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[PDF] Top 20 Measurement of the ratio B(t→wb)/b(t→wq) In pp collisions at S=8 Tev

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Measurement of the ratio B(t→wb)/b(t→wq) In pp collisions at S=8 Tev

Measurement of the ratio B(t→wb)/b(t→wq) In pp collisions at S=8 Tev

... section of 4.393 nb, computed using fewz [38] . The Z + γ process is also simulated with MadGraph and normalised to the LO predicted cross section of ...modelled at NLO with powheg ... See full document

26

Measurement of the $t\bar{t}$ production cross-section using $e\mu $ events with b-tagged jets in pp collisions at $\sqrt{s}$ = 7 and 8  $\,\mathrm{TeV}$ with the ATLAS detector

Measurement of the $t\bar{t}$ production cross-section using $e\mu $ events with b-tagged jets in pp collisions at $\sqrt{s}$ = 7 and 8  $\,\mathrm{TeV}$ with the ATLAS detector

... velop the analysis, to compare to the data and to evaluate signal and background efficiencies and ...through the full ATLAS detec- tor simulation [11] based on GEANT4 [12], or through a faster ... See full document

34

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

... Greece; the National Scientific Research Foundation, and Na- tional Innovation Office, Hungary; the Department of Atomic Energy and the Department of Science and Technology, India; ... See full document

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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

... D. Abbaneo, E. Auffray, G. Auzinger, M. Bachtis, P. Baillon, A.H. Ball, D. Barney, A. Benaglia, J. Bendavid, L. Benhabib, J.F. Benitez, G.M. Berruti, P. Bloch, A. Bocci, A. Bonato, C. Botta, H. Breuker, T. ... See full document

27

Measurement of the $t\bar{t}$ production cross-section using $e\mu$ events with b-tagged jets in pp collisions at $\sqrt{s}$=13 TeV with the ATLAS detector

Measurement of the $t\bar{t}$ production cross-section using $e\mu$ events with b-tagged jets in pp collisions at $\sqrt{s}$=13 TeV with the ATLAS detector

... A. Alonso 38 , F. Alonso 73 , C. Alpigiani 139 , M. Alstaty 87 , B. Alvarez Gonzalez 32 , D. Álvarez Piqueras 167 , M.G. Alviggi 105a , 105b , B.T. Amadio 16 , K. Amako 68 , Y. Amaral Coutinho 26a , C. Amelung 25 ... See full document

22

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

... by the following funding agencies: BMWFW and FWF (Austria); FNRS and FWO (Belgium); CNPq, CAPES, FAPERJ, and FAPESP (Brazil); MES (Bulgaria); CERN; CAS, MoST, and NSFC (China); COLCIENCIAS (Colombia); MSES and CSF ... See full document

31

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 Marie-Curie programme and the European Re- search Council and EPLANET (European Union); the Leventis Foundation; the ...Foundation; the Alexander von Humboldt Foundation; ... See full document

78

Measurement of the Z/$\gamma$*+b-jet cross section in pp collisions at $\sqrt{s}$ = 7 TeV

Measurement of the Z/$\gamma$*+b-jet cross section in pp collisions at $\sqrt{s}$ = 7 TeV

... describes the measurement with the Compact Muon Solenoid (CMS) detector of the pp → Z/γ ∗ + b-jet cross section with Z/γ ∗ → `` (where `` = ee or µµ), including at ... See full document

29

Measurement of the top quark mass in the dileptonic $t\bar{t}$ decay channel using the mass observables $M_{b\ell}$, $M_{T2}$, and $M_{b\ell\nu}$ in pp collisions at $\sqrt{s}=8$ TeV

Measurement of the top quark mass in the dileptonic $t\bar{t}$ decay channel using the mass observables $M_{b\ell}$, $M_{T2}$, and $M_{b\ell\nu}$ in pp collisions at $\sqrt{s}=8$ TeV

... with the infrared and collinear safe anti-k T al- gorithm [23], with a distance parameter R of ...implemented in the F AST J ET package [24]. The jet momentum is determined as ... See full document

48

Measurement Of The Integrated And Differential T(t)over-bar Production Cross Sections For High-p(t) Top Quarks In Pp Collisions At Root S=8 Tev

Measurement Of The Integrated And Differential T(t)over-bar Production Cross Sections For High-p(t) Top Quarks In Pp Collisions At Root S=8 Tev

... parameters in the fit, three of which are built into the model as uncertainties in the input distributions, these being the jet energy scale, jet energy resolution, and ... See full document

26

Measurement of the $b\overline{b}$ dijet cross section in pp collisions at $\sqrt{s} = 7$  TeV with the ATLAS detector

Measurement of the $b\overline{b}$ dijet cross section in pp collisions at $\sqrt{s} = 7$  TeV with the ATLAS detector

... correction of the measured distribution for detector e ffects and inefficiencies is done via an un- folding procedure that uses the iterative dynamically stabilised (IDS) method [ 30 ...]. At ... See full document

36

Measurement Of Dijet Azimuthal Decorrelation In Pp Collisions At Root S=8 Tev

Measurement Of Dijet Azimuthal Decorrelation In Pp Collisions At Root S=8 Tev

... description of the CMS detector, together with a definition of the coordinate system used and the relevant kinematic variables, can be found in ...]. The central feature ... See full document

23

Measurement of the $\mathrm{t}\overline{{\mathrm{t}}}$ production cross section in the all-jets final state in pp collisions at $\sqrt{s}=8$ $\,\text {TeV}$

Measurement of the $\mathrm{t}\overline{{\mathrm{t}}}$ production cross section in the all-jets final state in pp collisions at $\sqrt{s}=8$ $\,\text {TeV}$

... shown in Fig. 8 are obtained from the detector-level measurement, after correcting for bin migration effects and extrapolating to the full phase space using a bin- by-bin acceptance ... See full document

36

Measurement of the cross section for production of $b b^-$ bar $X$, decaying to muons in $pp$ collisions at $\sqrt{s}=7$ TeV

Measurement of the cross section for production of $b b^-$ bar $X$, decaying to muons in $pp$ collisions at $\sqrt{s}=7$ TeV

... description of the CMS detector is presented in Section ...describes the collision and simulated data used for this measurement and the selection ...description of ... See full document

33

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

... used in Ref. [25] and is only briefly described in this section. The particle-flow (PF) method [26, 27] is used to reconstruct final- state ...[29]) of opposite electric charge, with p ... See full document

34

Measurement of the differential cross-section of $B^{+}$ meson production in pp collisions at $\sqrt{s}$ = 7 TeV at ATLAS

Measurement of the differential cross-section of $B^{+}$ meson production in pp collisions at $\sqrt{s}$ = 7 TeV at ATLAS

... consisting of an inner tracker, a calorimeter and a muon ...outline of the components that are most relevant for this analysis is given ...below. The inner detector (ID) directly surrounds ... See full document

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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

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

22

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

... results of the three analyses are combined using the BLUE ...pair of measurements is estimated by generating dedicated pseudo- ...experiments. The correlation is 60% between NN and | η ... See full document

41

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

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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

... A.G. Goussiou 140 , N. Govender 147b,q , E. Gozani 154 , L. Graber 57 , I. Grabowska-Bold 41a , P.O.J. Gradin 58 , P. Grafström 22a,22b , J. Gramling 52 , E. Gramstad 121 , S. Grancagnolo 17 , V. Gratchev 125 , ... See full document

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