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[PDF] Top 20 Measurements of the $t\bar{t}$ charge asymmetry using the dilepton decay channel in pp collisions at $\sqrt{s} =$ 7 TeV

Has 10000 "Measurements of the $t\bar{t}$ charge asymmetry using the dilepton decay channel in pp collisions at $\sqrt{s} =$ 7 TeV" found on our website. Below are the top 20 most common "Measurements of the $t\bar{t}$ charge asymmetry using the dilepton decay channel in pp collisions at $\sqrt{s} =$ 7 TeV".

Measurements of the $t\bar{t}$ charge asymmetry using the dilepton decay channel in pp collisions at $\sqrt{s} =$ 7 TeV

Measurements of the $t\bar{t}$ charge asymmetry using the dilepton decay channel in pp collisions at $\sqrt{s} =$ 7 TeV

... S. Abdullin, M. Albrow, J. Anderson, G. Apollinari, L.A.T. Bauerdick, A. Beretvas, J. Berryhill, P.C. Bhat, K. Burkett, J.N. Butler, V. Chetluru, H.W.K. Cheung, F. Chlebana, S. Cihangir, V.D. Elvira, I. ... See full document

33

Measurement of the electron charge asymmetry in inclusive $W$ production in $pp$ collisions at $\sqrt{s}=7$ TeV

Measurement of the electron charge asymmetry in inclusive $W$ production in $pp$ collisions at $\sqrt{s}=7$ TeV

... S. Abdullin, M. Albrow, J. Anderson, L.A.T. Bauerdick, A. Beretvas, J. Berryhill, P.C. Bhat, I. Bloch, K. Burkett, J.N. Butler, V. Chetluru, H.W.K. Cheung, F. Chlebana, V.D. Elvira, I. Fisk, J. Freeman, Y. Gao, D. ... See full document

27

Measurements of top quark spin observables in $ t\overline{t} $ events using dilepton final states in $ \sqrt{s}=8 $ TeV pp collisions with the ATLAS detector

Measurements of top quark spin observables in $ t\overline{t} $ events using dilepton final states in $ \sqrt{s}=8 $ TeV pp collisions with the ATLAS detector

... shape of the fake and non-prompt lepton background distributions are taken from MC simulation but the normalisation is derived from data in a control region enriched in fake ...applying ... See full document

50

Measurement of the $t\bar{t}$ production cross section in the all-jet final state in pp collisions at $\sqrt{s}$ = 7 TeV

Measurement of the $t\bar{t}$ production cross section in the all-jet final state in pp collisions at $\sqrt{s}$ = 7 TeV

... collections of reconstructed particles are produced using a particle-flow (PF) algorithm [19, ...from the PF particles using the anti-k T jet algorithm [21], im- plemented ... See full document

29

Search for $t\bar t$ resonances in the lepton plus jets final state with ATLAS using 4.7 fb$^{-1}$ of $pp$ collisions at $\sqrt{s} = 7$ TeV

Search for $t\bar t$ resonances in the lepton plus jets final state with ATLAS using 4.7 fb$^{-1}$ of $pp$ collisions at $\sqrt{s} = 7$ TeV

... G. Aad 48 , T. Abajyan 21 , B. Abbott 111 , J. Abdallah 12 , S. Abdel Khalek 115 , A.A. Abdelalim 49 , O. Abdinov 11 , R. Aben 105 , B. Abi 112 , M. Abolins 88 , O.S. AbouZeid 158 , H. Abramowicz 153 , H. ... See full document

29

Measurement of the single-top-quark $t$-channel cross section in $pp$ collisions at $\sqrt{s}=7$ TeV

Measurement of the single-top-quark $t$-channel cross section in $pp$ collisions at $\sqrt{s}=7$ TeV

... described in detail elsewhere [9], and the key components for this anal- ysis are listed ...below. The main feature of the CMS detector is a superconducting solenoidal magnet with a ... See full document

41

Measurement of $\mathrm {t}\overline{\mathrm {t}}$ production with additional jet activity, including $\mathrm {b}$ quark jets, in the dilepton decay channel using pp collisions at $\sqrt{s} =$ 8 TeV

Measurement of $\mathrm {t}\overline{\mathrm {t}}$ production with additional jet activity, including $\mathrm {b}$ quark jets, in the dilepton decay channel using pp collisions at $\sqrt{s} =$ 8 TeV

... from the two neutrinos; the W boson invariant mass is fixed to ...and the top quark and antiquark masses are fixed to a value of ...pair of jets and lepton- jet combination fulfilling ... See full document

78

Measurements of $t\bar{t}$ cross sections in association with $b$ jets and inclusive jets and their ratio using dilepton final states in pp collisions at $\sqrt{s}$ = 13 TeV

Measurements of $t\bar{t}$ cross sections in association with $b$ jets and inclusive jets and their ratio using dilepton final states in pp collisions at $\sqrt{s}$ = 13 TeV

... The cross section ratio has been measured in a visible phase space region using the dilepton decay mode of tt¯ events and corrected to the particle level, corresponding to the detector a[r] ... See full document

24

Search for resonant $t\bar{t}$ production in lepton+jets events in $pp$ collisions at $\sqrt{s}=7$ TeV

Search for resonant $t\bar{t}$ production in lepton+jets events in $pp$ collisions at $\sqrt{s}=7$ TeV

... of the particle with respect to the counterclockwise beam ...surround the tracking volume. In this analysis the calorimetry provides high-resolution energy and direction ... See full document

37

Measurement of the $t\bar{t}$ production cross section in the $\tau$ + jets final state in $pp$ collisions at $\sqrt{s}=8$ TeV using the ATLAS detector

Measurement of the $t\bar{t}$ production cross section in the $\tau$ + jets final state in $pp$ collisions at $\sqrt{s}=8$ TeV using the ATLAS detector

... cover the kinematic range expected in data and a background sample enriched in dijet events from data [64] ...categories of discriminating variables are used. The first category ... See full document

26

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

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

... Since the jet energy scale (JES) is the leading systematic uncertainty in previous top-quark mass measurements, we construct a likelihood function that allows the determination ... See full document

33

Searches for new physics using the $t\bar{t}$ invariant mass distribution in pp collisions at $\sqrt{s}$=8  TeV

Searches for new physics using the $t\bar{t}$ invariant mass distribution in pp collisions at $\sqrt{s}$=8  TeV

... production of tt events is presented, from data corre- sponding to an integrated luminosity of ...1 of pp collisions ats = 8 TeV, recorded with the ... See full document

31

Measurement of masses in the $t \bar{t}$ system by kinematic endpoints in pp collisions at $\sqrt{s}$ = 7 TeV

Measurement of masses in the $t \bar{t}$ system by kinematic endpoints in pp collisions at $\sqrt{s}$ = 7 TeV

... determination of the top-quark mass sets a fundamental benchmark for the standard model (SM), and is one of the precision measurements that defines electroweak constraints on ... See full document

43

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

... listed in Table 1 are assumed to be fully correlated among the three input ...are the uncertainties on pileup, for which we assign full correlation between the 2011 analyses but no correlation ... See full document

33

Measurement of the W boson polarisation in $t\bar{t}$ events from pp collisions at $\sqrt{s}$ = 8 TeV in the lepton + jets channel with ATLAS

Measurement of the W boson polarisation in $t\bar{t}$ events from pp collisions at $\sqrt{s}$ = 8 TeV in the lepton + jets channel with ATLAS

... assess the impact of the different parton shower and hadronisation models, the Powheg+Herwig sample is compared to a Powheg+Pythia sample and the symmetrised difference is taken as a ... See full document

42

Search for a light pseudoscalar Higgs boson in the dimuon decay channel in $pp$ collisions at $\sqrt{s}=7$ TeV

Search for a light pseudoscalar Higgs boson in the dimuon decay channel in $pp$ collisions at $\sqrt{s}=7$ TeV

... to the Υ shape and continuum background are performed in the barrel and endcap regions separately, shown in ...1. The fitted numbers of events are given in Table 1; ... See full document

27

Measurement of the cross section ratio $\sigma_\mathrm{t \bar{t} b \bar{b}} / \sigma_\mathrm{t \bar{t}  jj }$ in pp collisions at $\sqrt{s}$ = 8 TeV

Measurement of the cross section ratio $\sigma_\mathrm{t \bar{t} b \bar{b}} / \sigma_\mathrm{t \bar{t} jj }$ in pp collisions at $\sqrt{s}$ = 8 TeV

... measurement of the cross section ratio σ ttbb /σ ttjj has been presented by the CMS experi- ment, using a data sample of pp collisions at a centre-of-mass ... See full document

31

Measurement of $t \bar{t}$ production with a veto on additional central jet activity in pp collisions at sqrt(s) = 7 TeV using the ATLAS detector

Measurement of $t \bar{t}$ production with a veto on additional central jet activity in pp collisions at sqrt(s) = 7 TeV using the ATLAS detector

... W. Liebig 13 , C. Limbach 20 , A. Limosani 87 , M. Limper 63 , S.C. Lin 152,v , F. Linde 106 , J.T. Linnemann 89 , E. Lipeles 121 , L. Lipinsky 126 , A. Lipniacka 13 , T.M. Liss 166 , D. Lissauer 24 , A. Lister 49 , A.M. ... See full document

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Measurement of the $t\bar{t}$ production cross section using events in the e$\mu$ final state in pp collisions at $\sqrt{s} =$ 13 TeV

Measurement of the $t\bar{t}$ production cross section using events in the e$\mu$ final state in pp collisions at $\sqrt{s} =$ 13 TeV

... events in the lepton+jets final state, can con- taminate the signal sample if a jet is incorrectly reconstructed as a lepton, or the lepton is in- correctly identified as being ... See full document

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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

... measurement of the tt production cross section in the channel tt → (` ν ` )( τν τ ) bb is presented, where ` is an electron or a muon, and the τ lepton is reconstructed through ... See full document

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