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[PDF] Top 20 Search for new phenomena in final states with two opposite-charge, same-flavor leptons, jets, and missing transverse momentum in pp collisions at $ \sqrt{s}=13 $ TeV

Has 10000 "Search for new phenomena in final states with two opposite-charge, same-flavor leptons, jets, and missing transverse momentum in pp collisions at $ \sqrt{s}=13 $ TeV" found on our website. Below are the top 20 most common "Search for new phenomena in final states with two opposite-charge, same-flavor leptons, jets, and missing transverse momentum in pp collisions at $ \sqrt{s}=13 $ TeV".

Search for new phenomena in final states with two opposite-charge, same-flavor leptons, jets, and missing transverse momentum in pp collisions at $ \sqrt{s}=13 $ TeV

Search for new phenomena in final states with two opposite-charge, same-flavor leptons, jets, and missing transverse momentum in pp collisions at $ \sqrt{s}=13 $ TeV

... uncertainties and some SM background components as described ...(NLO) and next-to-NLO cross sections [ 42 – 47 ] are used to normalize the simulated background samples, while NLO plus next-to-leading- ... See full document

55

Search for new physics in final states with two opposite-sign, same-flavor leptons, jets, and missing transverse momentum in pp collisions at sqrt(s) = 13 TeV

Search for new physics in final states with two opposite-sign, same-flavor leptons, jets, and missing transverse momentum in pp collisions at sqrt(s) = 13 TeV

... This search targets different modes of neutralino decays into final states with two opposite- sign, same-flavor leptons, jets, and E T miss ... See full document

36

Search for direct third-generation squark pair production in final states with missing transverse momentum and two $b$-jets in $\sqrt{s} =$ 8 TeV $pp$ collisions with the ATLAS detector

Search for direct third-generation squark pair production in final states with missing transverse momentum and two $b$-jets in $\sqrt{s} =$ 8 TeV $pp$ collisions with the ATLAS detector

... processes in the signal regions are the production of W or Z bosons in association with heavy-flavour jets (referred to as W +hf and Z+hf) and the production of ...Events ... See full document

51

Search for new phenomena in final states with an energetic jet and large missing transverse momentum in $pp$ collisions at $\sqrt{s}=13$  TeV using the ATLAS detector

Search for new phenomena in final states with an energetic jet and large missing transverse momentum in $pp$ collisions at $\sqrt{s}=13$  TeV using the ATLAS detector

... monojet-like final states and a dedicated strategy with a suppression power of approximately 10 3 is needed in order to reduce these backgrounds to a sub-percent ...described in ... See full document

46

A search for new phenomena in pp collisions at $\sqrt{s} = 13\,\text {TeV} $ in final states with missing transverse momentum and at least one jet using the $\alpha _{\mathrm {T}}$ variable

A search for new phenomena in pp collisions at $\sqrt{s} = 13\,\text {TeV} $ in final states with missing transverse momentum and at least one jet using the $\alpha _{\mathrm {T}}$ variable

... 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

56

Search for new phenomena in events containing a same-flavour opposite-sign dilepton pair, jets, and large missing transverse momentum in $\sqrt{s}=$ 13 $pp$ collisions with the ATLAS detector

Search for new phenomena in events containing a same-flavour opposite-sign dilepton pair, jets, and large missing transverse momentum in $\sqrt{s}=$ 13 $pp$ collisions with the ATLAS detector

... BMWFW and FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, Chile; CAS, MOST and NSFC, China; COLCIENCIAS, Colombia; MSMT CR, ... See full document

63

Search for direct production of charginos, neutralinos and sleptons in final states with two leptons and missing transverse momentum in $pp$ collisions at $\sqrt{s} =$ 8 TeV with the ATLAS detector

Search for direct production of charginos, neutralinos and sleptons in final states with two leptons and missing transverse momentum in $pp$ collisions at $\sqrt{s} =$ 8 TeV with the ATLAS detector

... prompt and non-prompt efficiencies are evaluated as functions of the p T of the lepton candidate in simulated events using MC truth ...data and MC are corrected for with normalization factors ... See full document

55

Search for new phenomena in final states with large jet multiplicities and missing transverse momentum with ATLAS using $\sqrt{s} =$ 13 TeV proton-proton collisions

Search for new phenomena in final states with large jet multiplicities and missing transverse momentum with ATLAS using $\sqrt{s} =$ 13 TeV proton-proton collisions

... A search is presented for new phenomena with large jet mul- tiplicities (from ≥ 7 to ≥ 10) and missing transverse ...The search used 3.2 fb − 1 of √ s = ... See full document

22

Search for Physics Beyond the Standard Model in Events with Two Leptons, Jets, and Missing Transverse Momentum in pp Collisions at sqrt(s) = 8 TeV

Search for Physics Beyond the Standard Model in Events with Two Leptons, Jets, and Missing Transverse Momentum in pp Collisions at sqrt(s) = 8 TeV

... presented two searches for BSM physics based on events with an opposite-sign SF lepton pair: a search for an edge in the dilepton mass spectrum out- side the Z boson mass region [4], ... See full document

39

Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at $\sqrt{s}=$8 TeV with the ATLAS detector

Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at $\sqrt{s}=$8 TeV with the ATLAS detector

... C. Maidantchik 24a , A.A. Maier 101 , A. Maio 126a,126b,126d , S. Majewski 116 , Y. Makida 66 , N. Makovec 117 , B. Malaescu 80 , Pa. Malecki 39 , V.P. Maleev 123 , F. Malek 55 , U. Mallik 63 , D. Malon 6 , C. ... See full document

47

Search for direct slepton and gaugino production in final states with two leptons and missing transverse momentum with the ATLAS detector in $pp$ collisions at $\sqrt{s}=7$ TeV

Search for direct slepton and gaugino production in final states with two leptons and missing transverse momentum with the ATLAS detector in $pp$ collisions at $\sqrt{s}=7$ TeV

... “fake leptons” refers to both misidentified jets and real leptons that arise from decays or ...fake leptons are identified as those satisfying a loose set of identifica- tion ... See full document

28

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

... 13 TeV by the CMS Collaboration [24–29]. The data set analysed in this analysis is a factor of 16 larger than that presented in ...The search strategy aims to provide sensitivity to a ... See full document

49

Search for new phenomena in final states with large jet multiplicities and missing transverse momentum at $\sqrt{s}$=8 TeV proton-proton collisions using the ATLAS experiment

Search for new phenomena in final states with large jet multiplicities and missing transverse momentum at $\sqrt{s}$=8 TeV proton-proton collisions using the ATLAS experiment

... + jets and Z + jets events are generated with up to five additional partons in the matrix element, except for processes involving b-quarks for which up to four additional partons are ... See full document

60

Search for gluinos in events with two same-sign leptons, jets and missing transverse momentum with the ATLAS detector in $pp$ collisions at $\sqrt{s}=7$ TeV

Search for gluinos in events with two same-sign leptons, jets and missing transverse momentum with the ATLAS detector in $pp$ collisions at $\sqrt{s}=7$ TeV

... data with a method similar to that described in ...identification and isolation ...[26], and for both electrons and muons the isolation criterion is ...tight-loose and ... See full document

19

Search for physics beyond the standard model in events with two leptons of same sign, missing transverse momentum, and jets in proton–proton collisions at $\sqrt{s} = 13\,\text {TeV} $

Search for physics beyond the standard model in events with two leptons of same sign, missing transverse momentum, and jets in proton–proton collisions at $\sqrt{s} = 13\,\text {TeV} $

... colleagues in the CERN accelerator departments for the excellent perfor- mance of the LHC and thank the technical and administrative staffs at CERN and at other CMS institutes ... See full document

42

Search for new phenomena in events with same-charge leptons and $b$-jets in $pp$ collisions at $\sqrt{s}= 13$ TeV with the ATLAS detector

Search for new phenomena in events with same-charge leptons and $b$-jets in $pp$ collisions at $\sqrt{s}= 13$ TeV with the ATLAS detector

... model and from the simulation of the response of the ...process and of the acceptance of the signal regions for that ...¯tW and t ¯tZ production, these uncertainties are estimated by varying the ... See full document

57

Search for new physics in events with opposite-sign leptons, jets, and missing transverse energy in $pp$ collisions at $\sqrt{s}=7$ TeV

Search for new physics in events with opposite-sign leptons, jets, and missing transverse energy in $pp$ collisions at $\sqrt{s}=7$ TeV

... a search for physics beyond the standard model in the opposite-sign dilep- ton final state using a data sample of proton-proton collisions at a center-of-mass energy of 7 ..., ... See full document

39

Search for supersymmetry in events with $b$-tagged jets and missing transverse momentum in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

Search for supersymmetry in events with $b$-tagged jets and missing transverse momentum in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

... where two decay modes for the bottom (top) squark are allowed and direct decays to the LSP, ˜b 1 → b ˜ χ 0 1 (˜t 1 → t ˜ χ 0 1 ) compete with decays via an intermediate chargino ( ˜ χ ± 1 ) state, ˜b ... See full document

50

Search for high-mass resonances in final states with a lepton and missing transverse momentum at $ \sqrt{s}=13 $ TeV

Search for high-mass resonances in final states with a lepton and missing transverse momentum at $ \sqrt{s}=13 $ TeV

... A search for new high-mass resonances in proton-proton collisions having final states with an electron or muon and missing transverse momentum ... See full document

41

Search for top squarks in final states with one isolated lepton, jets, and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector

Search for top squarks in final states with one isolated lepton, jets, and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector

... ] in the calorimeters using the anti-k t algorithm with a jet radius parameter R = ...]. Jets are corrected for contamination from pileup using the jet area method [ 97 – 99 ] and then ... See full document

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