[PDF] Top 20 Search for resonant diboson production in the $\mathrm {\ell \ell }q\bar{q}$ final state in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector
Has 10000 "Search for resonant diboson production in the $\mathrm {\ell \ell }q\bar{q}$ final state in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector" found on our website. Below are the top 20 most common "Search for resonant diboson production in the $\mathrm {\ell \ell }q\bar{q}$ final state in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector".
Search for resonant diboson production in the $\mathrm {\ell \ell }q\bar{q}$ final state in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector
... acknowledge the support of ANPCyT, Argentina; Yer- PhI, Armenia; ARC, Australia; BMWFW and FWF, Aus- tria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, ... See full document
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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
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Search for Scalar Charm Quark Pair Production in $pp$ Collisions at $\sqrt{s}=$ 8 TeV with the ATLAS Detector
... dedicated search for pair production of scalar partners of charm quarks are re- ...ported. The search is based on an integrated luminosity of ...of pp collisions at √ ... See full document
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Search for resonant $WZ$ production in the fully leptonic final state in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector
... For the HVT interpretation, W → W Z samples were gener- ...provided in Ref. [ 15 ], are used. In Model A, weakly coupled vector resonances arise from an exten- sion of the SM gauge group [ ... See full document
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Search for Higgs boson pair production in the $b\bar{b}b\bar{b}$ final state from pp collisions at $\sqrt{s} = 8$ TeVwith the ATLAS detector
... and the other is related to the e fficiency for b-tagging ...jets, the following uncertainties are accounted for: jet energy scale and resolution, as well as jet mass scale (JMS) and resolution ... See full document
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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
... clusters in the EM calorimeter and matched to tracks in the inner ...indicate the electromagnetic cluster energy and pseudorapid- ity, respectively, and η track the track ... See full document
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Measurement of event-shape observables in $Z \rightarrow \ell ^{+} \ell ^{-}$ events in $pp$ collisions at $\sqrt{s}=$ 7 TeV with the ATLAS detector at the LHC
... Since the UE is dominated by low-scale strong-force interactions, in which the strong coupling strength diverges and perturbative methods of quantum chromodynamics (QCD) lose predictivity, it is ... See full document
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Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
... The ATLAS detector is a general-purpose particle detector, de- scribed in detail in ...inner detector sur- rounded by a 2 T superconducting solenoid, electromagnetic and ... See full document
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Search for heavy resonances decaying to a $W$ or $Z$ boson and a Higgs boson in the $q\bar{q}^{(\prime)}b\bar{b}$ final state in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector
... J. Boudreau 127 , J. Bou ffard 2 , E.V. Bouhova-Thacker 75 , D. Boumediene 37 , C. Bourdarios 119 , S.K. Boutle 56 , A. Boveia 113 , J. Boyd 32 , I.R. Boyko 68 , J. Bracinik 19 , A. Brandt 8 , G. Brandt 57 , O. ... See full document
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Observation of the Z$\to\psi\ell^+\ell^-$ decay in pp collisions at $\sqrt{s}=$ 13 TeV
... sistent with the standard model, as well as upper limits on the branching fraction for anoma- lous production ...No resonant structure in the four-lepton decay has yet ... See full document
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Searches for heavy $ZZ$ and $ZW$ resonances in the $\ell\ell qq$ and $\nu\nu qq$ final states in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
... processes. The main background sources are Z and W bosons produced in association with jets (Z+jets and W+jets), with significant contributions from top quark production (both t¯t pair ... See full document
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Search for the electroweak production of supersymmetric particles in $\sqrt{s}$=8 TeV $pp$ collisions with the ATLAS detector
... The ATLAS experiment has performed extensive searches for the electroweak production of charginos, neutralinos, and ...extends the search for electroweak supersymmetry ... See full document
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Search for resonant top plus jet production in $t\bar{t}$ + jets events with the ATLAS detector in $pp$ collisions at $\sqrt{s}=7$ TeV
... R. Alon 172 , A. Alonso 79 , F. Alonso 70 , B. Alvarez Gonzalez 88 , M.G. Alviggi 102a,102b , K. Amako 65 , C. Amelung 23 , V.V. Ammosov 128, ∗ , S.P. Amor Dos Santos 124a , A. Amorim 124a,b , N. Amram 153 , C. ... See full document
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Search for resonant diboson production in the WW/WZ→ℓνjj decay channels with the ATLAS detector at $\sqrt{s}$ = 7 TeV
... A search for resonant diboson production using a data sample corresponding to ...by the ATLAS experiment at the Large Hadron Collider in pp ... See full document
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Search for diboson resonances with boson-tagged jets in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
... In the HVT phenomenological Lagrangian model, a new heavy vector triplet (W , Z ) is introduced, with the new gauge bosons degenerate in mass (also denoted by V in ... See full document
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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
... K. Motohashi 156 , R. Mount 142 , E. Mountricha 25 , S.V. Mouraviev 95 ,∗ , E.J.W. Moyse 86 , S. Muanza 85 , R.D. Mudd 18 , F. Mueller 100 , J. Mueller 124 , R.S.P. Mueller 99 , T. Mueller 28 , D. Muenstermann 72 ... See full document
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Search for anomalous couplings in boosted $\mathrm{ WW/WZ }\to\ell\nu\mathrm{ q \bar{q} }$ production in proton-proton collisions at $\sqrt{s} =$ 8 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 $WW/WZ$ resonance production in $\ell \nu qq$ final states in $pp$ collisions at $\sqrt{s} =$ 13 TeV with the ATLAS detector
... L.K. Gladilin 101 , C. Glasman 85 , J. Glatzer 13 , P.C.F. Glaysher 45 , A. Glazov 45 , M. Goblirsch-Kolb 25 , J. Godlewski 42 , S. Goldfarb 91 , T. Golling 52 , D. Golubkov 132 , A. Gomes 128a,128b,128d , R. ... See full document
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Search for new phenomena in the $W W$ to $\ell \nu \ell$' $\nu$' final state in $pp$ collisions at $\sqrt{s}=7$ 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 ANPCyT, ... See full document
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Measurement of the $k_\mathrm{t}$ splitting scales in $Z \to \ell\ell$ events in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector
... A.A. O’Rourke 45 , V. O’Shea 56 , F.G. Oakham 31,d , H. Oberlack 103 , T. Obermann 23 , J. Ocariz 83 , A. Ochi 70 , I. Ochoa 38 , J.P. Ochoa-Ricoux 34a , S. Oda 73 , S. Odaka 69 , H. Ogren 64 , A. Oh 87 , ... See full document
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