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[PDF] Top 20 Search for high-mass resonances in final states with a lepton and missing transverse momentum at root s=13 TeV

Has 10000 "Search for high-mass resonances in final states with a lepton and missing transverse momentum at root s=13 TeV" found on our website. Below are the top 20 most common "Search for high-mass resonances in final states with a lepton and missing transverse momentum at root s=13 TeV".

Search for high-mass resonances in final states with a lepton and missing transverse momentum at root s=13 TeV

Search for high-mass resonances in final states with a lepton and missing transverse momentum at root s=13 TeV

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

44

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

... 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

41

Search for long-lived particles using nonprompt jets and missing transverse momentum with proton-proton collisions at root s=13 TeV

Search for long-lived particles using nonprompt jets and missing transverse momentum with proton-proton collisions at root s=13 TeV

... shown in Fig. 1 (lower figure). Such an event would escape reconstruction in a tracker-based search because of the dif- ficulty in reconstructing tracks that originate from decay points ... See full document

26

Search for dark matter at $\sqrt{s}=13$ TeV in final states containing an energetic photon and large missing transverse momentum with the ATLAS detector

Search for dark matter at $\sqrt{s}=13$ TeV in final states containing an energetic photon and large missing transverse momentum with the ATLAS detector

... A.A.E. Bannoura 178 , L. Barak 32 , E.L. Barberio 91 , D. Barberis 53a,53b , M. Barbero 88 , T. Barillari 103 , M-S Barisits 32 , T. Barklow 145 , N. Barlow 30 , S.L. Barnes 36c , B.M. Barnett 133 , R.M. Barnett ... See full document

45

Search for supersymmetry in $pp$ collisions at $\sqrt{s}=7$ TeV in events with a single lepton, jets, and missing transverse momentum

Search for supersymmetry in $pp$ collisions at $\sqrt{s}=7$ TeV in events with a single lepton, jets, and missing transverse momentum

... nomena in heavy-ion ...solenoid, 13 m in length and 6 m in ...pipe) high-precision silicon pixel and silicon strip detectors for charged particle tracking; a ... See full document

59

Search for squarks and gluinos in events with an isolated lepton, jets, and missing transverse momentum at $\sqrt{s}=13$ TeV with the ATLAS detector

Search for squarks and gluinos in events with an isolated lepton, jets, and missing transverse momentum at $\sqrt{s}=13$ TeV with the ATLAS detector

... have high purity in the background process of interest, a sufficiently large number of events to obtain small statistical uncertainties in the background prediction, and a small contamination ... See full document

57

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

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

... 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

55

Search For High-mass Z Gamma Resonances In E(+)e(-)gamma And Mu(+)mu(-)gamma Final States In Proton-proton Collisions At Root S=8 And 13 Tev

Search For High-mass Z Gamma Resonances In E(+)e(-)gamma And Mu(+)mu(-)gamma Final States In Proton-proton Collisions At Root S=8 And 13 Tev

... together with the definition of the coordinate system used and the relevant kinematic variables, can be found elsewhere [ 14 ...solenoid, 13 m in length and 6 m in di- ameter, ... See full document

34

Search for supersymmetry in events with a tau lepton pair and missing transverse momentum in proton-proton collisions at root s=13TeV

Search for supersymmetry in events with a tau lepton pair and missing transverse momentum in proton-proton collisions at root s=13TeV

... each final state requires the presence of exactly two reconstructed leptons with opposite charges, corresponding to the eµ, eτ h , µτ h , or τ h τ h final ...various lepton selection ... See full document

65

Search for heavy gauge W' boson in events with an energetic lepton and large missing transverse momentum at $ \sqrt{s} = $ 13 TeV

Search for heavy gauge W' boson in events with an energetic lepton and large missing transverse momentum at $ \sqrt{s} = $ 13 TeV

... combined with the present analysis using the prescription from ...1 and Run ...data ats = 8 and 13 TeV are presented in ...(upper) and the muon (lower) ... See full document

24

Search for physics beyond the standard model in final states with a lepton and missing transverse energy in proton-proton collisions at root s = 8 TeV

Search for physics beyond the standard model in final states with a lepton and missing transverse energy in proton-proton collisions at root s = 8 TeV

... S. Luyckx, 4 S. Ochesanu, 4 B. Roland, 4 R. Rougny, 4 M. Van De Klundert, 4 H. Van Haevermaet, 4 P. Van Mechelen, 4 N. Van Remortel, 4 A. Van Spilbeeck, 4 F. Blekman, 5 S. Blyweert, 5 J. D ’Hondt, 5 ... See full document

38

Search For Dark Matter And Unparticles In Events With A Z Boson And Missing Transverse Momentum In Proton-proton Collisions At Root S=13 Tev

Search For Dark Matter And Unparticles In Events With A Z Boson And Missing Transverse Momentum In Proton-proton Collisions At Root S=13 Tev

... variations in the signal acceptance, and the ranges quoted cover both signals of DM and unparticles with different DM masses or scaling ...strength with each parameter separately varied ... See full document

46

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

... A search is presented for physics beyond the standard model in final states with two opposite-sign, same-flavor leptons, jets, and missing transverse ...sions ... See full document

36

Search for Z gamma resonances using leptonic and hadronic final states in proton-proton collisions at root s=13 TeV

Search for Z gamma resonances using leptonic and hadronic final states in proton-proton collisions at root s=13 TeV

... acceptance and efficiency is similar to the narrow-resonance case up to 2 ...TeV. At large resonance masses (>2 TeV), however, the effect of rapidly falling PDFs introduces a lower tail ... See full document

44

Search for supersymmetry in events with at least three electrons or muons, jets, and missing transverse momentum in proton-proton collisions at root s=13 TeV

Search for supersymmetry in events with at least three electrons or muons, jets, and missing transverse momentum in proton-proton collisions at root s=13 TeV

... For signal efficiency calculations additional uncertainties in the description of the initial-state radiation (ISR) are taken into account. The modeling of ISR by the ver- sion of the MadGraph5 amc@nlo generator ... See full document

47

Search for lepton-flavor violation in different-flavor, high-mass final states in $pp$ collisions at $\sqrt s=13 $ TeV with the ATLAS detector

Search for lepton-flavor violation in different-flavor, high-mass final states in $pp$ collisions at $\sqrt s=13 $ TeV with the ATLAS detector

... events with exactly two different-flavour leptons are ..., and exactly two reconstructed different-flavor lepton candidates meeting the above-mentioned ...Events with an additional electron, ... See full document

49

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

... simulated in this analysis and to evaluate the uncertainty on this background several samples are ...produced with the factorisation and renormalisation scales varied coherently, along ... See full document

22

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

... MSES and CSF (Croatia); RPF (Cyprus); SENESCYT (Ecuador); MoER, ERC IUT, and ERDF (Estonia); Academy of Finland, MEC, and HIP (Finland); CEA and CNRS/IN2P3 (France); BMBF, DFG, and HGF ... See full document

55

Search for low-mass quark-antiquark resonances produced in association with a photon at root s=13 TeV

Search for low-mass quark-antiquark resonances produced in association with a photon at root s=13 TeV

... energy and beam intensity have increased, there has been a loss of sensitivity to lower mass resonances, which stems from the increasing cross section of background multijet events, tighter online ... See full document

18

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

... t¯t and Wt because the mass of the Wb system not from the resonant top quark is typically higher than for an on-shell top quark in the phase space selected by this ...Wt and reduce the W+jets ... See full document

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