle multiplicity as a function of pseu- dorapidity is measured in approximately 1 µb −1 of proton–lead collisions at a ... See full document
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Measurement of the inclusive jet cross-sections in proton-proton collisions at $ \sqrt{s}=8 $ TeV with the ATLAS detector
... through the unfolding procedure using an ensemble of pseudo- ...pseudo-experiment in the ensemble, a weight fluctuated according to a Poisson distribution with a mean value equal to one ... 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
... particle multiplicity in Pb+Pb collisions can generate misidentified tracks and/or two-point tracklets when only two or three mea- surements are made on each ...trajectory. The ... See full document
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Measurement of the exclusive $\gamma \gamma \rightarrow \mu^+ \mu^-$ process in proton-proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
... Following the procedure described in Refs. [3,48] , the shape of the charged-particle multiplicity distribution in simulated DY events is reweighted to match the ... See full document
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Measurement of the $ t\overline{t} $ production cross-section as a function of jet multiplicity and jet transverse momentum in 7 TeV proton-proton collisions with the ATLAS detector
... details of the fragmentation differ between jets initiated by quarks and those initiated by gluons [ 25 ], the respective jet energy scale also differs ...However, the in situ ... 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
... TeV proton–proton collisions are ...measured in datasets corre- sponding to an integrated luminosity of ...−1 and 4.0 pb −1 , respectively, recorded with the ... See full document
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Measurement of the inelastic cross section in proton–lead collisions at $\sqrt {s_{NN}}=$ 5.02 TeV
... The measurement presented here is based on pPb data taken with the CMS experiment at the LHC at the beginning of ...description of the apparatus can be found ... See full document
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Measurement of inclusive jet and dijet cross-sections in proton-proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
... The ATLAS experiment [ 19 , 20 ] at the LHC is a multi-purpose particle detector with a forward-backward symmetric cylindrical geometry and a near 4π coverage ... See full document
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Jet energy measurement and its systematic uncertainty in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
... given in Eq. ( 13 ) for the di- rect balance in Z–jet events, the MPF technique in γ–jet events, and the multijet balance method are combined as described in ... See full document
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Search for excited leptons in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
... multi-purpose detector with a forward- backward symmetric cylindrical geometry and nearly 4π coverage in solid ...consists of an inner track- ing detector immersed ... See full document
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Measurement of the distributions of event-by-event flow harmonics in lead-lead collisions at = 2.76 TeV with the ATLAS detector at the LHC
... subsystems: the inner detector (ID) and the forward calorimeter ...(FCal). The ID is immersed in the 2 T axial field of a superconducting solenoid magnet, ... See full document
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Search for excited electrons and muons in $\sqrt{s}$=8 TeV proton-proton collisions with the ATLAS detector
... The ATLAS detector [20] consists of an inner tracking system surrounded by a superconducting solenoid, electromagnetic and hadronic calorimeters, and a muon ...a ... See full document
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Measurement of the production of neighbouring jets in lead–lead collisions at $\sqrt{s_{\mathrm{NN}}} = 2.76$TeV with the ATLAS detector
... compartments with an ad- ditional pre-sampler layer. The forward regions are instrumented with copper/LAr and tungsten/LAr forward calorimeters (FCal) covering ...electromagnetic ... See full document
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Measurement of exclusive $\gamma\gamma\rightarrow \ell^+\ell^-$ production in proton-proton collisions at $\sqrt{s} = 7$ TeV with the ATLAS detector
... The ATLAS experiment [ 20 ] at the LHC is a multi-purpose particle detector with a forward-backward symmetric cylindrical geometry and nearly 4π coverage in ... See full document
34
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
... calorimeters and muon chambers. All of these are well suited for measurements of azimuthal anisotropies over a large pseudorapidity ...subsystems: the inner detector (ID) and ... See full document
35
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 using the ... 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
... barrel and endcap electromagnetic calorimeters (ECal) and the forward calorimeter ...(FCal). The ID is contained within the 2 T field of a superconducting solenoid mag- ... See full document
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Observation of Associated Near-Side and Away-Side Long-Range Correlations in $\sqrt{s_{NN}}$=5.02 TeV Proton-Lead Collisions with the ATLAS Detector
... hodoscopes of 16 counters posi- tioned at z = ±3.6 m. The FCal consists of two sections that cover ...4.9. The FCal modules are com- posed of tungsten and copper absorbers ... See full document
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