[PDF] Top 20 ATLAS search for new phenomena in dijet mass and angular distributions using pp collisions at √s=7 TeV
Has 10000 "ATLAS search for new phenomena in dijet mass and angular distributions using pp collisions at √s=7 TeV" found on our website. Below are the top 20 most common "ATLAS search for new phenomena in dijet mass and angular distributions using pp collisions at √s=7 TeV".
ATLAS search for new phenomena in dijet mass and angular distributions using pp collisions at √s=7 TeV
... achieved using a procedure that diagonalises the total covariance matrix found from in situ techniques, selects the largest eigenvalues as ef- fective nuisance parameters, and groups the remaining parameters into ... See full document
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Search for new phenomena in dijet mass and angular distributions from pp collisions at root s=13 TeV with the ATLAS detector
... H. Lacker 16 , D. Lacour 82 , V.R. Lacuesta 166 , E. Ladygin 67 , R. Lafaye 5 , B. Laforge 82 , T. Lagouri 175 , S. Lai 55 , S. Lammers 62 , C.L. Lampen 7 , W. Lampl 7 , E. Lançon 137 , U. ... See full document
21
Search for new phenomena in dijet mass and angular distributions from pp collisions at √s=13 TeV with the ATLAS detector
... Fig. 1. The reconstructed dijet mass distribution (filled points) for events with | y ∗ | < 0 . 6 and p T > 440 ( 50 ) GeV for the leading (subleading) jets. The solid line depicts the fit to Eq. (1), ... See full document
21
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 ATLAS experiment [27,28] at the LHC is a multipurpose particle detector with a forward-backward symmetric cylindrical geometry with layers of tracking, calorimeter, and muon detectors over nearly the entire ... See full document
26
Search for new phenomena in different-flavour high-mass dilepton final states in pp collisions at √s=13 Tev with the ATLAS detector
... whom ATLAS could not be operated ...the ATLAS Tier-1 facili- ties at TRIUMF (Canada), NDGF (Denmark, Norway, Sweden), CC- IN2P3 (France), KIT/GridKA (Germany), INFN-CNAF (Italy), NL- T1 (Netherlands), PIC ... See full document
28
Search for anomalous electroweak production of WW/WZ in association with a high-mass dijet system in pp collisions at √s=8 TeV with the ATLAS detector
... The ATLAS detector [22] has a cylindrical geometry, 2 and consists of several layers of subdetectors around the interaction .... 7 and LAr calorimeters in the forward region provide additional EM and ... See full document
25
Search for new phenomena in events with at least three photons collected in pp collisions at √s = 8 TeV with the ATLAS detector
... I. Ibragimov 141 , L. Iconomidou-Fayard 117 , E. Ideal 176 , Z. Idrissi 135e , P. Iengo 30 , O. Igonkina 107 , T. Iizawa 171 , Y. Ikegami 66 , K. Ikematsu 141 , M. Ikeno 66 , Y. Ilchenko 31,r , D. Iliadis 154 , N. Ilic ... See full document
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Search for new phenomena in high-mass final states with a photon and a jet from pp collisions at root s=13 TeV with the ATLAS detector
... J. A. García Pascual 35a , M. Garcia-Sciveres 16 , R. W. Gardner 33 , N. Garelli 145 , V. Garonne 121 , A. Gascon Bravo 45 , K. Gasnikova 45 , C. Gatti 50 , A. Gaudiello 53a,53b , G. Gaudio 123a , I. L. Gavrilenko 98 , ... See full document
25
Search for new phenomena in events with a photon and missing transverse momentum in pp collisions at √s=13 TeV with the ATLAS detector
... the asymptotic approximation [68]. The likelihood fit includes both the SR and the CRs. Limits on the fiducial cross section of a potential signal beyond the SM, defined as the product of the cross section times the ... See full document
41
Search for magnetic monopoles in √s=7 TeV pp collisions with the ATLAS detector
... kinematic distributions from Drell-Yan monopole pair production is also ...the mass and energy regime of this study, the rays have kinetic ener- gies ranging from 1 MeV to a maximum of 100 MeV ...the ... See full document
19
Search for new phenomena in the WW → lνl'ν' final state in pp collisions at √s=7 TeV with the ATLAS detector
... ( pp → G ∗ ) × B R ( G ∗ → W W → ν ν ) ( , = e , μ or τ ) decreases from 108 pb to ...LO using calchep [35] v3.2 using the CTEQ6L1 PDF set [36], interfaced to pythia for parton showering and ...GeV ... See full document
20
Search for dark matter produced in association with a Higgs boson decaying to two bottom quarks in pp collisions at root s=8 TeV with the ATLAS detector
... ’ s position or energy reconstruction, the following sequential overlap removal procedures are implemented separately for the resolved and the boosted ...have angular separation in the range of 0 ... See full document
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Measurement of the W-boson mass in pp collisions at root s=7 TeV with the ATLAS detector
... V. Garonne 121 , A. Gascon Bravo 45 , K. Gasnikova 45 , C. Gatti 50 , A. Gaudiello 53a,53b , G. Gaudio 123a , I. L. Gavrilenko 98 , C. Gay 171 , G. Gaycken 23 , E. N. Gazis 10 , C. N. P. Gee 133 , M. Geisen 86 , M. P. ... See full document
14
Measurement of spin correlation between top and antitop quarks produced in pp¯ collisions at √s = 1 96 TeV
... element M is averaged over the colors and spins of the initial partons, and summed over the final colors and spins. For the hy- pothesis H = null, we set the spin correlation part to zero [11,12]. In the calculation, we ... See full document
8
Measurement of the W-boson mass in pp collisions at root s=7 TeV with the ATLAS detector
... M. Strauss 115 , P. Strizenec 146b , R. Ströhmer 177 , D. M. Strom 118 , R. Stroynowski 43 , A. Strubig 108 , S. A. Stucci 27 , B. Stugu 15 , N. A. Styles 45 , D. Su 145 , J. Su 127 , S. Suchek 60a , Y. ... See full document
61
Measurement of the W-boson mass in pp collisions at root s=7 TeV with the ATLAS detector
... M.P. Giordani 167a,167c , F.M. Giorgi 22a , P.F. Giraud 138 , P. Giromini 59 , D. Giugni 94a , F. Giuli 122 , C. Giuliani 103 , M. Giulini 60b , B.K. Gjelsten 121 , S. Gkaitatzis 156 , I. Gkialas 9 , E.L. ... See full document
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A Search for B-L R-Parity-Violating Scalar Top Decays in √s = 8 Tev Pp Collisions With the Atlas Experiment
... Before discussing the details of event generation, it is useful to first introduce the concept of an “event.” At the LHC, beams of protons are accelerated in opposite directions, and allowed to cross at specific ... See full document
187
Search for top squark pair production in compressed-mass-spectrum scenarios in proton-proton collisions at root s=8 TeV using the alpha(T) variable
... activity using a parked data set collected with a dedicated trig- ger stream [61], where “parked” means that, due to limitations in the available processing capability, the data were recorded with- out being ... See full document
28
Search for high mass resonances decaying to dilepton final states in pp collisions at s√=7 TeV with the ATLAS detector
... the mass window, and therefore, two more systematic uncertainties which are found to be negligible in the non-interfering channels have to be taken into account ...2–3 TeV mass range, relative to the ... See full document
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Search for third generation scalar leptoquarks in pp collisions at √s=7 TeV with the ATLAS detector
... MIZˇ S, Slovenia; DST/NRF, South Africa; MICINN, Spain; SRC and Wallenberg Foundation, Sweden; SER, SNSF and Cantons of Bern and Geneva, Switzerland; NSC, Taiwan; TAEK, Turkey; STFC, the Royal Society and ... See full document
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