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[PDF] Top 20 Search for supersymmetry in the all-hadronic final state using top quark tagging in pp collisions at root s=13 TeV

Has 10000 "Search for supersymmetry in the all-hadronic final state using top quark tagging in pp collisions at root s=13 TeV" found on our website. Below are the top 20 most common "Search for supersymmetry in the all-hadronic final state using top quark tagging in pp collisions at root s=13 TeV".

Search for supersymmetry in the all-hadronic final state using top quark tagging in pp collisions at root s=13 TeV

Search for supersymmetry in the all-hadronic final state using top quark tagging in pp collisions at root s=13 TeV

... Germany; the General Secretariat for Research and Technology, Greece; the National Scientific Research Foundation, and National Innovation Office, Hungary; the Department of Atomic Energy and ... See full document

33

Search for direct production of supersymmetric partners of the top quark in the all-jets final state in proton-proton collisions at $ \sqrt{s}=13 $ TeV

Search for direct production of supersymmetric partners of the top quark in the all-jets final state in proton-proton collisions at $ \sqrt{s}=13 $ TeV

... S. Abdullin, M. Albrow, G. Apollinari, A. Apresyan, A. Apyan, S. Banerjee, L.A.T. Bauerdick, A. Beretvas, J. Berryhill, P.C. Bhat, G. Bolla, K. Burkett, J.N. Butler, A. Canepa, G.B. Cerati, H.W.K. Cheung, ... See full document

58

Search for natural supersymmetry in events with top quark pairs and photons in pp collisions at $\sqrt{s} =$ 8 TeV

Search for natural supersymmetry in events with top quark pairs and photons in pp collisions at $\sqrt{s} =$ 8 TeV

... a search for natural gauge-mediated supersymmetry (SUSY) in a scenario in which the top squark is the lightest squark, the next-to-lightest SUSY particle is a ... See full document

36

Search for vector-boson resonances decaying to a top quark and bottom quark in the lepton plus jets final state in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector

Search for vector-boson resonances decaying to a top quark and bottom quark in the lepton plus jets final state in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector

... satisfies the lepton identification cri- teria. The simulation of this background source is challenging as it suffers from large systematic uncertainties and does not reli- ably reproduce the observed ... See full document

24

Search for supersymmetry in hadronic final states with missing transverse energy using the variables $\alpha_T$ and b-quark multiplicity in pp collisions at $\sqrt s=8$ TeV

Search for supersymmetry in hadronic final states with missing transverse energy using the variables $\alpha_T$ and b-quark multiplicity in pp collisions at $\sqrt s=8$ TeV

... signatures in final states with multiple b-quark jets, a method that improves the statistical power of the predictions from simulation, particularly for n b ≥ 2, is ...employed. ... See full document

45

Measurement of the top-quark mass in all-jets tt events in pp collisions at root s=7 TeV

Measurement of the top-quark mass in all-jets tt events in pp collisions at root s=7 TeV

... estimate the com- position of the data sample, to determine and calibrate the ideograms, and to evaluate the systematic ...uncertainties. The t¯t signal events have been generated for ... See full document

24

Search for heavy resonances decaying to a top quark and a bottom quark in the lepton+jets final state in proton–proton collisions at 13 TeV

Search for heavy resonances decaying to a top quark and a bottom quark in the lepton+jets final state in proton–proton collisions at 13 TeV

... . The transverse components of the neutrino momentum are set to the  p T miss and the longitudinal component pν z is calculated by constraining the invariant mass of the lepton ... See full document

25

Search for direct pair production of supersymmetric top quarks decaying to all-hadronic final states in pp collisions at $\sqrt{s} = 8\;\text {TeV} $

Search for direct pair production of supersymmetric top quarks decaying to all-hadronic final states in pp collisions at $\sqrt{s} = 8\;\text {TeV} $

... line in the lower pane of each plot in Figs. 12 and 13 labelled “MC without ...resents the sum of the MC contributions, relative to the prediction, prior to weighting by ... See full document

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Search for new physics in top quark production in dilepton final states in proton-proton collisions at root s=13 TeV

Search for new physics in top quark production in dilepton final states in proton-proton collisions at root s=13 TeV

... bottom quark (“bjets”) are analyzed. The search is sensitive to new physics contributions to tW and t¯t production, and the six effective couplings, C G , C (3) φq , C tW , C tG , C uG , and C ... See full document

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Search for supersymmetry in a final state containing two photons and missing transverse momentum in $\sqrt{s}$ = 13 TeV $pp$ collisions at the LHC using the ATLAS detector

Search for supersymmetry in a final state containing two photons and missing transverse momentum in $\sqrt{s}$ = 13 TeV $pp$ collisions at the LHC using the ATLAS detector

... J. Del Peso 83 , T. Del Prete 124a,124b , D. Delgove 117 , F. Deliot 136 , C.M. Delitzsch 51 , A. Dell’Acqua 32 , L. Dell’Asta 24 , M. Dell’Orso 124a,124b , M. Della Pietra 104a,k , D. della Volpe 51 , M. Delmastro 5 , ... See full document

34

Search for $W' \rightarrow tb$ decays in the hadronic final state using pp collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

Search for $W' \rightarrow tb$ decays in the hadronic final state using pp collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

... J-Y. Hostachy 57 , A. Hostiuc 140 , S. Hou 153 , A. Hoummada 137a , J. Howarth 87 , J. Hoya 74 , M. Hrabovsky 117 , J. Hrdinka 32 , I. Hristova 17 , J. Hrivnac 119 , T. Hryn’ova 5 , A. Hrynevich 96 , P.J. Hsu 63 , ... See full document

22

Search for top quark partners with charge 5/3 in proton-proton collisions at root s=13 TeV

Search for top quark partners with charge 5/3 in proton-proton collisions at root s=13 TeV

... b)] in (upper) 0 or (lower) ≥1 W-tagged jets and (left) 1 or (right) ≥2 b-tagged jets categories with 0 t-tagged jets for combined electron and muon samples, at the final selection ...level. ... See full document

44

Search for top-squark pair production in the single-lepton final state in pp collisions at $\sqrt{s}$ = 8 TeV

Search for top-squark pair production in the single-lepton final state in pp collisions at $\sqrt{s}$ = 8 TeV

... successful at describing particle physics phenom- ...as the hierarchy problem, where fine-tuned cancellations of large quantum corrections are required in order for the Higgs boson to have a ... See full document

61

Search for the pair production of light top squarks in the e(+/-)mu(-/+) final state in proton-proton collisions at root s=13 TeV

Search for the pair production of light top squarks in the e(+/-)mu(-/+) final state in proton-proton collisions at root s=13 TeV

... After the event selection, the vast majority of events (≈98%) come from top quark pro- duction processes (tt, ...a top squark mass similar to that of the top quark, ... See full document

41

Inclusive search for supersymmetry using the razor variables in $pp$ collisions at $\sqrt{s}=7$ TeV

Inclusive search for supersymmetry using the razor variables in $pp$ collisions at $\sqrt{s}=7$ TeV

... inclusive search for new heavy particles. The analysis is designed to be largely independent of the details of the decay chains and measures devi- ations from the characteristic ... See full document

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Search for supersymmetry in pp collisions at $ \sqrt{s}=13 $ TeV in the single-lepton final state using the sum of masses of large-radius jets

Search for supersymmetry in pp collisions at $ \sqrt{s}=13 $ TeV in the single-lepton final state using the sum of masses of large-radius jets

... from the Marie-Curie program and the European Research Council and EPLANET (European Union); the Leventis Foundation; the ...tion; the Alexander von Humboldt Foundation; the ... See full document

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Inclusive search for supersymmetry in pp collisions at root s=13 TeV using razor variables and boosted object identification in zero and one lepton final states

Inclusive search for supersymmetry in pp collisions at root s=13 TeV using razor variables and boosted object identification in zero and one lepton final states

... momentum. The razor kinematic variables are sensitive to large mass differences between the parent particle and the invisible particles of a decay chain and help to identify the presence of ... See full document

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Search for top squark pair production in pp collisions at root s=13 TeV using single lepton events

Search for top squark pair production in pp collisions at root s=13 TeV using single lepton events

... assess all relevant theoretical and experimental uncertainties that can affect the shapes of the kinematic distributions of our signal region definitions by recomputing acceptances after modifying ... See full document

42

Search for Z gamma resonances using leptonic and hadronic final states in proton-proton collisions at root s=13 TeV

Search for Z gamma resonances using leptonic and hadronic final states in proton-proton collisions at root s=13 TeV

... detector at the LHC in 2016. Two decay modes of the Z boson are ...investigated. In the leptonic channels, the Z boson candidates are reconstructed using electron ... See full document

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Search for resonances decaying into top-quark pairs using fully hadronic decays in $pp$ collisions with ATLAS at $\sqrt{s}=7$ TeV

Search for resonances decaying into top-quark pairs using fully hadronic decays in $pp$ collisions with ATLAS at $\sqrt{s}=7$ TeV

... events in the signal region (subsample P) is calculated with an iterative method that uses the lack of correlation in b-tagging efficiencies between the leading and recoil ... See full document

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