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[PDF] Top 20 Search for electroweak production of supersymmetric states in scenarios with compressed mass spectra at $\sqrt{s}=13$ TeV with the ATLAS detector

Has 10000 "Search for electroweak production of supersymmetric states in scenarios with compressed mass spectra at $\sqrt{s}=13$ TeV with the ATLAS detector" found on our website. Below are the top 20 most common "Search for electroweak production of supersymmetric states in scenarios with compressed mass spectra at $\sqrt{s}=13$ TeV with the ATLAS detector".

Search for electroweak production of supersymmetric states in scenarios with compressed mass spectra at $\sqrt{s}=13$ TeV with the ATLAS detector

Search for electroweak production of supersymmetric states in scenarios with compressed mass spectra at $\sqrt{s}=13$ TeV with the ATLAS detector

... Examples of kinematic distributions after the background-only fit showing the data as well as the expected background in control regions CR-tau (left) and CR-top ...(right). The ... See full document

53

Search for $WW/WZ$ resonance production in $\ell \nu qq$ final states in $pp$ collisions at $\sqrt{s} =$ 13 TeV with the ATLAS detector

Search for $WW/WZ$ resonance production in $\ell \nu qq$ final states in $pp$ collisions at $\sqrt{s} =$ 13 TeV with the ATLAS detector

... events with a W boson produced in association with jets ...sources of SM background include the production of top quarks, multijets, dibo- sons and Z ...bosons with ... See full document

44

Search for a supersymmetric partner to the top quark in final states with jets and missing transverse momentum at $\sqrt{s}=7$ TeV with the ATLAS detector

Search for a supersymmetric partner to the top quark in final states with jets and missing transverse momentum at $\sqrt{s}=7$ TeV with the ATLAS detector

... presence of high-p T top quarks that decay through t → bW → bjj in the ˜t 1 t ˜ ⋆ 1 final state is exploited to further reduce SM backgrounds by only considering events with reconstructed ... See full document

20

Search for pair production of heavy vector-like quarks decaying into hadronic final states in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector

Search for pair production of heavy vector-like quarks decaying into hadronic final states in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector

... MES of Russia and NRC KI, Russian Federation; JINR; MESTD, Serbia; MSSR, Slovakia; ARRS and MIZ Š, Slovenia; DST/NRF, South Africa; MINECO, Spain; SRC and Wallenberg Foundation, Sweden; SERI, SNSF and Cantons ... See full document

36

Search for neutral Higgs bosons of the minimal supersymmetric standard model in pp collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector

Search for neutral Higgs bosons of the minimal supersymmetric standard model in pp collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector

... between the two searches are that they are optimized for different production mechanisms and Higgs boson mass ...Additionally, the three Higgs bosons of the MSSM, which can have ... See full document

55

Search for the dimuon decay of the Higgs boson in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector

Search for the dimuon decay of the Higgs boson in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector

... using the anti-k t algorithm [42] with a radius parameter of R ¼ ...and the jet p T must be larger than 25 (30) GeV for jηj < ...using the track and vertex informa- tion inside a jet ... See full document

20

Search for new phenomena in different-flavour high-mass dilepton final states in pp collisions at $\sqrt{s}=13$  Tev with the ATLAS detector

Search for new phenomena in different-flavour high-mass dilepton final states in pp collisions at $\sqrt{s}=13$  Tev with the ATLAS detector

... from the energy in clusters of cells in the electromagnetic calorimeter associated with a track in the ID [ 58 ...decays. The LH discriminant utilises ... See full document

41

Measurement of the $ZZ$ Production Cross Section in $pp$ Collisions at $\sqrt{s}$ = 13 TeV with the ATLAS Detector

Measurement of the $ZZ$ Production Cross Section in $pp$ Collisions at $\sqrt{s}$ = 13 TeV with the ATLAS Detector

... Studying the production of pairs of Z bosons in proton- proton (pp) interactions at the Large Hadron Collider (LHC) tests the electroweak sector of ... See full document

19

Search for new phenomena in dijet mass and angular distributions from $pp$ collisions at $\sqrt{s}=$ 13 TeV with the ATLAS detector

Search for new phenomena in dijet mass and angular distributions from $pp$ collisions at $\sqrt{s}=$ 13 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, ... See full document

38

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

... 8.186 with the A14 tune for the PS modelling, hadronisation, and underlying ...event. The ME calcula- tion is performed at tree level and includes the emission of up to ... 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 ...between the three channels considered: e µ, eτ, ...as the vertex whose constituent tracks have the highest sum of p 2 T , and ... See full document

49

Search for new phenomena with photon+jet events in proton-proton collisions at $ \sqrt{s}=13 $ TeV with the ATLAS detector

Search for new phenomena with photon+jet events in proton-proton collisions at $ \sqrt{s}=13 $ TeV with the ATLAS detector

... Final states consisting of a photon and a jet (γ+jet) with large invariant mass could be produced in proton– proton (pp) collisions at the Large Hadron Collider (LHC) ... See full document

38

Search for pair production of higgsinos in final states with at least three $b$-tagged jets in $\sqrt{s} = 13$ TeV $pp$ collisions using the ATLAS detector

Search for pair production of higgsinos in final states with at least three $b$-tagged jets in $\sqrt{s} = 13$ TeV $pp$ collisions using 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, ... See full document

49

Search for squarks and gluinos in final states with jets and missing transverse momentum at $\sqrt{s} =$ 13 TeV with the ATLAS detector

Search for squarks and gluinos in final states with jets and missing transverse momentum at $\sqrt{s} =$ 13 TeV with the ATLAS detector

... modelling of background processes are evaluated by comparing samples produced with different MC ...generators. The W/Z+jets events generated with Sherpa are com- pared to events generated ... See full document

45

Search for low-mass dijet resonances using trigger-level jets with the ATLAS detector in $pp$ collisions at $\sqrt{s}=13$ TeV

Search for low-mass dijet resonances using trigger-level jets with the ATLAS detector in $pp$ collisions at $\sqrt{s}=13$ TeV

... resonances with sub-TeV masses using the ATLAS detector at the Large Hadron Collider can be statistically limited by the bandwidth available to inclusive single-jet ... See full document

20

Search for High-Mass Resonances Decaying to $\tau\nu$ in pp Collisions at $\sqrt{s}$=13  TeV with the ATLAS Detector

Search for High-Mass Resonances Decaying to $\tau\nu$ in pp Collisions at $\sqrt{s}$=13  TeV with the ATLAS Detector

... associated with reconstructed electrons, muons, and jets are found to have a very small ...impact. The uncertainty in the combined 2015 þ 2016 integrated luminosity is ...used in Ref. ... See full document

20

Search for diboson resonances with boson-tagged jets in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

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

23

Search for long-lived particles in final states with displaced dimuon vertices in $pp$ collisions at $\sqrt{s}=$ 13 TeV with the ATLAS detector

Search for long-lived particles in final states with displaced dimuon vertices in $pp$ collisions at $\sqrt{s}=$ 13 TeV with the ATLAS detector

... Distributions of m µµ and signed r vtx for opposite-charge and same-charge (SS) dimuon vertices satisfying the preselection criteria are shown in Figure 2 ...are the expected contributions ... See full document

48

Search for direct top squark pair production in final states with two leptons in $\sqrt{s} = 13$ TeV $pp$ collisions with the ATLAS detector

Search for direct top squark pair production in final states with two leptons in $\sqrt{s} = 13$ TeV $pp$ collisions with the ATLAS detector

... aid in the estimation of the background from SM processes and to model the SUSY ...signal. The event generator, parton shower and hadronisation generator, cross-section ... See full document

64

Search for strong production of supersymmetric particles in final states with missing transverse momentum and at least three $b$-jets at $\sqrt{s}$= 8 TeV proton-proton collisions with the ATLAS detector

Search for strong production of supersymmetric particles in final states with missing transverse momentum and at least three $b$-jets at $\sqrt{s}$= 8 TeV proton-proton collisions with the ATLAS detector

... dominant detector-related systematic uncertainties on the amount of irreducible back- ground are due to the jet energy scale (JES) and resolution (JER) uncertainties; they range respectively ... See full document

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