[PDF] Top 20 Search for new phenomena in a lepton plus high jet multiplicity final state with the ATLAS experiment using $ \sqrt{s}=13 $ TeV proton-proton collision data
Has 10000 "Search for new phenomena in a lepton plus high jet multiplicity final state with the ATLAS experiment using $ \sqrt{s}=13 $ TeV proton-proton collision data" found on our website. Below are the top 20 most common "Search for new phenomena in a lepton plus high jet multiplicity final state with the ATLAS experiment using $ \sqrt{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 $ \sqrt{s}=13 $ TeV proton-proton collision data
... 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, Chile; ... See full document
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Search for new phenomena in events with high jet multiplicity and low missing transverse momentum in proton–proton collisions at $\sqrt{s}=8$ TeV
... dedicated search is presented for new phenomena in inclusive 8- and 10-jet final states with low missing transverse momentum, with and without identification of jets ... See full document
11
Search for new phenomena in high-mass diphoton final states using 37 fb$^{-1}$ of proton--proton collisions collected at $\sqrt{s}=13$ TeV with the ATLAS detector
... The ATLAS detector [20,21] is a multi-purpose detector with a forward–backward symmetric cylindrical ...1 The systems most relevant for the presented searches are the inner ... See full document
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Search for new phenomena in photon+jet events collected in proton--proton collisions at sqrt(s) = 8 TeV with the ATLAS detector
... In the absence of any signal, three types of γ + jet signals are explored: a generic Gaussian-shaped sig- nal with an arbitrary production cross-section, result- ing from resonances ... See full document
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Search for new phenomena in monophoton final states in proton-proton collisions at $\sqrt s =$ 8 TeV
... colleagues in the CERN accelerator departments for the excellent perfor- mance of the LHC and thank the technical and administrative staffs at CERN and at other CMS institutes for their ... See full document
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Search for New Phenomena in Dijet Angular Distributions in Proton-Proton Collisions at $\sqrt{s} = 8$ TeV Measured with the ATLAS Detector
... Uncertainties in the SM and signal predictions include theoretical uncertainties and experimental uncertainties on the measured angular ...certainties in the SM and signal predictions ... 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 $\sqrt{s}$ = 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, Chile; ... See full document
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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 or 1/Λ 4 for ... See full document
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Search for new phenomena in final states with large jet multiplicities and missing transverse momentum with ATLAS using $\sqrt{s} =$ 13 TeV proton-proton collisions
... acknowledge the support of ANPCyT, Argentina; YerPhI, Ar- menia; ARC, Australia; BMWFW and FWF, Austria; ANAS, Azerbai- jan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, ... See full document
22
Search for new phenomena in final states with large jet multiplicities and missing transverse momentum at $\sqrt{s}$=8 TeV proton-proton collisions using the ATLAS experiment
... acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Aus- tralia; BMWF and FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, Chile; ... See full document
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Search for new phenomena with multiple charged leptons in proton–proton collisions at $\sqrt{s}= 13$ $\,\text {TeV}$
... a search for physics beyond the standard model in final states with at least three charged leptons, in any combination of electrons or ...muons. The data sample ... See full document
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Search for new high-mass phenomena in the dilepton final state using 36 fb$^{−1}$ of proton-proton collision data at $ \sqrt{s}=13 $ TeV with the ATLAS detector
... E.B. Diehl 92 , J. Dietrich 17 , S. Díez Cornell 45 , A. Dimitrievska 14 , J. Dingfelder 23 , P. Dita 28b , S. Dita 28b , F. Dittus 32 , F. Djama 88 , T. Djobava 54b , J.I. Djuvsland 60a , M.A.B. do Vale ... See full document
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Search for high-mass $\mathrm{ Z }\gamma$ resonances in proton-proton collisions at $\sqrt{s}=$ 8 and 13 TeV using jet substructure techniques
... a search for new spin-0 resonances decaying to a Z boson and a photon, where the Z boson decays hadronically, in the mass range from ...3.0 TeV, using 2012 and 2015 ... See full document
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Search for new physics in the monophoton final state in proton-proton collisions at $ \sqrt{s}=13 $ TeV
... a high transverse momentum photon have been investigated to search for new phenomena, using a data set cor- responding to ...√ s = 13 TeV at the CERN ... See full document
36
Search for black holes in high-multiplicity final states in proton-proton collisions at $ \sqrt{s}=$13 TeV
... A search for new physics in energetic, high-multiplicity final states has been performed using proton– proton collision data collected with ... See full document
29
Search for new phenomena with the $M_{\mathrm {T2}}$ variable in the all-hadronic final state produced in proton–proton collisions at $\sqrt{s} = 13$ $\,\text {TeV}$
... processed using the particle-flow (PF) algorithm [21], which is designed to recon- struct and identify all particles using the optimal combination of information from the elements of ... See full document
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Search for new phenomena with photon+jet events in proton-proton collisions at $ \sqrt{s}=13 $ TeV with the ATLAS detector
... cells 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 ...]. ... See full document
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Search for nonpointing photons in the diphoton and $E^{miss}_T$ final state in $\sqrt{s}$=7 TeV proton-proton collisions using the ATLAS detector
... on the capabilities of the ATLAS calorimeter system, which covers the pseudora- pidity range |η| < ...losses in material upstream of the EM ...calorimeters. The solid ... See full document
26
Search for $W' \to t\bar{b}$ in the lepton plus jets final state in proton-proton collisions at a centre-of-mass energy of $\sqrt{s}$ = 8 TeV with the ATLAS detector
... top-quark s-channel and Wt processes are simulated with the Powheg [31, 32] generator, which uses a NLO QCD matrix element with the CT10 PDFs ...[29]. The parton shower and ... See full document
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Search for $\mathrm{t}\overline{\mathrm{t}}$H production in the all-jet final state in proton-proton collisions at $\sqrt{s}=$ 13 TeV
... colleagues in the CERN accelerator departments for the excellent perfor- mance of the LHC and thank the technical and administrative staffs at CERN and at other CMS institutes for their ... See full document
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