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[PDF] Top 20 Search for pair production of heavy vector-like quarks decaying into hadronic final states in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector

Has 10000 "Search for pair production of heavy vector-like quarks decaying into hadronic final states in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector" found on our website. Below are the top 20 most common "Search for pair production of heavy vector-like quarks decaying into hadronic final states in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector".

Search for pair production of heavy vector-like quarks decaying into hadronic final states in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector

Search for pair production of heavy vector-like quarks decaying into hadronic final states in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector

... MES of Russia and NRC KI, Russian Federation; JINR; MESTD, Serbia; MSSR, Slovakia; ARRS and MIZ Š, Slovenia; DST/NRF, South Africa; MINECO, Spain; SRC and Wallenberg Foundation, Sweden; SERI, SNSF and Cantons ... See full document

36

Search for pair production of higgsinos in final states with at least three $b$-tagged jets in $\sqrt{s} = 13$ TeV $pp$ collisions using the ATLAS detector

Search for pair production of higgsinos in final states with at least three $b$-tagged jets in $\sqrt{s} = 13$ TeV $pp$ collisions using the ATLAS detector

... J.J. Lozano Bahilo 172 , H. Lu 61a , N. Lu 103 , Y.J. Lu 62 , H.J. Lubatti 145 , C. Luci 70a,70b , A. Lucotte 56 , C. Luedtke 50 , F. Luehring 63 , I. Luise 132 , W. Lukas 74 , L. Luminari 70a , B. Lund-Jensen 151 , M.S. ... See full document

49

Search for single production of a vector-like quark via a heavy gluon in the $4b$ final state with the ATLAS detector in $pp$ collisions at $\sqrt{s} = 8$ TeV

Search for single production of a vector-like quark via a heavy gluon in the $4b$ final state with the ATLAS detector in $pp$ collisions at $\sqrt{s} = 8$ TeV

... for vector-like quarks in the ATLAS and CMS experiments, in both the pair and single produc- tion processes [ 11 – 22 ], constrain their mass to be above ... See full document

35

Search for single production of vector-like quarks decaying into a b quark and a W boson in proton-proton collisions at $\sqrt s =$ 13 TeV

Search for single production of vector-like quarks decaying into a b quark and a W boson in proton-proton collisions at $\sqrt s =$ 13 TeV

... A search is presented for a heavy vector-like quark, decaying into a b quark and a W boson, which is produced singly in association with a light flavor quark and a ... See full document

32

Search for pair production of vector-like top quarks in events with one lepton, jets, and missing transverse momentum in $ \sqrt{s}=13 $ TeV $pp$ collisions with the ATLAS detector

Search for pair production of vector-like top quarks in events with one lepton, jets, and missing transverse momentum in $ \sqrt{s}=13 $ TeV $pp$ collisions with the ATLAS detector

... J. Barreiro Guimarães da Costa 35a , R. Bartoldus 145 , A.E. Barton 75 , P. Bartos 146a , A. Basalaev 125 , A. Bassalat 119, f , R.L. Bates 56 , S.J. Batista 161 , J.R. Batley 30 , M. Battaglia 139 , M. Bauce 134a,134b , ... See full document

39

Search for long-lived particles in final states with displaced dimuon vertices in $pp$ collisions at $\sqrt{s}=$ 13 TeV with the ATLAS detector

Search for long-lived particles in final states with displaced dimuon vertices in $pp$ collisions at $\sqrt{s}=$ 13 TeV with the ATLAS detector

... Distributions of m µµ and signed r vtx for opposite-charge and same-charge (SS) dimuon vertices satisfying the preselection criteria are shown in Figure 2 ...are the expected contributions ... See full document

48

Search for the production of single vector-like and excited quarks in the $Wt$ final state in $pp$ collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector

Search for the production of single vector-like and excited quarks in the $Wt$ final state in $pp$ collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector

... M. Fanti 91a,91b , A. Farbin 8 , A. Farilla 134a , T. Farooque 12 , S. Farrell 15 , S.M. Farrington 170 , P. Farthouat 30 , F. Fassi 135e , P. Fassnacht 30 , D. Fassouliotis 9 , M. Faucci Giannelli 77 , A. ... See full document

45

Search for direct pair production of the top squark in all-hadronic final states in proton-proton collisions at $\sqrt{s}=8$ TeV with the ATLAS detector

Search for direct pair production of the top squark in all-hadronic final states in proton-proton collisions at $\sqrt{s}=8$ TeV with the ATLAS detector

... numbers of events in the various control regions are included in a profile likelihood fit to determine the SM background estimates in each signal ...(discussed in detail ... See full document

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Search for heavy resonances decaying into a vector boson and a Higgs boson in final states with charged leptons, neutrinos and b quarks at $ \sqrt{s}=13 $ TeV

Search for heavy resonances decaying into a vector boson and a Higgs boson in final states with charged leptons, neutrinos and b quarks at $ \sqrt{s}=13 $ TeV

... predicted in extensions of the SM Higgs sector, such as in two Higgs doublet models (2HDM) [18], which introduce a second scalar doublet in addition to the one from the ... See full document

44

Search for dark matter produced in association with a hadronically decaying vector boson in $pp$ collisions at $\sqrt{s} =$ 13 TeV with the ATLAS detector

Search for dark matter produced in association with a hadronically decaying vector boson in $pp$ collisions at $\sqrt{s} =$ 13 TeV with the ATLAS detector

... categories of jet candidates are built, each using the anti-k ⊥ clustering algorithm [ 22 ...clusters of energy deposits in calorimeter cells seeded by those with energies signific- ... See full document

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Searches for heavy diboson resonances in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

Searches for heavy diboson resonances in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

... on the HVT phenomenological Lagrangian which introduces a new triplet of heavy vector bosons that contains three states with identical masses: the two electrically charged ... See full document

46

Search for direct top squark pair production in final states with two tau leptons in pp collisions at $\sqrt{s}=8$  TeV with the ATLAS detector

Search for direct top squark pair production in final states with two tau leptons in pp collisions at $\sqrt{s}=8$  TeV with the ATLAS detector

... describing the shower shape in the calorimeters and information from the tracking system are used to separate the collimated τ had decay products from the generally broader jets ... See full document

48

Search for top squarks decaying to tau sleptons in $pp$ collisions at  $\sqrt{s}= 13$ TeV with the ATLAS detector

Search for top squarks decaying to tau sleptons in $pp$ collisions at $\sqrt{s}= 13$ TeV with the ATLAS detector

... targeted final state has two tau leptons, two b-quarks and missing transverse ...momentum. The dominant SM background process with this signature is pair production of top ... See full document

33

Search for heavy, top-like quark pair production in the dilepton final state in $pp$ collisions at $\sqrt{s} = 7$ TeV

Search for heavy, top-like quark pair production in the dilepton final state in $pp$ collisions at $\sqrt{s} = 7$ TeV

... feature of the CMS apparatus is a superconducting solenoid, 13 m in length and 6 m in diameter, which provides an axial magnetic field of ...Within the field volume are ... See full document

27

Search for dark matter in association with a Higgs boson decaying to $b$-quarks in $pp$ collisions at $\sqrt s=13$ TeV with the ATLAS detector

Search for dark matter in association with a Higgs boson decaying to $b$-quarks in $pp$ collisions at $\sqrt s=13$ TeV with the ATLAS detector

... immersed in a 2 T axial magnetic field provided by a thin superconducting solenoid, consisting of silicon pixel and microstrip detectors, which provide precision tracking in the pseu- ... See full document

21

Search for $WW/WZ$ resonance production in $\ell \nu qq$ final states in $pp$ collisions at $\sqrt{s} =$ 13 TeV with the ATLAS detector

Search for $WW/WZ$ resonance production in $\ell \nu qq$ final states in $pp$ collisions at $\sqrt{s} =$ 13 TeV with the ATLAS detector

... events with a W boson produced in association with jets ...sources of SM background include the production of top quarks, multijets, dibo- sons and Z ...bosons ... See full document

44

Search for the standard model Higgs boson produced in association with top quarks and decaying into a $b\bar{b}$ pair in $pp$ collisions at $\sqrt{s}$ = 13  TeV with the ATLAS detector

Search for the standard model Higgs boson produced in association with top quarks and decaying into a $b\bar{b}$ pair in $pp$ collisions at $\sqrt{s}$ = 13  TeV with the ATLAS detector

... for the very successful operation of the LHC, as well as the support staff from our institutions without whom ATLAS could not be operated ...acknowledge the support of ... See full document

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Search for heavy Majorana neutrinos with the ATLAS detector in pp collisions at $ \sqrt{s}=8 $ TeV

Search for heavy Majorana neutrinos with the ATLAS detector in pp collisions at $ \sqrt{s}=8 $ TeV

... The search is guided by two theoretical models. In the first model, the SM is extended in the simplest way to include right-handed neutrinos [ 8 ], such that light ... See full document

44

A search for pair-produced resonances in four-jet final states at $\sqrt{s} =$ 13 TeV with the ATLAS detector

A search for pair-produced resonances in four-jet final states at $\sqrt{s} =$ 13 TeV with the ATLAS detector

... ratio into ¯b ¯s. Its width is expected to be small, and negligible with respect to the detector ...set of samples is also used to interpret the analysis for the ... See full document

41

Search for direct top-squark pair production in final states with two leptons in pp collisions at $\sqrt{s} =$ 8TeV with the ATLAS detector

Search for direct top-squark pair production in final states with two leptons in pp collisions at $\sqrt{s} =$ 8TeV with the ATLAS detector

... used in the prediction are defined as follows: r is the probability for real leptons satisfying the loose selection criteria to also pass the tight selection and f is the ... See full document

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