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[PDF] Top 20 Search for TeV-scale gravity signatures in high-mass final states with leptons and jets with the ATLAS detector at $\sqrt{s}=13$ TeV

Has 10000 "Search for TeV-scale gravity signatures in high-mass final states with leptons and jets with the ATLAS detector at $\sqrt{s}=13$ TeV" found on our website. Below are the top 20 most common "Search for TeV-scale gravity signatures in high-mass final states with leptons and jets with the ATLAS detector at $\sqrt{s}=13$ TeV".

Search for TeV-scale gravity signatures in high-mass final states with leptons and jets with the ATLAS detector at $\sqrt{s}=13$ TeV

Search for TeV-scale gravity signatures in high-mass final states with leptons and jets with the ATLAS detector at $\sqrt{s}=13$ TeV

... of the distribution of the scalar sum of the transverse momenta of leptons and jets is sens- itive to the production of high-mass ...holes with two to ... See full document

30

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 heavy Majorana or Dirac neutrinos and right-handed $W$ gauge bosons in final states with two charged leptons and two jets at $\sqrt{s}$ = 13 TeV with the ATLAS detector

Search for heavy Majorana or Dirac neutrinos and right-handed $W$ gauge bosons in final states with two charged leptons and two jets 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; ... See full document

51

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

... Other detector-related systematic uncertainties, such as those in lepton reconstruction efficiency, energy scale, energy resolution and in the modelling of the trigger e ... See full document

64

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

... For the irreducible backgrounds, the uncertainties include those from the background model and from the simulation of the response of the ...detector. The ... See full document

57

Search for new particles decaying to $Z Z$ using final states with leptons and jets with the ATLAS detector in $\sqrt{s}=7$ TeV proton-proton collisions

Search for new particles decaying to $Z Z$ using final states with leptons and jets with the ATLAS detector in $\sqrt{s}=7$ TeV proton-proton collisions

... production in the SM (W W, W Z, ZZ) are modeled using herwig and scaled to the next-to-leading order (NLO) pro- duction cross sections as computed by mcfm ...6.0 with MRST2007 LO* [24]. ... See full document

42

Search for resonances in diphoton events at $\sqrt{s}$=13 TeV with the ATLAS detector

Search for resonances in diphoton events at $\sqrt{s}$=13 TeV with the ATLAS detector

... using the Diphox NLO computation, where the photon four-vectors are smeared with the detector resolution, and also with Sherpa generated samples which are then passed ... See full document

49

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

... yields and exclusion fit results with the signal strength parameter set to zero for the exclusive electroweakino and slepton signal ...prompt leptons are categorized as ... See full document

53

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 is ...presented. ... See full document

41

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

... 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 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

... The ATLAS and CMS experiments at the Large Hadron Collider (LHC) were conceived to address a variety of questions not fully explained within the Standard Model (SM) of particle ... See full document

48

A search for pair-produced resonances in four-jet final states at $\sqrt{s} =$ 13 TeV with the ATLAS detector

A search for pair-produced resonances in four-jet final states at $\sqrt{s} =$ 13 TeV with the ATLAS detector

... small, and negligible with respect to the detector ...interpret the analysis for the case where both top squarks decay into light quarks, since the analysis is not ... See full document

41

Search for high-mass new phenomena in the dilepton final state using proton-proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

Search for high-mass new phenomena in the dilepton final state using proton-proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

... GeV with bin widths varying from 100 to 1500 GeV. The prior probability is chosen to be uniform and positive in the cross-section for the Z ′ limit calculation and 1/Λ 2 ... See full document

35

Search for strong gravity in multijet final states produced in pp collisions at $\sqrt{s} =$ 13 TeV using the ATLAS detector at the LHC

Search for strong gravity in multijet final states produced in pp collisions at $\sqrt{s} =$ 13 TeV using the ATLAS detector at the LHC

... importance. The inner detector, immersed in a magnetic field provided by a solenoidal magnet, has full coverage in φ and covers the pseudorapidity 1 range |η| < ...pixel ... See full document

40

Search for excited leptons in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

Search for excited leptons in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

... + jets background is generated with Alpgen 2.13 [19], while the t¯ t background is produced with MC@NLO ...[20]. In both cases, Jimmy ...interactions and Herwig 6.510 [22] is ... See full document

22

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

... to the data and simulation of the signal models at a series of discrete masses to set 95% credibility-level upper limits on the cross section times acceptance [30] for the ... See full document

20

Search for light top squark pair production in final states with leptons and $b^-$ jets with the ATLAS detector in $\sqrt{s}=7$ TeV proton-proton collisions

Search for light top squark pair production in final states with leptons and $b^-$ jets with the ATLAS detector in $\sqrt{s}=7$ TeV proton-proton collisions

... Conceptually, the variable is constructed by dividing an event’s topology into a subsystem comprising both the visible and invisible particles originating from the hard-scattering process of ... See full document

21

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

... MNiSW and NCN, Poland; FCT, Portugal; MNE/IFA, Romania; MES of Russia and NRC KI, Russian Federation; JINR; MESTD, Serbia; MSSR, Slovakia; ARRS and MIZ Š, Slovenia; DST/NRF, South Africa; MINECO, ... See full document

20

Search for supersymmetry in $pp$ collisions at $\sqrt{s}=7$ TeV in final states with missing transverse momentum and $b^-$ jets with the ATLAS detector

Search for supersymmetry in $pp$ collisions at $\sqrt{s}=7$ TeV in final states with missing transverse momentum and $b^-$ jets with the ATLAS detector

... termination in the SR0 and SR1, respectively, are com- puted using MC ...on the signal region ...(JES and JER, b-tagging efficiency and fake rate, lep- ton identification ... See full document

29

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 ... See full document

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