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[PDF] Top 20 Search for electroweak production of charginos and neutralinos in multilepton final states in proton-proton collisions at $\sqrt{s}=$ 13 TeV

Has 10000 "Search for electroweak production of charginos and neutralinos in multilepton final states in proton-proton collisions at $\sqrt{s}=$ 13 TeV" found on our website. Below are the top 20 most common "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

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

... program and the European Research Council and Horizon 2020 Grant, contract ...Ministry of Education, Youth and Sports (MEYS) of the Czech Republic; the Council of Science ... See full document

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Search for electroweak production of charginos in final states with two τ leptons in pp collisions at $ \sqrt{s}=8 $ TeV

Search for electroweak production of charginos in final states with two τ leptons in pp collisions at $ \sqrt{s}=8 $ TeV

... a search for the electroweak production of supersymmet- ric particles in pp collisions in final states with two τ ...1 and 19.6 fb − 1 depending on ... See full document

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Search for natural and split supersymmetry in proton-proton collisions at $ \sqrt{s}=13 $ TeV in final states with jets and missing transverse momentum

Search for natural and split supersymmetry in proton-proton collisions at $ \sqrt{s}=13 $ TeV in final states with jets and missing transverse momentum

... reconstructs and identifies each individual particle with an optimized combination of information from the various elements of the CMS ...detector. In this process, the identification ... 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

... ance in inclusive Z boson production events ...) of the system of supersymmetric ...1.18 at p ISR T ≈ 125 GeV and ...applied in order not to alter the signal ... See full document

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Search for new physics in the monophoton final state in proton-proton collisions at $ \sqrt{s}=13 $ TeV

Search for new physics in the monophoton final state in proton-proton collisions at $ \sqrt{s}=13 $ TeV

... Proton-proton collisions producing large missing transverse momentum and a high transverse momentum photon have been investigated to search for new phenomena, using a data set cor- ... See full document

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Searches for third-generation squark production in fully hadronic final states in proton-proton collisions at $ \sqrt{s} = 8$ TeV

Searches for third-generation squark production in fully hadronic final states in proton-proton collisions at $ \sqrt{s} = 8$ TeV

... data and simulation samples as well as the control and search regions are all defined to be kinematically similar, so most of the uncertainties due to mismodelling of event kinemat- ics ... See full document

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Search for Z$\gamma$ resonances using leptonic and hadronic final states in proton-proton collisions at $\sqrt{s}=$ 13 TeV

Search for Z$\gamma$ resonances using leptonic and hadronic final states in proton-proton collisions at $\sqrt{s}=$ 13 TeV

... because of the large Lorentz boost of a Z boson produced in the decay of a heavy ...fraction of events corresponding to the merged topology, which has low background from SM sources, ... See full document

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Search for the direct production of charginos and neutralinos  in final states with tau leptons in $\sqrt{s} = $ 13 TeV $pp$ collisions with the ATLAS detector

Search for the direct production of charginos and neutralinos in final states with tau leptons in $\sqrt{s} = $ 13 TeV $pp$ collisions with the ATLAS detector

... 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, ... See full document

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Search for $\mathrm{t}\overline{\mathrm{t}}$H production in the all-jet final state in proton-proton collisions at $\sqrt{s}=$ 13 TeV

Search for $\mathrm{t}\overline{\mathrm{t}}$H production in the all-jet final state in proton-proton collisions at $\sqrt{s}=$ 13 TeV

... 124850 and 125105 (Hungary); the Council of Science and Industrial Research, India; the HOMING PLUS programme of the Foundation for Polish Science, cofinanced from European Union, Regional ... See full document

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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

... modeling of tt and W + jets production, the dominant background processes, two control regions that are enriched in events from these processes are defined by modifying the event selection ... 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 with systematic ... See full document

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Search for new physics with dijet angular distributions in proton-proton collisions at $ \sqrt{s}=13 $ TeV

Search for new physics with dijet angular distributions in proton-proton collisions at $ \sqrt{s}=13 $ TeV

... the electroweak scale, which can make black hole production possible at the LHC ...scale and decay into multijets through Hawking radiation [27], have previously been sought in multijet ... See full document

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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 decays, and ... 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

Search for bottom squark pair production in proton–proton collisions at $\sqrt{s}=13$  TeV with the ATLAS detector

... Uncertainties in the modelling of the top-quark pair and single-top-quark (Wt) backgrounds are sub- dominant in SRA and dominant in ...samples and those of ... 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

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

... occur in a variety of theoretical models that at- tempt to extend the standard model (SM) of particle ...superstring and left-right-symmetric models (LR), achieve unification of ... See full document

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Search for electroweak production of charginos and neutralinos using leptonic final states in $pp$ collisions at $\sqrt{s}=7$ TeV

Search for electroweak production of charginos and neutralinos using leptonic final states in $pp$ collisions at $\sqrt{s}=7$ TeV

... G. Cerminara, T. Christiansen, J.A. Coarasa Perez, D. D’Enterria, A. Dabrowski, A. De Roeck, S. Di Guida, M. Dobson, N. Dupont-Sagorin, A. Elliott-Peisert, B. Frisch, W. Funk, G. Georgiou, M. Giffels, D. Gigi, K. ... See full document

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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

... 124850 and 125105 (Hungary); the Coun- cil of Science and Industrial Research, India; the HOMING PLUS program of the Foundation for Polish Science, cofinanced from European Union, Regional ... See full document

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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} $

... S. Abdullin, M. Albrow, M. Alyari, 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, ... 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

... lifetime of order 10 − 27 ...tensor and does not distinguish between various par- ticle species, microscopic BHs decay democratically into all SM degrees of freedom, ...values of quantum ... See full document

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

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

... summarized in Table 1. The CRs are defined at both preselection and signal region selection ...CRs at the pre- selection level are defined with looser cuts in order to check the ... See full document

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