[PDF] Top 20 Search for low-scale gravity signatures in multi-jet final states with the ATLAS detector at $ \sqrt{s}=8 $ TeV
Has 10000 "Search for low-scale gravity signatures in multi-jet final states with the ATLAS detector at $ \sqrt{s}=8 $ TeV" found on our website. Below are the top 20 most common "Search for low-scale gravity signatures in multi-jet final states with the ATLAS detector at $ \sqrt{s}=8 $ TeV".
Search for low-scale gravity signatures in multi-jet final states with the ATLAS detector at $ \sqrt{s}=8 $ TeV
... M. Iodice 134a , K. Iordanidou 35 , V. Ippolito 57 , A. Irles Quiles 167 , C. Isaksson 166 , M. Ishino 68 , M. Ishitsuka 157 , R. Ishmukhametov 111 , C. Issever 120 , S. Istin 19a , J.M. Iturbe Ponce 84 , R. Iuppa ... See full document
45
Search for direct top squark pair production in final states with two tau leptons in pp collisions at $\sqrt{s}=8$ TeV with the ATLAS detector
... describing the shower shape in the calorimeters and information from the tracking system are used to separate the collimated τ had decay products from the generally broader jets ... See full document
48
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 through ... 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
... A.A. O’Rourke 44 , V. O’Shea 55 , F.G. Oakham 31,d , H. Oberlack 102 , T. Obermann 23 , J. Ocariz 82 , A. Ochi 69 , I. Ochoa 37 , J.P. Ochoa-Ricoux 34a , S. Oda 72 , S. Odaka 68 , H. Ogren 63 , A. Oh 86 , ... See full document
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Search for supersymmetry at $\sqrt{s}$=8 TeV in final states with jets and two same-sign leptons or three leptons with the ATLAS detector
... background in the SR3b region is expected to be completely dominated by events with at least one light or charm jet mis-tagged as a b-jet, ...of the background estimate ... See full document
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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
Search for new phenomena with photon+jet events in proton-proton collisions at $ \sqrt{s}=13 $ TeV with the ATLAS detector
... using the anti-k t algorithm with radius parameter R = ...problems in the detector, or identified as arising from non-collision backgrounds, are discarded [ 45 ...]. Jet ... See full document
38
Search for Quantum Black Hole Production in High-Invariant-Mass Lepton$+$Jet Final States Using $pp$ Collisions at $\sqrt{s} =$ 8 TeV and the ATLAS Detector
... a search for quantum black-hole production using ...collected with the ATLAS detector in pp collisions at the LHC at √ s = 8 ...TeV. ... See full document
20
Search for R-parity-violating supersymmetric particles in multi-jet final states produced in $p$-$p$ collisions at $\sqrt{s} =13$ TeV using the ATLAS detector at the LHC
... M. Schioppa 40b , 40a , K.E. Schleicher 50 , S. Schlenker 35 , K.R. Schmidt-Sommerfeld 113 , K. Schmieden 35 , C. Schmitt 97 , S. Schmitt 44 , S. Schmitz 97 , U. Schnoor 50 , L. Schoeffel 142 , A. ... See full document
23
Search for direct pair production of the top squark in all-hadronic final states in proton-proton collisions at $\sqrt{s}=8$ TeV with the ATLAS detector
... J. Janssen 21 , M. Janus 171 , G. Jarlskog 80 , N. Javadov 64,b , T. Jav ˚urek 48 , L. Jeanty 15 , J. Jejelava 51a,o , G.-Y. Jeng 151 , D. Jennens 87 , P. Jenni 48,p , J. Jentzsch 43 , C. Jeske 171 , S. J´ez´equel ... See full document
57
Search for electroweak production of supersymmetric particles in final states with two or three leptons at $\sqrt{s}=13\,$TeV with the ATLAS detector
... R.E. Ticse Torres 99 , V.O. Tikhomirov 108,ap , Yu.A. Tikhonov 120b,120a , S. Timoshenko 110 , P. Tipton 181 , S. Tisserant 99 , K. Todome 163 , S. Todorova-Nova 5 , S. Todt 46 , J. Tojo 85 , ... 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
... L.K. Gladilin 101 , C. Glasman 85 , J. Glatzer 13 , P.C.F. Glaysher 45 , A. Glazov 45 , M. Goblirsch-Kolb 25 , J. Godlewski 42 , S. Goldfarb 91 , T. Golling 52 , D. Golubkov 132 , A. Gomes 128a,128b,128d , R. ... See full document
44
Search for $s$-channel single top-quark production in proton–proton collisions at $\sqrt s=8$ TeV with the ATLAS detector
... on the reconstruction and energy cal- ibration of jets, electrons and muons are propagated in the anal- ysis through variations in the modelling of the detector ...For ... See full document
19
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
... channels. The colour labelled “Others” includes contributions from Z, di-boson and multi-jet production ...processes. The hatched band shows the systematic uncertainty, which includes ... See full document
29
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in $pp$ collisions at $\sqrt{s}=13$ TeV using the ATLAS detector
... cover the pseudorapidity range |η| < 3.2. The hadronic calorimetry in the range |η| < ...of the central barrel. In the endcaps (|η| > ...match the outer ... See full document
46
Search for heavy long-lived multi-charged particles in pp collisions at $\sqrt{s}=\;8$ TeV using the ATLAS detector
... The ATLAS detector [ 10 ] covers nearly the entire solid angle around the collision ...tracking detector (ID) comprising a silicon pixel detector (pixel), a silicon ... See full document
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Further search for supersymmetry at $\sqrt{s}=7$ TeV in final states with jets, missing transverse momentum and isolated leptons with the ATLAS detector
... E.A. Ouellette 169 , F. Ould-Saada 117 , A. Ouraou 136 , Q. Ouyang 33a , A. Ovcharova 15 , M. Owen 82 , S. Owen 139 , V.E. Ozcan 19a , N. Ozturk 8 , A. Pacheco Pages 12 , C. Padilla Aranda 12 , S. ... See full document
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Search for Monotop Signatures in Proton-Proton Collisions at $\sqrt s =$ 8 TeV
... beyond the standard model (BSM), such as those with universal extra dimensions [1] or supersymmetry [2, 3], predict the existence of neutral massive particles that are “invisible”, that is, they ... See full document
29
Search for doubly charged Higgs boson production in multi-lepton final states with the ATLAS detector using proton–proton collisions at $\sqrt{s}=13\,\text {TeV}$
... A. Sapronov 68 , J.G. Saraiva 128a,128d , B. Sarrazin 23 , O. Sasaki 69 , K. Sato 164 , E. Sauvan 5 , G. Savage 80 , P. Savard 161,d , N. Savic 103 , C. Sawyer 133 , L. Sawyer 82,u , J. Saxon 33 , C. Sbarra 22a , A. ... See full document
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Search for Scalar Charm Quark Pair Production in $pp$ Collisions at $\sqrt{s}=$ 8 TeV with the ATLAS Detector
... negligible. The estimation of the main background processes is carried out by defining a set of three data control regions (CR) that do not overlap with each other or with the sig- nal ... See full document
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