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[PDF] Top 20 Measurement of masses in the $t \bar{t}$ system by kinematic endpoints in pp collisions at $\sqrt{s}$ = 7 TeV

Has 10000 "Measurement of masses in the $t \bar{t}$ system by kinematic endpoints in pp collisions at $\sqrt{s}$ = 7 TeV" found on our website. Below are the top 20 most common "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

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

43

Search for charge-asymmetric production of W$′$ bosons in $t\bar{t} +$ jet events from pp collisions at $\sqrt{s} =$ 7 TeV

Search for charge-asymmetric production of W$′$ bosons in $t\bar{t} +$ jet events from pp collisions at $\sqrt{s} =$ 7 TeV

... Electrons in the η range around the interface between the ECAL endcap and ECAL barrel ...from the selection. From the high-quality vertices that are close to the beam ... See full document

29

Measurement of diffraction dissociation cross sections in pp collisions at $\sqrt{s}$ = 7 TeV

Measurement of diffraction dissociation cross sections in pp collisions at $\sqrt{s}$ = 7 TeV

... events. In addition, a minimal activity in the main CMS detectors is imposed offline by requiring at least two particle-flow (PF) objects reconstructed within the geometrical ... See full document

49

Measurement of the $t \bar t$ production cross section using events with one lepton and at least one jet in pp collisions at $\sqrt{s}$  = 13 TeV

Measurement of the $t \bar t$ production cross section using events with one lepton and at least one jet in pp 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

38

Search for $Z$ ' resonances decaying to $t\bar{t}$ in dilepton+jets final states in $pp$ collisions at $\sqrt{s}=7$ TeV

Search for $Z$ ' resonances decaying to $t\bar{t}$ in dilepton+jets final states in $pp$ collisions at $\sqrt{s}=7$ TeV

... check the background modeling, a control sample is created by requiring zero b- tagged ...dominated by non-tt ...sample in the ee, µµ, and eµ channels. The shape of ... See full document

29

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

29

Measurement of the W-boson helicity in top-quark decays from $t\bar{t}$ production in lepton+jets events in pp collisions at $\sqrt{s} =$ 7 TeV

Measurement of the W-boson helicity in top-quark decays from $t\bar{t}$ production in lepton+jets events in pp collisions at $\sqrt{s} =$ 7 TeV

... feature of the Compact Muon Solenoid (CMS) detector is a superconducting solenoid, 13 m in length and 6 m in diameter, which provides a uniform axial magnetic field of ...3.8 T. ... See full document

41

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

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

... η of the jet [23]; the simulated pileup multiplicity distribution is changed within its un- certainty; and the scale factors between data and the simulation for the b-tagging ... See full document

29

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

... The measurement of the top quark-antiquark pair (tt) cross section provides a test of the hadro- production of top quark pairs as predicted by quantum ... See full document

34

Measurement of jet multiplicity distributions in $\mathrm {t}\overline{\mathrm {t}}$ production in pp collisions at $\sqrt{s} = 7\,\text {TeV} $

Measurement of jet multiplicity distributions in $\mathrm {t}\overline{\mathrm {t}}$ production in pp collisions at $\sqrt{s} = 7\,\text {TeV} $

... A kinematic reconstruction method [5] is used to determine the kinematic properties of the tt pair and to identify the two b jets originating from the decay of ... See full document

41

Measurement of Spin Correlations in $t\bar{t}$ Production using the Matrix Element Method in the Muon+Jets Final State in $pp$ Collisions at $\sqrt{s} =$ 8 TeV

Measurement of Spin Correlations in $t\bar{t}$ Production using the Matrix Element Method in the Muon+Jets Final State in $pp$ Collisions at $\sqrt{s} =$ 8 TeV

... analysis, the transfer function is used to correct the jet kinematic ...quantities. The re- constructed jet energy information, corrected for JES and JER, is mapped onto parton-level ... See full document

38

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 = ...suggests the top quark could have an important connection to physics beyond the standard model (SM), particularly ... See full document

34

Measurement of lepton differential distributions and the top quark mass in $t\bar{t}$ production in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector

Measurement of lepton differential distributions and the top quark mass in $t\bar{t}$ production in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector

... S. Senkin 37 , C. Serfon 121 , L. Serin 119 , L. Serkin 167a,167b , M. Sessa 136a,136b , R. Seuster 172 , H. Severini 115 , T. Sfiligoj 78 , F. Sforza 165 , A. Sfyrla 52 , E. Shabalina 57 , N.W. Shaikh ... See full document

84

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

... component of the Large Hadron Collider (LHC) [1] physics program is the measurement of the properties of the top quark, which is the most massive fundamental ... See full document

26

Search for resonant top plus jet production in $t\bar{t}$ + jets events with the ATLAS detector in $pp$ collisions at $\sqrt{s}=7$ TeV

Search for resonant top plus jet production in $t\bar{t}$ + jets events with the ATLAS detector in $pp$ collisions at $\sqrt{s}=7$ TeV

... uses the full ATLAS 7 TeV pp collision dataset collected in 2011, corresponding to ...−1 of integrated luminosity [13, 14] deliv- ered by the ...[16]. The ... See full document

20

Measurement of the integrated and differential $t \bar t$ production cross sections for high-$p_t$ top quarks in $pp$ collisions at $\sqrt s =$ 8 TeV

Measurement of the integrated and differential $t \bar t$ production cross sections for high-$p_t$ top quarks in $pp$ collisions at $\sqrt s =$ 8 TeV

... match the conditions observed in ...reproduce the distribution of the number of primary vertices that arises from additional pp interactions within the same or ... See full document

40

Measurement of the $\Lambda_{b}^0$ lifetime in pp collisions at $\sqrt{s} = 7$ TeV

Measurement of the $\Lambda_{b}^0$ lifetime in pp collisions at $\sqrt{s} = 7$ TeV

... identified by their type. Muons are measured in gas-ionisation detectors that are embedded in the steel return yoke outside the ...solenoid. In the barrel, there is a ... See full document

29

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

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

... A 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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