[PDF] Top 20 Search for heavy resonances decaying to tau lepton pairs in proton-proton collisions at s√=13 TeV
Has 10000 "Search for heavy resonances decaying to tau lepton pairs in proton-proton collisions at s√=13 TeV" found on our website. Below are the top 20 most common "Search for heavy resonances decaying to tau lepton pairs in proton-proton collisions at s√=13 TeV".
Search for heavy resonances decaying to tau lepton pairs in proton-proton collisions at s√=13 TeV
... S. Abdullin, M. Albrow, G. Apollinari, S. Banerjee, L.A.T. Bauerdick, A. Beretvas, J. Berryhill, P.C. Bhat, G. Bolla, K. Burkett, J.N. Butler, H.W.K. Cheung, F. Chlebana, S. Cihangir † , M. ... See full document
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Search for heavy resonances decaying to a Z boson and a photon in pp collisions at √s=13 TeV with the ATLAS detector
... inelastic proton–proton collisions (re- ferred to as pile-up) are simulated with the soft QCD processes of Pythia ...photon, lepton and jet reconstruction and selection efficiencies, and their ... See full document
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Search for heavy resonances decaying to a Z boson and a photon in pp collisions at root s=13 TeV with the ATLAS detector
... inelastic proton–proton collisions (referred to as pile-up) are simulated with the soft QCD processes of Pythia ...photon, lepton and jet reconstruction and selection e ffi ciencies, and their ... See full document
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Search for heavy neutrinos or third-generation leptoquarks in final states with two hadronically decaying τ leptons and two jets in proton-proton collisions at √s=13 TeV
... jet background prediction is dominated by the statistical uncertainty of the data used in the control regions (about 27%). The contamination from other backgrounds in the QCD multijet control regions has a negligible ... See full document
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Search for heavy ZZ resonances in the ℓ+ℓ−ℓ+ℓ− and ℓ+ℓ−νν¯ final states using proton–proton collisions at s√=13 TeV with the ATLAS detector
... D. M. Portillo Quintero 83 , S. Pospisil 130 , K. Potamianos 45 , I. N. Potrap 68 , C. J. Potter 30 , H. Potti 11 , T. Poulsen 84 , J. Poveda 32 , M. E. Pozo Astigarraga 32 , P. Pralavorio 88 , A. Pranko 16 , ... See full document
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Search for long-lived neutral particles decaying into lepton-jets in 20.3 fb−1 proton-proton collisions at √s = 8 TeV with the ATLAS detector
... and decaying far from the primary vertex to pairs of electrons / muons / ...A lepton-jet gun Monte Carlo generator has been developed to optimize search criteria and to produce detection ... See full document
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ATLAS search for a heavy gauge boson decaying to a charged lepton and a neutrino in pp collisions at √s=7 TeV
... L. Kashif 173 , G. Kasieczka 58b , R.D. Kass 109 , A. Kastanas 14 , M. Kataoka 5 , Y. Kataoka 155 , E. Katsoufis 10 , J. Katzy 42 , V. Kaushik 7 , K. Kawagoe 69 , T. Kawamoto 155 , G. Kawamura 81 , M.S. Kayl 105 , ... See full document
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Search for heavy ZZ resonances in the l(+) l(-) l(+) l(-) and l(+) l(-) nu(nu)over-bar final states using proton-proton collisions at root s=13 TeV with the ATLAS detector
... N. Barlow 30 , S. L. Barnes 36c , B. M. Barnett 133 , R. M. Barnett 16 , Z. Barnovska-Blenessy 36a , A. Baroncelli 136a , G. Barone 25 , A. J. Barr 122 , L. Barranco Navarro 170 , F. Barreiro 85 , J. Barreiro ... See full document
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Search for resonant WZ production in the fully leptonic final state in proton–proton collisions at √s =13 TeV with the ATLAS detector
... diboson resonances provide an essential test of theories of electroweak symmetry breaking beyond the Standard Model ...Vector resonances are predicted in various BSM sce- narios, such as in extended gauge ... See full document
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Search for high-mass Zγ resonances in e+e−γ and μ+μ−γ final states in proton-proton collisions at s√=8 and 13 TeV
... high lepton identification efficiency even for highly-boosted Z boson decays, as expected in the decay of high-mass ...the lepton is quantified by summing the transverse momenta of the relevant PF ... See full document
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Search for new phenomena with photon+jet events in proton proton collisions at √s=13 TeV with the ATLAS detector
... A search is performed for the production of high-mass resonances decaying into a photon and a jet in ...of proton-proton collisions at a centre-of-mass energy of √ s = ... See full document
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Search for heavy lepton resonances decaying to a Z boson and a lepton in pp collisions at s=8 TeV with the ATLAS detector
... the search are interpreted in the context of vector-like lepton [ 16] and type-III seesaw [17] scenarios in which the new heavy leptons decay through mixing with electrons or muons (`) induced by ... See full document
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Search for high-mass diphoton resonances in proton-proton collisions at 13 TeV and combination with 8 TeV search
... The photon candidates in an event are grouped into all pos- sible pairs. At least one photon candidate in the pair must have | η | < 1 . 44, i.e., be reconstructed in the barrel. Events with both photons in the ... See full document
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Search for narrow resonances in dilepton mass spectra in proton-proton collisions at root s=13 TeV and combination with 8 TeV data
... reconstruction, lepton identification and, in the case of muons, the effect of the trigger, is determined from Monte Carlo (MC) ...bosons decaying to e + e − and μ + μ − pairs, are employed to ... See full document
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Search for heavy particles decaying into top-quark pairs using lepton-plus-jets events in proton-proton collisions at root s=13 TeV with the ATLAS detector
... M. Schernau 169 , C. Schiavi 56b,56a , S. Schier 143 , L. K. Schildgen 24 , Z. M. Schillaci 26 , E. J. Schioppa 35 , M. Schioppa 40b,40a , K. E. Schleicher 53 , S. Schlenker 35 , K. R. Schmidt-Sommerfeld ... See full document
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Search for resonances in the mass distribution of jet pairs with one or two jets identified as b-jets in proton–proton collisions at √s=13 TeV with the ATLAS detector
... M. Medinnis 44 , S. Meehan 139 , S. Mehlhase 101 , A. Mehta 76 , K. Meier 60a , C. Meineck 101 , B. Meirose 43 , D. Melini 167 , B.R. Mellado Garcia 146c , M. Melo 145a , F. Meloni 18 , A. Mengarelli 22a , ... See full document
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Search for squarks and gluinos in events with hadronically decaying tau leptons, jets and missing transverse momentum in proton–proton collisions at √s=13 TeV recorded with the ATLAS detector
... J. Nielsen 138 , A. Nikiforov 17 , V. Nikolaenko 131,af , I. Nikolic-Audit 82 , K. Nikolopoulos 19 , J. K. Nilsen 120 , P. Nilsson 27 , Y. Ninomiya 158 , A. Nisati 133a , R. Nisius 102 , T. Nobe 158 , M. Nomachi 119 , I. ... See full document
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Search for single production of vector like quarks decaying into a b quark and a W boson in proton–proton collisions at 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 b ...of proton–proton ... See full document
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Measurement of tau polarisation in Z/gamma* -> tau tau decays in proton-proton collisions at root s=8 TeV with the ATLAS detector
... R. Cherkaoui El Moursli 137e , E. Cheu 7 , K. Cheung 63 , L. Chevalier 138 , V. Chiarella 50 , G. Chiarelli 126a,126b , G. Chiodini 76a , A. S. Chisholm 32 , A. Chitan 28b , Y. H. Chiu 172 , M. V. Chizhov 68 , K. ... See full document
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Search for excited electrons singly produced in proton-proton collisions at root s=13 TeV with the ATLAS experiment at the LHC
... D. Pohl 24 , I. Pokharel 52 , G. Polesello 69a , A. Poley 18 , A. Policicchio 71a,71b , R. Polifka 36 , A. Polini 23b , C. S. Pollard 45 , V. Polychronakos 29 , D. Ponomarenko 111 , L. Pontecorvo 36 , G. A. ... See full document
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