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[PDF] Top 20 Measurement of the dependence of transverse energy production at large pseudorapidity on the hard-scattering kinematics of proton-proton collisions at $\sqrt{s} = 2.76$ TeV with ATLAS

Has 10000 "Measurement of the dependence of transverse energy production at large pseudorapidity on the hard-scattering kinematics of proton-proton collisions at $\sqrt{s} = 2.76$ TeV with ATLAS" found on our website. Below are the top 20 most common "Measurement of the dependence of transverse energy production at large pseudorapidity on the hard-scattering kinematics of proton-proton collisions at $\sqrt{s} = 2.76$ TeV with ATLAS".

Measurement of the dependence of transverse energy production at large pseudorapidity on the hard-scattering kinematics of proton-proton collisions at $\sqrt{s} = 2.76$ TeV with ATLAS

Measurement of the dependence of transverse energy production at large pseudorapidity on the hard-scattering kinematics of proton-proton collisions at $\sqrt{s} = 2.76$ TeV with ATLAS

... J.K. Nilsen 119 , P. Nilsson 25 , Y. Ninomiya 155 , A. Nisati 132a , R. Nisius 101 , T. Nobe 155 , L. Nodulman 6 , M. Nomachi 118 , I. Nomidis 29 , T. Nooney 76 , S. Norberg 113 , M. Nordberg 30 , O. ... See full document

33

Performance of missing transverse momentum reconstruction with the ATLAS detector using proton-proton collisions at $\sqrt{s}$ = 13 TeV

Performance of missing transverse momentum reconstruction with the ATLAS detector using proton-proton collisions at $\sqrt{s}$ = 13 TeV

... missing transverse momentum (E T miss ) is an important observable serving as an experimental proxy for the transverse momentum carried by undetected particles produced in protonproton ... See full document

66

Measurement of pseudorapidity distributions of charged particles in proton-proton collisions at $\sqrt{s}$ = 8 TeV by the CMS and TOTEM experiments

Measurement of pseudorapidity distributions of charged particles in proton-proton collisions at $\sqrt{s}$ = 8 TeV by the CMS and TOTEM experiments

... 0.49 at η = 5.375 and 2.61 ± 0.28 at η = 6.350, with negligible statistical uncer- ...tainty. The pseudorapidity density of the NSD-enhanced sample ranges between ...for ... See full document

39

Measurement of the pseudorapidity and centrality dependence of the transverse energy density in PbPb collisions at $\sqrt{s_{NN}}=2.76$ TeV

Measurement of the pseudorapidity and centrality dependence of the transverse energy density in PbPb collisions at $\sqrt{s_{NN}}=2.76$ TeV

... In the analysis at least two reconstructed tracks were required to form a ver- tex within ± 25 cm of the nominal interaction point along the beam line and within a radius of ... See full document

27

Measurement of the transverse polarization of $\Lambda$ and $\bar{\Lambda}$ hyperons produced in proton-proton collisions at $\sqrt{s}=7$ TeV using the ATLAS detector

Measurement of the transverse polarization of $\Lambda$ and $\bar{\Lambda}$ hyperons produced in proton-proton collisions at $\sqrt{s}=7$ TeV using the ATLAS detector

... in the pseudorapidity range of |η| < 2.5. The ID consists of two types of silicon detectors (pixel and microstrip) and a gas-filled detector with a transition radiation ... See full document

23

Measurement of $W^+W^-$ production in association with one jet in proton--proton collisions at $\sqrt{s} =8$ TeV with the ATLAS detector

Measurement of $W^+W^-$ production in association with one jet in proton--proton collisions at $\sqrt{s} =8$ TeV with the ATLAS detector

... signature of exactly one electron and one muon with opposite electric charge, and missing transverse momentum can be produced by a variety of SM processes which are treated as back- ... See full document

34

Measurement of the production cross section of an isolated photon associated with jets in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

Measurement of the production cross section of an isolated photon associated with jets in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

... system. The first level trigger (level- 1) is hardware based: using a trigger cell granularity ...that of the electromag- netic calorimeter, it searches for electromagnetic clus- ters within a fixed ... See full document

34

Measurement of the inclusive jet cross-sections in proton-proton collisions at $ \sqrt{s}=8 $ TeV with the ATLAS detector

Measurement of the inclusive jet cross-sections in proton-proton collisions at $ \sqrt{s}=8 $ TeV with the ATLAS detector

... The ATLAS experiment [ 27 ] at the LHC is a multipurpose particle detector with a forward-backward symmetric cylindrical geometry and a near 4π coverage in solid ...consists of ... See full document

56

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

... centrality 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 ... See full document

46

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 muon spectrometer to tracks re- constructed in the inner ...detector. The momentum of the combined muon track is calculated from the mo- menta of the two ... See full document

27

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

... in the dijet data; this feature is discussed below. Figure 5 shows the ratio of the E T density in the dijet transverse region to the E T density in minimum bias ... See full document

56

Measurement of inclusive jet and dijet cross-sections in proton-proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

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 in solid ...consists ... See full document

48

Measurement of the inclusive energy spectrum in the very forward direction in proton-proton collisions at $ \sqrt{s}=13 $ TeV

Measurement of the inclusive energy spectrum in the very forward direction in proton-proton collisions at $ \sqrt{s}=13 $ TeV

... detectors of CMS are complemented by calorimeters in the forward direction, which all rely on the detection of Cherenkov photons produced when charged particles pass through their ... See full document

30

Measurement of the transverse momentum and $\phi ^*_{\eta }$ distributions of Drell–Yan lepton pairs in proton–proton collisions at $\sqrt{s}=8$  TeV with the ATLAS detector

Measurement of the transverse momentum and $\phi ^*_{\eta }$ distributions of Drell–Yan lepton pairs in proton–proton collisions at $\sqrt{s}=8$  TeV with the ATLAS detector

... 1: The distribution of events passing the selection requirements in the electron-pair channel as a function of dilepton invariant mass m `` (left) and electron pseudorapidity η ... See full document

77

Measurement of the inelastic proton-proton cross section at $ \sqrt{s}=13 $ TeV

Measurement of the inelastic proton-proton cross section at $ \sqrt{s}=13 $ TeV

... by the presence of both beams in the interaction point (“zero bias”), signaled by beam pick-up monitors located at ± 175 m from the interaction ...requiring the presence ... See full document

30

Measurement of the inelastic proton-proton cross section at $\sqrt{s}=7$ TeV

Measurement of the inelastic proton-proton cross section at $\sqrt{s}=7$ TeV

... G. Cerminara, T. Christiansen, J.A. Coarasa Perez, D. D’Enterria, A. Dabrowski, A. De Roeck, S. Di Guida, M. Dobson, N. Dupont-Sagorin, A. Elliott-Peisert, B. Frisch, W. Funk, G. Georgiou, M. Giffels, D. Gigi, K. ... See full document

33

Search for bottom squark pair production in proton–proton collisions at $\sqrt{s}=13$  TeV with the ATLAS detector

Search for bottom squark pair production in proton–proton collisions at $\sqrt{s}=13$  TeV with the ATLAS detector

... P.B. Shatalov 97 , K. Shaw 163a,163b , S.M. Shaw 85 , A. Shcherbakova 146a,146b , C.Y. Shehu 149 , P. Sherwood 79 , L. Shi 151,ak , S. Shimizu 68 , C.O. Shimmin 162 , M. Shimojima 102 , M. Shiyakova 66 ,al , A. ... See full document

37

Performance of Missing Transverse Momentum Reconstruction in Proton-Proton Collisions at 7 TeV with ATLAS

Performance of Missing Transverse Momentum Reconstruction in Proton-Proton Collisions at 7 TeV with ATLAS

... The ATLAS detector [1] is a multipurpose particle physics ap- paratus with a forward-backward symmetric cylindrical geom- etry and near 4 π coverage in solid ...angle. The inner tracking ... See full document

33

Search for excited leptons in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

Search for excited leptons in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

... (SM) of particle physics is an extremely successful effective theory which has been ex- tensively tested over the past forty ...number of fundamental questions are left unanswered. In particular, ... See full document

22

Search for tb resonances in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

Search for tb resonances in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

... using the HERWIG v6.5 MC generator and their cross sections are obtained at NLO using the MCFM [25] pro- gram with the MSTW2008 ...PDFs. The MC samples sim- ulated with ... See full document

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