[PDF] Top 20 Measurements of b-jet tagging efficiency with the ATLAS detector using $ t\overline{t} $ events at $ \sqrt{s}=13 $ TeV
Has 10000 "Measurements of b-jet tagging efficiency with the ATLAS detector using $ t\overline{t} $ events at $ \sqrt{s}=13 $ TeV" found on our website. Below are the top 20 most common "Measurements of b-jet tagging efficiency with the ATLAS detector using $ t\overline{t} $ events at $ \sqrt{s}=13 $ TeV".
Measurements of b-jet tagging efficiency with the ATLAS detector using $ t\overline{t} $ events at $ \sqrt{s}=13 $ TeV
... E. Valdes Santurio 43a,43b , M. Valente 52 , S. Valentinetti 23b,23a , A. Valero 171 , L. Valéry 44 , R.A. Vallance 21 , A. Vallier 5 , J.A. Valls Ferrer 171 , T.R. Van Daalen 14 , W. Van Den Wollenberg 118 , H. ... See full document
49
Measurement of jet shapes in top-quark pair events at $\sqrt{s}$ = 7 TeV using the ATLAS detector
... corrects the light-jet sample for purity effects. Similarly, the odd- numbered ...Figs. 13–21 show the integrated shapes hΨ(r)i as a function of r and in bins of p ... See full document
30
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
... those with two real prompt leptons from W or Z boson decays (in- cluding those produced via leptonic τ decays), and those where at least one of the reconstructed lepton candidates is ... See full document
34
Inclusive and differential measurements of the $t\overline{t}$ charge asymmetry in pp collisions at $\sqrt{s} =$ 8 TeV
... collisions at a centre-of-mass energy of 8 TeV. The data, collected with the CMS experiment at the LHC, corre- spond to an integrated luminosity of ... See full document
38
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
... than the ones imposed at trigger level. The tag-and-probe method measures the efficiency of these require- ments, yielding typical efficiencies of 70% and 92% for ... See full document
38
Measurement of the jet mass in highly boosted ${\mathrm{t}}\overline{\mathrm{t}}$ events from pp collisions at $\sqrt{s}=8$ $\,\text {TeV}$
... feature of the CMS detector is a superconducting solenoid of 6 m internal diameter, providing a magnetic field of ...composed of a barrel and two endcap sections reside within ... See full document
44
Comprehensive measurements of $t$-channel single top-quark production cross sections at $\sqrt{s} = 7$ TeV with the ATLAS detector
... in the training pro- cess to dampen statistical fluctuations in the training sample and to avoid ...overtraining. At the preprocessing stage men- tioned above (Sec. VI B ), the ... See full document
50
Measurements of fiducial cross-sections for $t\bar{t}$ production with one or two additional b-jets in pp collisions at $\sqrt{s}$ =8 TeV using the ATLAS detector
... M.G. Alviggi 104a,104b , B.T. Amadio 15 , K. Amako 66 , Y. Amaral Coutinho 24a , C. Amelung 23 , D. Amidei 89 , S.P. Amor Dos Santos 126a,126c , A. Amorim 126a,126b , S. Amoroso 48 , N. Amram 153 , G. Amundsen 23 ... See full document
58
Search for new phenomena with photon+jet events in proton-proton collisions at $ \sqrt{s}=13 $ TeV with the ATLAS detector
... clusters of calorimeter cells using the anti-k t algorithm with radius parameter R = ...in the detector, or identified as arising from non-collision backgrounds, are ... See full document
38
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. ... See full document
29
Determination of the top-quark pole mass using $ t\overline{t} $ + 1-jet events collected with the ATLAS experiment in 7 TeV pp collisions
... R. Walker 100 , W. Walkowiak 142 , C. Wang 33c , F. Wang 174 , H. Wang 15 , H. Wang 40 , J. Wang 42 , J. Wang 33a , K. Wang 87 , R. Wang 6 , S.M. Wang 152 , T. Wang 21 , X. Wang 177 , C. Wanotayaroj 116 , A. ... See full document
40
Measurements of jet vetoes and azimuthal decorrelations in dijet events produced in $pp$ collisions at $\sqrt{s}=7\,\mathrm{TeV}$ using the ATLAS detector
... probe of higher-order QCD effects can be made by studying the azimuthal angle between the jets in the dijet system, ∆ φ ...alters the bal- ance between the partons and produces ... See full document
29
Measurement of jet multiplicity distributions in $\mathrm {t}\overline{\mathrm {t}}$ production in pp collisions at $\sqrt{s} = 7\,\text {TeV} $
... determine the kinematic properties of the tt pair and to identify the two b jets originating from the decay of the top quark and ...In the kinematic ... See full document
41
Measurements of jet charge with dijet events in pp collisions at $\sqrt{s}=8$ TeV
... idea of estimating the charge of a parton from a jet-based observable has a long ...history. The jet charge observable was suggested initially by Field and Feynman ...scattering ... See full document
40
A search for $t\bar{t}$ resonances with the ATLAS detector in 2.05 fb$^{-1}$ of proton-proton collisions at $\sqrt{s}=7$ TeV
... 4, the SM t¯ t and single top backgrounds are simulated using the MC@NLO gen- erator with ...investigate the impact of the choice of PDFs on modelling ... See full document
25
Measurement of the $t\bar{t}Z$ and $t\bar{t}W$ production cross sections in multilepton final states using 3.2 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector
... L.A.M. Wiik-Fuchs 23 , A. Wildauer 103 , F. Wilk 87 , H.G. Wilkens 32 , H.H. Williams 124 , S. Williams 109 , C. Willis 93 , S. Willocq 89 , J.A. Wilson 19 , I. Wingerter-Seez 5 , F. Winklmeier 118 , O.J. ... See full document
42
Search for New Phenomena in $t\bar{t}$ Events With Large Missing Transverse Momentum in Proton-Proton Collisions at $\sqrt{s}=7$ TeV with the ATLAS Detector
... minosity. The data were collected using electron and muon ...ensure the quality of beam conditions, detector performance and data are im- ...samples with full AT- LAS ... See full document
18
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 ... See full document
78
A search for pair-produced resonances in four-jet final states at $\sqrt{s} =$ 13 TeV with the ATLAS detector
... negligible with respect to the detector resolution. This set of samples is also used to interpret the analysis for the case where both top squarks decay into light quarks, since ... See full document
41
Measurement of jet substructure observables in $\mathrm{t\overline{t}}$ events from proton-proton collisions at $\sqrt{s}=$ 13TeV
... be b-tagged. The Combined Secondary Vertex (CSVv2) b tagging algorithm is used at a working point, which has a mean efficiency of 63% for the correct identification ... See full document
55
temas relacionados