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[PDF] Top 20 Search for heavy long-lived charged R-hadrons with the ATLAS detector in 3.2 fb(-1) of proton-proton collision data at root s=13 TeV

Has 10000 "Search for heavy long-lived charged R-hadrons with the ATLAS detector in 3.2 fb(-1) of proton-proton collision data at root s=13 TeV" found on our website. Below are the top 20 most common "Search for heavy long-lived charged R-hadrons with the ATLAS detector in 3.2 fb(-1) of proton-proton collision data at root s=13 TeV".

Search for heavy long-lived charged R-hadrons with the ATLAS detector in 3.2 fb(-1) of proton-proton collision data at root s=13 TeV

Search for heavy long-lived charged R-hadrons with the ATLAS detector in 3.2 fb(-1) of proton-proton collision data at root s=13 TeV

... R -hadron signal events are generated with gluino (bottom- squark and top-squark) masses from 600 GeV to 2000 GeV (600 GeV to 1400 GeV). Pair production of gluinos and squarks is simulated in Pythia 6.427 [27] ... See full document

19

Search for new phenomena in high-mass diphoton final states using 37 fb¯¹ of proton–proton collisions collected at √s=13 TeV with the ATLAS detector

Search for new phenomena in high-mass diphoton final states using 37 fb¯¹ of proton–proton collisions collected at √s=13 TeV with the ATLAS detector

... selected data sample is studied using three methods detailed in ...The 2 × 2D sideband method and the matrix method are based on sidebands constructed by invert- ing photon identification and isolation ... See full document

21

Search for long lived, heavy particles in final states with a muon and multi track displaced vertex in proton proton collisions at √s=7 TeV with the ATLAS detector

Search for long lived, heavy particles in final states with a muon and multi track displaced vertex in proton proton collisions at √s=7 TeV with the ATLAS detector

... of heavy particles with long ...a search for events containing one or more such particles, which decay at a significant distance from their production point, using a final state containing ... See full document

20

Search for heavy particles decaying into top-quark pairs using lepton-plus-jets events in proton-proton collisions at root s=13 TeV with the ATLAS detector

Search for heavy particles decaying into top-quark pairs using lepton-plus-jets events in proton-proton collisions at root s=13 TeV with the ATLAS detector

... R. Nisius 113 , I. Nitsche 47 , T. Nitta 177 , T. Nobe 160 , Y. Noguchi 83 , M. Nomachi 129 , I. Nomidis 33 , M. A. Nomura 29 , T. Nooney 90 , M. Nordberg 35 , N. Norjoharuddeen 131 , T. Novak 89 , O. Novgorodova ... See full document

39

Measurement of charged particle distributions sensitive to the underlying event in s=13 TeV proton proton collisions with the ATLAS detector at the LHC

Measurement of charged-particle distributions sensitive to the underlying event in √s=13 TeV proton-proton collisions with the ATLAS detector at the LHC

... and heavy-ion physics, using hydrodynamic flow modelling in high-density regions and a string-based hadronisation model ...ATLAS’s 13 TeV minimum-bias data, including the tails of distribu- ... See full document

42

Measurement of the Inelastic Proton-Proton Cross Section at root s=13 TeV with the ATLAS Detector at the LHC

Measurement of the Inelastic Proton-Proton Cross Section at root s=13 TeV with the ATLAS Detector at the LHC

... the detector, which can send charged particles through the detector parallel to the beam; collision-induced radiation; and activation ...× 2, accounting for the 37 colliding pairs of ... See full document

30

Search for high-mass new phenomena in the dilepton final state using proton-proton collisions at root s=13 TeV with the ATLAS detector

Search for high-mass new phenomena in the dilepton final state using proton-proton collisions at root s=13 TeV with the ATLAS detector

... the ATLAS detector covered by the tracking detectors ( | η | < ...semileptonic heavy-flavour hadron ...the search, and the Very Loose and Loose working points are used in the ... See full document

35

Search for chargino-neutralino production using recursive jigsaw reconstruction in final states with two or three charged leptons in proton-proton collisions at root s=13 TeV with the ATLAS detector

Search for chargino-neutralino production using recursive jigsaw reconstruction in final states with two or three charged leptons in proton-proton collisions at root s=13 TeV with the ATLAS detector

... A search for electroweak production of supersymmetric particles is performed in two-lepton and three-lepton final states using recursive jigsaw ...The search uses data col- lected in 2015 and 2016 by ... See full document

59

Search for new phenomena in dijet events using 37 fb-1 of pp collision data collected at s =13 TeV with the ATLAS detector

Search for new phenomena in dijet events using 37 fb-1 of pp collision data collected at s =13 TeV with the ATLAS detector

... the proton-proton collision data set recorded at p ffiffiffi s ¼ 13 TeV with the ATLAS detector at the Large Hadron Collider in 2015 and 2016, corresponding to ... See full document

26

Search  for  resonant  WZ production  in  the  fully  leptonic  final  state  in proton–proton  collisions  at √s =13 TeV with  the  ATLAS  detector

Search for resonant WZ production in the fully leptonic final state in proton–proton collisions at √s =13 TeV with the ATLAS detector

... the search for resonant W Z production beyond that in Run 1 pp collision data at √ s = 8 TeV performed by the ATLAS [24] and CMS [25] ...for heavy V V and V H ... See full document

22

Search for narrow resonances in dilepton mass spectra in proton-proton collisions at root s=13 TeV and combination with 8 TeV data

Search for narrow resonances in dilepton mass spectra in proton-proton collisions at root s=13 TeV and combination with 8 TeV data

... A search for narrow resonances in dielectron and dimuon invariant mass spectra has been performed using data obtained from protonproton collisions at √ s = 13 TeV ... See full document

24

Search for new high mass phenomena in the dilepton final state using 36 fb−1 of proton proton collision data at s=13 TeV with the ATLAS detector

Search for new high mass phenomena in the dilepton final state using 36 fb−1 of proton proton collision data at s=13 TeV with the ATLAS detector

... V.V. Kostyukhin 23 , A. Kotwal 48 , A. Koulouris 10 , A. Kourkoumeli-Charalampidi 123a,123b , C. Kourkoumelis 9 , E. Kourlitis 141 , V. Kouskoura 27 , A.B. Kowalewska 42 , R. Kowalewski 172 , T.Z. Kowalski 41a , ... See full document

61

Search for long-lived neutral particles decaying into lepton-jets in 20.3 fb−1 proton-proton collisions at √s = 8 TeV with the ATLAS detector

Search for long-lived neutral particles decaying into lepton-jets in 20.3 fb−1 proton-proton collisions at √s = 8 TeV with the ATLAS detector

... optimize search criteria and to produce detection efficiency ...the detector to lepton-jets and guide their characterization and the identification of the variables useful for the selection of ... See full document

6

Performance of missing transverse momentum reconstruction with the ATLAS detector using proton proton collisions at root s=13 TeV

Performance of missing transverse momentum reconstruction with the ATLAS detector using proton proton collisions at root s=13 TeV

... the ATLAS detector is evaluated using data collected in protonproton collisions at the LHC at a centre- of-mass energy of 13 TeV in ...and charged-particle tracks ... See full document

65

Searches for heavy long lived sleptons and R hadrons with the ATLAS detector in pp collisions at √s=7 TeV

Searches for heavy long lived sleptons and R hadrons with the ATLAS detector in pp collisions at √s=7 TeV

... V. Kukhtin 64 , Y. Kulchitsky 90 , S. Kuleshov 32b , C. Kummer 98 , M. Kuna 78 , J. Kunkle 120 , A. Kupco 125 , H. Kurashige 66 , M. Kurata 160 , Y.A. Kurochkin 90 , V. Kus 125 , E.S. Kuwertz 147 , M. Kuze 157 , ... See full document

33

Search for diphoton events with large missing transverse momentum in 7 TeV proton–proton collision data with the ATLAS detector

Search for diphoton events with large missing transverse momentum in 7 TeV proton–proton collision data with the ATLAS detector

... D.P.C. Sankey 129 , A. Sansoni 47 , C. Santamarina Rios 85 , C. Santoni 34 , R. Santonico 133a , 133b , H. Santos 124a , J.G. Saraiva 124a , T. Sarangi 173 , E. Sarkisyan-Grinbaum 8 , F. Sarri 122a , 122b , G. ... See full document

21

Search for excited electrons singly produced in proton-proton collisions at root s=13 TeV with the ATLAS experiment at the LHC

Search for excited electrons singly produced in proton-proton collisions at root s=13 TeV with the ATLAS experiment at the LHC

... D. Pohl 24 , I. Pokharel 52 , G. Polesello 69a , A. Poley 18 , A. Policicchio 71a,71b , R. Polifka 36 , A. Polini 23b , C. S. Pollard 45 , V. Polychronakos 29 , D. Ponomarenko 111 , L. Pontecorvo 36 , G. A. ... See full document

30

Muon reconstruction performance of the ATLAS detector in proton–proton collision data at √s=13 TeV

Muon reconstruction performance of the ATLAS detector in proton–proton collision data at √s=13 TeV

... N. Semprini-Cesari 22a,22b , C. Serfon 120 , L. Serin 118 , L. Serkin 164a,164b , M. Sessa 135a,135b , R. Seuster 169 , H. Severini 114 , T. Sfiligoj 77 , F. Sforza 32 , A. Sfyrla 51 , E. Shabalina 56 , N. W. ... See full document

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A search for tt¯ resonances with the ATLAS detector in 2 05 fb( 1) of proton proton collisions at √s=7 TeV

A search for tt¯ resonances with the ATLAS detector in 2 05 fb( 1) of proton proton collisions at √s=7 TeV

... cho Toro 33 , P. Camarri 133a,133b , D. Cameron 117 , L.M. Caminada 14 , S. Campana 29 , M. Campanelli 77 , V. Canale 102a,102b , F. Canelli 30,g , A. Canepa 159a , J. Cantero 80 , R. Cantrill 76 , L. ... See full document

24

Search for new phenomena in a lepton plus high jet multiplicity final state with the ATLAS experiment using √s=13 TeV proton-proton collision data

Search for new phenomena in a lepton plus high jet multiplicity final state with the ATLAS experiment using √s=13 TeV proton-proton collision data

... (≥ 3), the MC simulation strongly underestimates the background contributions compared to the data-driven background ...the data with no signal component included in the fit ... See full document

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