[PDF] Top 20 Search for doubly charged Higgs boson production in multi-lepton final states with the ATLAS detector using proton–proton collisions at $\sqrt{s}=13\,\text {TeV}$
Has 10000 "Search for doubly charged Higgs boson production in multi-lepton final states with the ATLAS detector using proton–proton collisions at $\sqrt{s}=13\,\text {TeV}$" found on our website. Below are the top 20 most common "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 $\sqrt{s}=13\,\text {TeV}$
... J.T. Baines 133 , M. Bajic 39 , O.K. Baker 179 , P.J. Bakker 109 , E.M. Baldin 111,c , P. Balek 175 , F. Balli 138 , W.K. Balunas 124 , E. Banas 42 , A. Bandyopadhyay 23 , Sw. Banerjee 176,e , A.A.E. Bannoura 178 , L. ... See full document
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Search for new phenomena with multiple charged leptons in proton–proton collisions at $\sqrt{s}= 13$ $\,\text {TeV}$
... ; the Thailand 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 ... 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 $\sqrt{s} = 13$ $\text {TeV}$ with the ATLAS detector
... acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWFW and FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, Chile; ... See full document
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Search for pair production of Higgs bosons in the $b\bar{b}b\bar{b}$ final state using proton--proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector
... M. Düren 54 , A. Durglishvili 53b , D. Duschinger 46 , B. Dutta 44 , M. Dyndal 44 , C. Eckardt 44 , K.M. Ecker 102 , R.C. Edgar 91 , N.C. Edwards 48 , T. Eifert 32 , G. Eigen 15 , K. Einsweiler 16 , T. Ekelof 165 , M. El ... 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
... singly charged scalar resonance. The model extends the Higgs sector by including one real and one complex triplet, while preserving custodial symmetry, ensuring that the parame- ter ρ = ... See full document
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Search for pair production of Higgs bosons in the $b\bar{b}b\bar{b}$ final state using proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector
... S.K. Radhakrishnan 155 , P. Rados 105 , F. Ragusa 71a,71b , G. Rahal 53 , J.A. Raine 101 , S. Rajagopalan 27b , T. Rashid 131 , S. Raspopov 6 , M.G. Ratti 71a,71b , D.M. Rauch 48 , F. Rauscher 115 , ... See full document
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Search for heavy charged long-lived particles in proton-proton collisions at $\sqrt{s} = 13$ TeV using an ionisation measurement with the \mbox{ATLAS} detector
... a search for heavy charged long-lived particles produced in proton–proton collisions at √ s = 13 TeV at the LHC using a data ... See full document
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Search for doubly-charged Higgs bosons in like-sign dilepton final states at $\sqrt{s}=7$ TeV with the ATLAS detector
... A search for doubly-charged Higgs bosons decaying to pairs of electrons and/or muons is pre- ...sented. The search is performed using a data sample corresponding to an ... See full document
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Search for WH production with a light Higgs boson decaying to prompt electron-jets in proton-proton collisions at $\sqrt{s}$=7 TeV with the ATLAS detector
... The ATLAS detector [27] is a multi-purpose particle physics detector with forward- backward symmetric cylindrical ...geometry‡. The inner detector (ID) provides ... See full document
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Search for new phenomena in high-mass diphoton final states using 37 fb$^{-1}$ of proton--proton collisions collected at $\sqrt{s}=13$ TeV with the ATLAS detector
... of the selected data sample is studied using three methods detailed in .... The 2 × 2D sideband method and the matrix method are based on sidebands constructed by invert- ing photon ... See full document
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Search for high-mass resonances in dilepton final states in proton-proton collisions at $\sqrt{s}=$ 13 TeV
... extend the gauge group of the SM by additional U 0 ( 1 ) gauge ...groups. The U 0 ( 1 ) gauge groups, or a linear combination of them, can be broken near the TeV scale, giving rise to ... See full document
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Search for chargino-neutralino production using recursive jigsaw reconstruction in final states with two or three charged leptons in proton-proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
... V.S. Lang 44 , J.C. Lange 14 , R.J. Langenberg 35 , A.J. Lankford 168 , F. Lanni 29 , K. Lantzsch 24 , A. Lanza 68a , A. Lapertosa 53b,53a , S. Laplace 132 , J.F. Laporte 142 , T. Lari 66a , F. Lasagni Manghi ... See full document
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Search for displaced muonic lepton jets from light Higgs boson decay in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
... particles with large decay lengths and collimated final states represent, from an experimental point of view, a chal- lenge both for the trigger and for the reconstruction capabilities ... 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 $\sqrt{s}=13\text{ }\text{ }\mathrm{TeV}$
... (OSSF) lepton pair with mass below 12 GeV are vetoed to reduce back- ground from low-mass ...pair with mass below 81 GeV when the trilepton mass is within a Z boson mass window ( 91 ... See full document
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Search for Higgs boson pair production in the $bb\tau\tau$ final state in proton-proton collisions at $\sqrt{(}s)=8\text{ }\text{ }\mathrm{TeV}$
... h lepton starts with a PF jet as the initial ...by the reconstruction of the π 0 components in the jet which are then combined with the charged hadron ... See full document
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Search for the associated production of a Higgs boson with a single top quark in proton-proton collisions at $ \sqrt{s}=8 $ TeV
... presents the search for the production of a Higgs boson in association with a single top quark (tHq), using data collected in ... See full document
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Search for bottom squark pair production in proton–proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
... in the final state and applying further selection criteria similar to those of the corresponding signal ...events with good-quality electrons and muons the “signal lepton” ... See full document
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Search for supersymmetry in final states with missing transverse momentum and multiple $b$-jets in proton-proton collisions at $ \sqrt{s}=13 $ TeV with the ATLAS detector
... A.E. Barton 87 , P. Bartos 28a , A. Basalaev 134 , A. Bassalat 128 , R.L. Bates 55 , S.J. Batista 165 , J.R. Batley 31 , M. Battaglia 143 , M. Bauce 70a,70b , F. Bauer 142 , H.S. Bawa 150,m , J.B. Beacham 122 , M.D. ... See full document
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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
... 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 in section 8 ... See full document
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A search for $ t\overline{t} $ resonances using lepton-plus-jets events in proton-proton collisions at $ \sqrt{s}=8 $ TeV with the ATLAS detector
... M. Donadelli 24d , S. Donati 124a,124b , P. Dondero 121a,121b , J. Donini 34 , J. Dopke 131 , A. Doria 104a , M.T. Dova 71 , A.T. Doyle 53 , E. Drechsler 54 , M. Dris 10 , E. Dubreuil 34 , E. Duchovni 172 , G. ... See full document
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