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[PDF] Top 20 Search for standard model production of four top quarks with same-sign and multilepton final states in proton–proton collisions at $\sqrt{s} = 13\,\text {TeV} $

Has 10000 "Search for standard model production of four top quarks with same-sign and multilepton final states in proton–proton collisions at $\sqrt{s} = 13\,\text {TeV} $" found on our website. Below are the top 20 most common "Search for standard model production of four top quarks with same-sign and multilepton final states in proton–proton collisions at $\sqrt{s} = 13\,\text {TeV} $".

Search for standard model production of four top quarks with same-sign and multilepton final states in proton–proton collisions at $\sqrt{s} = 13\,\text {TeV} $

Search for standard model production of four top quarks with same-sign and multilepton final states in proton–proton collisions at $\sqrt{s} = 13\,\text {TeV} $

... generated with up to two additional partons, and the WZ, ZZ and ttH samples, which are generated with no additional partons with the POWHEG BOX v2 [25, 26] ...sample with Z/γ ∗ → ... See full document

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Search for new physics in same-sign dilepton events in proton–proton collisions at $\sqrt{s} = 13\,\text {TeV} $

Search for new physics in same-sign dilepton events in proton–proton collisions at $\sqrt{s} = 13\,\text {TeV} $

... Multiple search regions are defined by classifying events in terms of missing trans- verse momentum, the scalar sum of jet transverse momenta, the transverse mass asso- ciated with a W ... See full document

40

Search for physics beyond the standard model in events with two leptons of same sign, missing transverse momentum, and jets in proton–proton collisions at $\sqrt{s} = 13\,\text {TeV} $

Search for physics beyond the standard model in events with two leptons of same sign, missing transverse momentum, and jets in proton–proton collisions at $\sqrt{s} = 13\,\text {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

42

Search for new phenomena with multiple charged leptons in proton–proton collisions at $\sqrt{s}= 13$ $\,\text {TeV}$

Search for new phenomena with multiple charged leptons in proton–proton collisions at $\sqrt{s}= 13$ $\,\text {TeV}$

... Center of Excellence in Physics, the Institute for the Promotion of Teaching Science and Technology of Thailand, Special Task Force for Activating Research and the National Sci- ... See full document

42

Search for doubly charged Higgs boson production in multi-lepton final states with the ATLAS detector using proton–proton collisions at $\sqrt{s}=13\,\text {TeV}$

Search for doubly charged Higgs boson production in multi-lepton final states with the ATLAS detector using proton–proton collisions at $\sqrt{s}=13\,\text {TeV}$

... A. Sapronov 68 , J.G. Saraiva 128a,128d , B. Sarrazin 23 , O. Sasaki 69 , K. Sato 164 , E. Sauvan 5 , G. Savage 80 , P. Savard 161,d , N. Savic 103 , C. Sawyer 133 , L. Sawyer 82,u , J. Saxon 33 , C. Sbarra 22a , A. ... See full document

52

Search for Standard Model Production of Four Top Quarks in the Lepton + Jets Channel in pp Collisions at $\sqrt{s}$ = 8 TeV

Search for Standard Model Production of Four Top Quarks in the Lepton + Jets Channel in pp Collisions at $\sqrt{s}$ = 8 TeV

... expected in the data. Because of the very large tt background, the direct obser- vation of events leading to a measurement of σ tttt is ...However, in many models beyond the SM (BSM) ... See full document

29

Search for black holes and sphalerons in high-multiplicity final states in proton-proton collisions at $ \sqrt{s}=13 $ TeV

Search for black holes and sphalerons in high-multiplicity final states in proton-proton collisions at $ \sqrt{s}=13 $ TeV

... collected with the CMS experiment at the LHC in proton-proton collisions at a center- of-mass energy of 13 TeV in ...2016. ... See full document

47

Search for direct pair production of scalar top quarks in the single- and dilepton channels in proton-proton collisions at $ \sqrt{s}=8 $ TeV

Search for direct pair production of scalar top quarks in the single- and dilepton channels in proton-proton collisions at $ \sqrt{s}=8 $ TeV

... 1 of pp collision data taken ats = 8 TeV, we search for direct top squark pair production in both single-lepton and dilepton final ... See full document

46

Search for physics beyond the standard model in final states with a lepton and missing transverse energy in proton-proton collisions at sqrt(s) = 8 TeV

Search for physics beyond the standard model in final states with a lepton and missing transverse energy in proton-proton collisions at sqrt(s) = 8 TeV

... accordance with previous analyses [15–19, 21–24], no interference with the SM W boson is ...absence of interference can be interpreted as the result of a V+A coupling of the SSM W 0 ... See full document

57

Search for leptoquarks coupled to third-generation quarks in proton-proton collisions at $\sqrt{s}=$ 13 TeV

Search for leptoquarks coupled to third-generation quarks in proton-proton collisions at $\sqrt{s}=$ 13 TeV

... Three of the most significant measured deviations from standard model predictions, the enhanced decay rate for B → D ðÞ τν, hints of lepton universality violation in B → K ðÞ ll ... See full document

19

Search for pair production of vector-like T and B quarks in single-lepton final states using boosted jet substructure in proton-proton collisions at  $\sqrt{s}=13$ TeV

Search for pair production of vector-like T and B quarks in single-lepton final states using boosted jet substructure in proton-proton collisions at $\sqrt{s}=13$ TeV

... boson) and a third generation quark. This search is performed in final states with one charged lepton and several jets, exploiting techniques to identify W or Higgs bosons ... See full document

44

Search for high-mass resonances in dilepton final states in proton-proton collisions at $\sqrt{s}=$ 13 TeV

Search for high-mass resonances in dilepton final states in proton-proton collisions at $\sqrt{s}=$ 13 TeV

... A search is presented for new high-mass resonances decaying into electron or muon ...The search uses proton-proton collision data at a centre-of-mass energy of 13 ... See full document

42

Search for top squarks decaying via four-body or chargino-mediated modes in single-lepton final states in proton-proton collisions at $\sqrt{s} =$ 13 TeV

Search for top squarks decaying via four-body or chargino-mediated modes in single-lepton final states in proton-proton collisions at $\sqrt{s} =$ 13 TeV

... phenomena, in particular supersymmetry (SUSY) [1–6], are among the main objectives of the physics programme at the CERN ...one of the most promising extensions of the standard ... See full document

44

Search for single production of vector-like quarks decaying to a Z boson and a top or a bottom quark in proton-proton collisions at $ \sqrt{s}=13 $ TeV

Search for single production of vector-like quarks decaying to a Z boson and a top or a bottom quark in proton-proton collisions at $ \sqrt{s}=13 $ TeV

... discovery of a Higgs boson [1–3] with a mass of 125 GeV [4] by the ATLAS and CMS experiments confirmed the success of the standard model (SM) in predicting a wide ... See full document

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Search for black holes in high-multiplicity final states in proton-proton collisions at $ \sqrt{s}=$13 TeV

Search for black holes in high-multiplicity final states in proton-proton collisions at $ \sqrt{s}=$13 TeV

... A search for new physics in energetic, high-multiplicity final states has been performed using protonproton collision data collected with the CMS detector at a ... See full document

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Observation of electroweak production of same-sign W boson pairs in the two jet and two same-sign lepton final state in proton-proton collisions at $\sqrt{s} = $ 13 TeV

Observation of electroweak production of same-sign W boson pairs in the two jet and two same-sign lepton final state in proton-proton collisions at $\sqrt{s} = $ 13 TeV

... decays of heavy quarks, hadrons misidentified as leptons, and electrons from photon conversions are sup- pressed by the identification and isolation requirements imposed on electrons ... See full document

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Searches for pair production of charginos and top squarks in final states with two oppositely charged leptons in proton-proton collisions at $\sqrt{s}=$ 13 TeV

Searches for pair production of charginos and top squarks in final states with two oppositely charged leptons in proton-proton collisions at $\sqrt{s}=$ 13 TeV

... A search for pair production of supersymmetric particles in events with two oppo- sitely charged leptons (electrons or muons) and missing transverse momentum is ...luminosity ... See full document

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Search for standard model production of four top quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV

Search for standard model production of four top quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV

... 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

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Search for electroweak production of charginos and neutralinos in multilepton final states in proton-proton collisions at $\sqrt{s}=$ 13 TeV

Search for electroweak production of charginos and neutralinos in multilepton final states in proton-proton collisions at $\sqrt{s}=$ 13 TeV

... The standard model (SM) describes the vast majority of particle physics ...multitude of challenges from precision ...existence of such phenomena. A recent triumph of the SM is ... See full document

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Search for Evidence of the Type-III Seesaw Mechanism in Multilepton Final States in Proton-Proton Collisions at $\sqrt{s}=13\text{ }\text{ }\mathrm{TeV}$

Search for Evidence of the Type-III Seesaw Mechanism in Multilepton Final States in Proton-Proton Collisions at $\sqrt{s}=13\text{ }\text{ }\mathrm{TeV}$

... example of the complete background estimation, ...predictions and the observed events with three leptons, OSSF1, above Z, and for events with four or more leptons, OSSF1, along ... See full document

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