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[PDF] Top 20 Measurement of four-jet differential cross sections in $\sqrt{s}=8$ TeV proton-proton collisions using the ATLAS detector

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Measurement of four-jet differential cross sections in $\sqrt{s}=8$ TeV proton-proton collisions using the ATLAS detector

Measurement of four-jet differential cross sections in $\sqrt{s}=8$ TeV proton-proton collisions using the ATLAS detector

... J.B. De Vivie De Regie 117 , W.J. Dearnaley 72 , R. Debbe 25 , C. Debenedetti 137 , D.V. Dedovich 65 , I. Deigaard 107 , J. Del Peso 82 , T. Del Prete 124a,124b , D. Delgove 117 , F. Deliot 136 , C.M. Delitzsch 49 , M. ... See full document

75

Measurement of differential production cross-sections for a $Z$ boson in association with $b$-jets in 7 TeV proton-proton collisions with the ATLAS detector

Measurement of differential production cross-sections for a $Z$ boson in association with $b$-jets in 7 TeV proton-proton collisions with the ATLAS detector

... M. Huhtinen 30 , T.A. H¨ ulsing 82 , M. Hurwitz 15 , N. Huseynov 64,b , J. Huston 89 , J. Huth 57 , G. Iacobucci 49 , G. Iakovidis 10 , I. Ibragimov 142 , L. Iconomidou-Fayard 116 , E. Ideal 177 , P. Iengo 103a , O. ... See full document

57

Measurement of differential cross sections for Z boson production in association with jets in proton-proton collisions at $\sqrt{s} =$ 13 TeV

Measurement of differential cross sections for Z boson production in association with jets in proton-proton collisions at $\sqrt{s} =$ 13 TeV

... reconstruct the events. It combines the infor- mation from the various elements of the CMS detector to reconstruct and identify each particle in the ...event. ... See full document

51

Performance of algorithms that reconstruct missing transverse momentum in $\sqrt{s}=$ 8 TeV proton-proton collisions in the ATLAS detector

Performance of algorithms that reconstruct missing transverse momentum in $\sqrt{s}=$ 8 TeV proton-proton collisions in the ATLAS detector

... deposits in the soft term and uses only the inner detector (ID) ...to the amount of pileup; however, it does not have as good a response as the CST E T miss , due mainly ... See full document

69

Measurements of the electron and muon inclusive cross-sections in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

Measurements of the electron and muon inclusive cross-sections in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

... Additionally, the efficiency of the electron identification cuts in the simu- lation is compared with a measurement made on data using a tag-and-probe (T&P) ... See full document

53

Jet energy measurement and its systematic uncertainty in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

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

100

Measurement of differential cross sections of isolated-photon plus heavy-flavour jet production in pp collisions at $\sqrt{s}=8$ TeV using the ATLAS detector

Measurement of differential cross sections of isolated-photon plus heavy-flavour jet production in pp collisions at $\sqrt{s}=8$ TeV using the ATLAS detector

... ranges of the size of the relative uncertainties in the mea- surement as a function of E γ T due to the various sources are pro- vided in Table 2 .... ... See full document

23

Measurement of the $ t\overline{t}\gamma $ production cross section in proton-proton collisions at $ \sqrt{s}=8 $ TeV with the ATLAS detector

Measurement of the $ t\overline{t}\gamma $ production cross section in proton-proton collisions at $ \sqrt{s}=8 $ TeV with the ATLAS detector

... J. Barreiro Guimarães da Costa 35a , R. Bartoldus 145 , A.E. Barton 75 , P. Bartos 146a , A. Basalaev 125 , A. Bassalat 119, f , R.L. Bates 56 , S.J. Batista 161 , J.R. Batley 30 , M. Battaglia 139 , M. Bauce 134a,134b , ... See full document

42

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

27

Measurement of the inclusive jet cross-section in proton-proton collisions at $ \sqrt{s}=7 $ TeV using 4.5 fb$^{−1}$ of data with the ATLAS detector

Measurement of the inclusive jet cross-section in proton-proton collisions at $ \sqrt{s}=7 $ TeV using 4.5 fb$^{−1}$ of data with the ATLAS detector

... uncertainty. The effect of this uncertainty in the cross-section measurements is evaluated by smearing the energy of reconstructed jets in the MC simulation ... See full document

63

Measurements of jet multiplicity and differential production cross sections of $Z +$ jets events in proton-proton collisions at $\sqrt{s} =$ 7 TeV

Measurements of jet multiplicity and differential production cross sections of $Z +$ jets events in proton-proton collisions at $\sqrt{s} =$ 7 TeV

... during the data acquisition period because of the increasing instantaneous ...pairs of 17 GeV and 8 GeV are used for most of the data ...sample. The electron ... See full document

41

Measurement of total and differential $W^+W^-$ production cross sections in proton-proton collisions at $\sqrt{s}=$ 8 TeV with the ATLAS detector and limits on anomalous triple-gauge-boson couplings

Measurement of total and differential $W^+W^-$ production cross sections in proton-proton collisions at $\sqrt{s}=$ 8 TeV with the ATLAS detector and limits on anomalous triple-gauge-boson couplings

... M. Bauce 134a,134b , F. Bauer 138 , H.S. Bawa 145, f , J.B. Beacham 113 , M.D. Beattie 74 , T. Beau 82 , P.H. Beauchemin 163 , R. Beccherle 126a,126b , P. Bechtle 22 , H.P. Beck 17,g , K. Becker 122 , M. Becker 85 , M. ... See full document

78

Measurements of differential cross sections for associated production of a W boson and jets in proton-proton collisions at $\sqrt{s} =$ 8 TeV

Measurements of differential cross sections for associated production of a W boson and jets in proton-proton collisions at $\sqrt{s} =$ 8 TeV

... subsystems. The first level of the trigger system, composed of custom hardware pro- cessors, uses information from the calorimeters and muon detectors to select events in a fixed ... See full document

50

Measurement of differential cross sections for inclusive isolated-photon and photon+jets production in proton-proton collisions at $\sqrt{s} =$ 13 TeV

Measurement of differential cross sections for inclusive isolated-photon and photon+jets production in proton-proton collisions at $\sqrt{s} =$ 13 TeV

... general-purpose detector built to explore physics at the TeV scale. The central fea- ture of the CMS apparatus is a superconducting solenoid of 6 m internal diameter, ... See full document

39

Search for excited electrons and muons in $\sqrt{s}$=8 TeV proton-proton collisions with the ATLAS detector

Search for excited electrons and muons in $\sqrt{s}$=8 TeV proton-proton collisions with the ATLAS detector

... from the data all simulated backgrounds except Z + jets. The normalization of the Z + jets MC sample is corrected accordingly by a scale factor, separately determined to be ...both the ... See full document

39

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

... With the determined flavour fractions, the W +jets normalisation for pretag–selected events using ...to the tag–selected events using the tagging fractions ...(i.e. the ... See full document

45

Measurement of the triple-differential cross section for photon+jets production in proton-proton collisions at $\sqrt{s}$=7 TeV

Measurement of the triple-differential cross section for photon+jets production in proton-proton collisions at $\sqrt{s}$=7 TeV

... Measurements of the differential cross sections and ratios of the differential cross sections for different angular configurations are compared to ... See full document

33

Measurement of the differential cross sections for the associated production of a $W$ boson and jets in proton-proton collisions at $\sqrt{s}=13$ TeV

Measurement of the differential cross sections for the associated production of a $W$ boson and jets in proton-proton collisions at $\sqrt{s}=13$ 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 institutes for ... See full document

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Performance of jet substructure techniques for large-$R$ jets in proton-proton collisions at $\sqrt{s}$ = 7 TeV using the ATLAS detector

Performance of jet substructure techniques for large-$R$ jets in proton-proton collisions at $\sqrt{s}$ = 7 TeV using the ATLAS detector

... three jet algorithms are studied: the anti-k t algorithm [ 37 ], the Cambridge– Aachen (C/A) algorithm [ 38 , 39 ], and the k t algorithm [ 40 – 42 ...within the framework of ... See full document

93

Search for new phenomena in photon+jet events collected in proton--proton collisions at sqrt(s) = 8 TeV with the ATLAS detector

Search for new phenomena in photon+jet events collected in proton--proton collisions at sqrt(s) = 8 TeV with the ATLAS detector

... standard ATLAS selection criteria that are de- signed to reject backgrounds from hadrons ...[49]. The photon candidates must meet η-dependent requirements on hadronic leakage and shower shapes in ... See full document

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