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[PDF] Top 20 Measurements Of T(t)over-bar Charge Asymmetry Using Dilepton Final States In Pp Collisions At Root S=8 Tev

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Measurements Of T(t)over-bar Charge Asymmetry Using Dilepton Final States In Pp Collisions At Root S=8 Tev

Measurements Of T(t)over-bar Charge Asymmetry Using Dilepton Final States In Pp Collisions At Root S=8 Tev

... mass of the top quark, measured by this experiment as m t = 172 ...particularly in the mechanism of electroweak (EW) symmetry ...Precision measurements of top quark properties have the ... See full document

23

Measurement of the t(t)over-bar production cross section in pp collisions at root s=8 TeV in dilepton final states containing one tau lepton

Measurement of the t(t)over-bar production cross section in pp collisions at root s=8 TeV in dilepton final states containing one tau lepton

... Ministry of Education, Youth and Sports (MEYS) of the Czech Republic; the Council of Science and Industrial Research, India; the HOMING PLUS programme of Foundation For Polish Science, ... See full document

22

Measurement of the $t \bar{t}$ production cross section in the dilepton channel in pp collisions at $\sqrt{s}$ = 8 TeV

Measurement of the $t \bar{t}$ production cross section in the dilepton channel in pp collisions at $\sqrt{s}$ = 8 TeV

... simulated using POWHEG . Inclusive production of the WZ and ZZ diboson final states is simulated with PYTHIA ...duction of WW fully leptonic final states is simulated with ... See full document

29

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 ...composed of a barrel and two endcap ... See full document

31

Measurements of $t\bar{t}$ spin correlations and top-quark polarization using dilepton final states in $pp$ collisions at $\sqrt{s}$ = 7 TeV

Measurements of $t\bar{t}$ spin correlations and top-quark polarization using dilepton final states in $pp$ collisions at $\sqrt{s}$ = 7 TeV

... predictions of Fig. 1 and Table 2 for this Letter. We congratulate our colleagues in the CERN accelerator departments for the excellent performance of the LHC and thank the techni- cal and ... See full document

29

Measurements of t t-bar spin correlations and top quark polarization using dilepton final states in pp collisions at sqrt(s) = 8 TeV

Measurements of t t-bar spin correlations and top quark polarization using dilepton final states in pp collisions at sqrt(s) = 8 TeV

... Measurements of the top quark-antiquark (t¯t) spin correlations and the top quark polarization are presented for t¯t pairs produced in pp collisions at ffiffiffis p ¼ 8 ... See full document

25

Searches For R-parity-violating Supersymmetry In Pp Collisions At Root S=8 Tev In Final States With 0-4 Leptons

Searches For R-parity-violating Supersymmetry In Pp Collisions At Root S=8 Tev In Final States With 0-4 Leptons

... any of the λ 00 ijk are nonzero, in events with zero or one lepton using the jet and b-tagged jet multiplicities of the event and in dilepton events by means of a ... See full document

44

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

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

... scattering of the proton-proton collisions is evaluated from pseudo-experiments for which the distribution of m t was obtained after varying parameters of the PDF by ± 1σ with respect to their ... See full document

31

Measurement of the charge asymmetry in top quark pair production in pp collisions at $\sqrt(s) =$ 8 TeV using a template method

Measurement of the charge asymmetry in top quark pair production in pp collisions at $\sqrt(s) =$ 8 TeV using a template method

... Corroboration of results from experiments at the Tevatron using measure- ments at the LHC is complicated by several differences between the two ...while at the Tevatron the majority ... See full document

27

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

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 ...leptons of the ... See full document

50

Measurements of $t \bar t$ charge asymmetry using dilepton final states in pp collisions at $\sqrt s=8$ TeV

Measurements of $t \bar t$ charge asymmetry using dilepton final states in pp collisions at $\sqrt s=8$ TeV

... mass of the top quark, measured by this experiment as m t = ...particularly in the mechanism of electroweak (EW) symmetry ...Precision measurements of top quark properties have the ... See full document

34

Inclusive and differential measurements of the t(t)over-bar charge asymmetry in pp collisions at root s=8 TeV

Inclusive and differential measurements of the t(t)over-bar charge asymmetry in pp collisions at root s=8 TeV

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

27

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

Measurements of the associated production of a Z boson and b jets in pp collisions at root s=8 TeV

Measurements of the associated production of a Z boson and b jets in pp collisions at root s=8 TeV

... subtraction of all non-Drell–Yan background con- tributions, the extraction of the Z (1b) and Z(2b) event yields requires an evaluation of the purity of the b tagging selection, ...fraction ... See full document

35

Study of hadronic event-shape variables in multijet final states in pp collisions at root s=7 TeV

Study of hadronic event-shape variables in multijet final states in pp collisions at root s=7 TeV

... studies of event-shape variables at hadron colliders include those of the CDF experiment at the Tevatron [6], and early measurements at the LHC [7, ...studied in the ... See full document

34

Search for supersymmetry in hadronic final states using MT2 in $pp$ collisions at $\sqrt{s} = 7$ TeV

Search for supersymmetry in hadronic final states using MT2 in $pp$ collisions at $\sqrt{s} = 7$ TeV

... resulting in similar final states is presented using a data sample of ...1 of pp collisions collected ats = 7 TeV with the CMS detector ... See full document

37

Inclusive Quarkonium Production At Forward Rapidity In Pp Collisions At Root S=8 Tev

Inclusive Quarkonium Production At Forward Rapidity In Pp Collisions At Root S=8 Tev

... N. Bastid 70 , S. Basu 132 , B. Bathen 54 , G. Batigne 113 , A. Batista Camejo 70 , B. Batyunya 66 , P. C. Batzing 22 , I. G. Bearden 81 , H. Beck 53 , C. Bedda 110 , N. K. Behera 50 , I. Belikov 55 , F. Bellini ... See full document

14

Measurement of the top quark mass using charged particles in pp collisions at root s=8 TeV

Measurement of the top quark mass using charged particles in pp collisions at root s=8 TeV

... Science of the Russian Federation, the Federal Agency of Atomic Energy of the Russian Federation, Russian Academy of Sciences, and the Russian Foundation for Basic Research; the Ministry ... See full document

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Search for new phenomena in monophoton final states in proton-proton collisions at root s=8 TeV

Search for new phenomena in monophoton final states in proton-proton collisions at root s=8 TeV

... sum of the transverse energy (in GeV) of additional pho- tons is required to be less than (0 ...), of neutral hadrons is required to be less than (1 ...and of charged hadrons is ... See full document

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