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[PDF] Top 20 Measurement of the top quark pair production cross section in $pp$ collisions at $\sqrt{s}=7$ TeV in dilepton final states with ATLAS

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Measurement of the top quark pair production cross section in $pp$ collisions at $\sqrt{s}=7$ TeV in dilepton final states with ATLAS

Measurement of the top quark pair production cross section in $pp$ collisions at $\sqrt{s}=7$ TeV in dilepton final states with ATLAS

... R.J. Madaras 14 , W.F. Mader 43 , R. Maenner 58c , T. Maeno 24 , P. M¨ attig 174 , S. M¨ attig 41 , P.J. Magalhaes Martins 124a,h , L. Magnoni 29 , E. Magradze 54 , Y. Mahalalel 153 , K. Mahboubi 48 , G. Mahout 17 ... See full document

22

Measurement of the WZ production cross section in pp collisions at $\sqrt(s) =$ 13 TeV

Measurement of the WZ production cross section in pp collisions at $\sqrt(s) =$ 13 TeV

... for the trigger effi- ciency and 2–4% for the lepton identification and isolation require- ments, depending on the lepton ...to the use of simulated samples: 1% for the effects ... See full document

23

Measurement of the top-antitop production cross section in the tau+jets channel in pp collisions at sqrt(s) = 7 TeV

Measurement of the top-antitop production cross section in the tau+jets channel in pp collisions at sqrt(s) = 7 TeV

... D. Abbaneo, E. Auffray, G. Auzinger, M. Bachtis, P. Baillon, A.H. Ball, D. Barney, J.F. Benitez, C. Bernet 5 , G. Bianchi, P. Bloch, A. Bocci, A. Bonato, C. Botta, H. Breuker, T. Camporesi, G. Cerminara, T. Christiansen, ... See full document

27

Measurement of the charge asymmetry in top-quark pair production in proton-proton collisions at $\sqrt{s}=7$ TeV

Measurement of the charge asymmetry in top-quark pair production in proton-proton collisions at $\sqrt{s}=7$ TeV

... performance of the unfolding algorithm is tested in sets of pseudoexperiments, each of which provides a randomly-generated sample ...distribution. The number of events ... See full document

33

Measurement of the $W^{\pm}Z$ boson pair-production cross section in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS Detector

Measurement of the $W^{\pm}Z$ boson pair-production cross section in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS Detector

... certainties in the scale and resolution of the electron energy, muon momentum, jet energy and E miss T , as well as uncertainties in the scale factors applied to the ... See full document

39

Measurement of the $ZZ$ Production Cross Section in $pp$ Collisions at $\sqrt{s}$ = 13 TeV with the ATLAS Detector

Measurement of the $ZZ$ Production Cross Section in $pp$ Collisions at $\sqrt{s}$ = 13 TeV with the ATLAS Detector

... inclusive with respect to additional ...tion with two leptonically decaying Z bosons and a third hadronically decaying weak boson and contributions from double parton scattering are included in ... See full document

19

Measurement of the production cross section for Z/gamma* in association with jets in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

Measurement of the production cross section for Z/gamma* in association with jets in $pp$ collisions at $\sqrt{s}=7$ 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

60

Measurement of the cross-section for producing a W boson in association with a single top quark in pp collisions at $ \sqrt{s}=13 $ TeV with ATLAS

Measurement of the cross-section for producing a W boson in association with a single top quark in pp collisions at $ \sqrt{s}=13 $ TeV with ATLAS

... O. Gueta 155 , B. Gui 113 , E. Guido 53a,53b , T. Guillemin 5 , S. Guindon 2 , U. Gul 56 , C. Gumpert 32 , J. Guo 36b , Y. Guo 36c,q , R. Gupta 43 , S. Gupta 122 , G. Gustavino 134a,134b , P. Gutierrez 115 ... See full document

40

Measurement of isolated-photon pair production in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

Measurement of isolated-photon pair production in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

... for the leading and the subleading candidates. In the two- dimensional fit method, the templates are shifted by +160 and +120 MeV respectively in order to maximize the ... See full document

47

Observation of top-quark pair production in association with a photon and measurement of the $t\bar{t}\gamma$ production cross section in pp collisions at $\sqrt{s}=7$ TeV using the ATLAS detector

Observation of top-quark pair production in association with a photon and measurement of the $t\bar{t}\gamma$ production cross section in pp collisions at $\sqrt{s}=7$ TeV using the ATLAS detector

... for top-quark pairs (t¯ t) produced together with a photon (γ) with transverse energy greater than 20 GeV using a sample of t¯ t candidate events in final states ... See full document

29

Search for scalar bottom quark pair production with the ATLAS detector in $pp$ Collisions at $\sqrt{s}=7$ TeV

Search for scalar bottom quark pair production with the ATLAS detector in $pp$ Collisions at $\sqrt{s}=7$ TeV

... for the very successful operation of the LHC, as well as the support staff from our institutions without whom ATLAS could not be operated ...acknowledge the support of ... See full document

18

Measurement of the prompt J/ $\psi $ pair production cross-section in pp collisions at $\sqrt{s} = 8$  TeV with the ATLAS detector

Measurement of the prompt J/ $\psi $ pair production cross-section in pp collisions at $\sqrt{s} = 8$  TeV 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, Canada; CERN; CONICYT, ... See full document

53

Measurement of the $t \bar t$ production cross section in $pp$ collisions at $\sqrt s = 8$ TeV in dilepton final states containing one $\tau$ lepton

Measurement of the $t \bar t$ production cross section in $pp$ collisions at $\sqrt s = 8$ TeV in dilepton final states containing one $\tau$ lepton

... feature of the CMS apparatus is a superconducting solenoid of 6 m internal di- ameter and 13 m in length, providing a magnetic field of ...Within the superconducting solenoid ... See full document

31

Measurement of the $ZZ$ production cross section and search for anomalous couplings in 2 l2l ' final states in $pp$ collisions at $\sqrt{s}=7$ TeV

Measurement of the $ZZ$ production cross section and search for anomalous couplings in 2 l2l ' final states in $pp$ collisions at $\sqrt{s}=7$ TeV

... description of the CMS detector can be found elsewhere [22]. The central feature of the CMS apparatus is a superconducting solenoid of 6 m internal diameter, providing a mag- ... See full document

29

Measurement of the cross section for top quark pair production in association with a W or Z boson in proton-proton collisions at $\sqrt{s} =$ 13 TeV

Measurement of the cross section for top quark pair production in association with a W or Z boson in proton-proton collisions at $\sqrt{s} =$ 13 TeV

... colleagues in the CERN accelerator departments for the excellent perfor- mance of the LHC and thank the technical and administrative staffs at CERN and at other CMS ... See full document

46

Measurement of the production cross section of jets in association with a Z boson in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector

Measurement of the production cross section of jets in association with a Z boson in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector

... on the jet energy scale (JES), determined from the combination of methods based on MC and in-situ techniques used to determine the scale, constitutes the dominant component ... See full document

57

Measurement of the top-quark mass in $t\bar{t}$ events with lepton+jets final states in $pp$ collisions at $\sqrt{s}=7$ TeV

Measurement of the top-quark mass in $t\bar{t}$ events with lepton+jets final states in $pp$ collisions at $\sqrt{s}=7$ TeV

... Academy of Finland, MEC, and HIP (Finland); CEA and CNRS/IN2P3 (France); BMBF, DFG, and HGF (Germany); GSRT (Greece); OTKA and NKTH (Hungary); DAE and DST (India); IPM (Iran); SFI (Ireland); INFN (Italy); NRF and ... See full document

33

Measurement of the differential cross sections for top quark pair production as a function of kinematic event variables in pp collisions at $\sqrt s$=7 and 8 TeV

Measurement of the differential cross sections for top quark pair production as a function of kinematic event variables in pp collisions at $\sqrt s$=7 and 8 TeV

... colleagues in the CERN accelerator departments for the excellent performance of the LHC and thank the technical and administrative staffs at CERN and at other CMS ... See full document

25

Measurement of the top quark pair production charge asymmetry in proton-proton collisions at $\sqrt{s}$ = 7 TeV using the ATLAS detector

Measurement of the top quark pair production charge asymmetry in proton-proton collisions at $\sqrt{s}$ = 7 TeV using the ATLAS detector

... MES of Russia and ROSATOM, Rus- sian Federation; JINR; MSTD, Serbia; MSSR, Slovakia; ARRS and MIZˇ S, Slovenia; DST/NRF, South Africa; MINECO, Spain; SRC and Wallenberg Foundation, Sweden; SER, SNSF and ... See full document

45

Measurement of the isolated di-photon cross-section in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

Measurement of the isolated di-photon cross-section in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

... J. Biesiada 14 , M. Biglietti 134a,134b , H. Bilokon 47 , M. Bindi 19a,19b , S. Binet 115 , A. Bingul 18c , C. Bini 132a,132b , C. Biscarat 177 , U. Bitenc 48 , K.M. Black 21 , R.E. Blair 5 , J.-B. Blanchard 115 , ... See full document

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