[PDF] Top 20 Search for high-mass new phenomena in the dilepton final state using proton-proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
Has 10000 "Search for high-mass new phenomena in the dilepton final state using proton-proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector" found on our website. Below are the top 20 most common "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
... 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
35
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
... A search is presented for new phenomena with large jet mul- tiplicities (from ≥ 7 to ≥ 10) and missing transverse ...momentum. The search used 3.2 fb − 1 of √ s = ... See full document
22
Search for new phenomena with the $M_{\mathrm {T2}}$ variable in the all-hadronic final state produced in proton–proton collisions at $\sqrt{s} = 13$ $\,\text {TeV}$
... S. Abdullin, M. Albrow, G. Apollinari, A. Apresyan, A. Apyan, S. Banerjee, L.A.T. Bauerdick, A. Beretvas, J. Berryhill, P.C. Bhat, G. Bolla, K. Burkett, J.N. Butler, A. Canepa, G.B. Cerati, H.W.K. Cheung, ... See full document
46
Performance of missing transverse momentum reconstruction with the ATLAS detector using proton-proton collisions at $\sqrt{s}$ = 13 TeV
... for the transverse momentum carried by undetected particles produced in proton–proton (pp) collisions measured with the ATLAS detector [ 1 ] at ... See full document
66
Search for new physics in same-sign dilepton events in proton–proton collisions at $\sqrt{s} = 13\,\text {TeV} $
... energy in the electromagnetic calorimeter with tracks in the silicon tracker ...[27]. The identification is performed using a Boosted Decision Tree multivariate ... See full document
40
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
... The ATLAS detector [24] covers nearly the entire solid angle around the collision point, and consists of an in- ner tracking detector surrounded by a solenoid, EM and ... See full document
26
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
... deposits in the EM calorimeter as described in ...whether the EM cluster is associated with a conversion track candidate reconstructed in the ...matched, the ... See full document
38
Search for contact interactions and large extra dimensions in the dilepton channel using proton-proton collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector
... of the ATLAS detector using G EANT 4 [ 23 – 25 ]. The DY back- ground is generated with P OWHEG [ 26 ] for the next-to- leading-order (NLO) matrix elements using ... See full document
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Search for high-mass dilepton resonances in pp collisions at $\sqrt{s}=8$ TeV with the ATLAS detector
... only the central values for ABM11 fall outside of the MSTW2008NNLO PDF’s uncertainty ...of the latter uncertainty and the ABM11 cen- tral value is formed with respect to the ... See full document
31
Search for new phenomena in monophoton final states in proton-proton collisions at $\sqrt s =$ 8 TeV
... Within the superconducting solenoid volume are a silicon pixel and strip tracker, a lead tungstate crystal electromagnetic calorimeter (ECAL), and a brass and scintillator hadron calorimeter (HCAL), each composed ... See full document
33
Search for new phenomena with multiple charged leptons in proton–proton collisions at $\sqrt{s}= 13$ $\,\text {TeV}$
... a search for new physics in final states with three or more leptons, elec- trons or muons, produced at the CERN LHC, in proton-proton (pp) ... See full document
42
Search for doubly charged Higgs boson production in multi-lepton final states with the ATLAS detector using proton–proton collisions at $\sqrt{s}=13\,\text {TeV}$
... J. Montejo Berlingen 32 , F. Monticelli 74 , S. Monzani 94a,94b , R.W. Moore 3 , N. Morange 119 , D. Moreno 21 , M. Moreno Llácer 32 , P. Morettini 53a , S. Morgenstern 32 , D. Mori 144 , T. Mori 157 , M. ... See full document
52
Search for pair production of Higgs bosons in the $b\bar{b}b\bar{b}$ final state using proton--proton 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
43
Search for heavy charged long-lived particles in proton-proton collisions at $\sqrt{s} = 13$ TeV using an ionisation measurement with the \mbox{ATLAS} detector
... large mass, LLPs are expected to be slow ( β γ ≤ 0 . 9 1 in a large fraction of cases) and therefore, if charged, to have a specific ionisation larger than any SM particle of unit charge at ... See full document
21
Search for new physics with dijet angular distributions in proton-proton collisions at $ \sqrt{s}=13 $ TeV
... models with large ED, the fundamental Planck scale can be comparable to the electroweak scale, which can make black hole production possible at the LHC ...than the Planck scale ... See full document
34
Search for pair production of Higgs bosons in the $b\bar{b}b\bar{b}$ final state using proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector
... S.K. Radhakrishnan 155 , P. Rados 105 , F. Ragusa 71a,71b , G. Rahal 53 , J.A. Raine 101 , S. Rajagopalan 27b , T. Rashid 131 , S. Raspopov 6 , M.G. Ratti 71a,71b , D.M. Rauch 48 , F. Rauscher 115 , ... See full document
50
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
... J. Price 73 , L.E. Price 6 , D. Prieur 124 , M. Primavera 72a , M. Proissl 46 , K. Prokofiev 109 , F. Prokoshin 32b , E. Protopapadaki 137 , S. Protopopescu 25 , J. Proudfoot 6 , X. Prudent 44 , M. Przybycien 38a ... See full document
60
Search for New Phenomena in $t\bar{t}$ Events With Large Missing Transverse Momentum in Proton-Proton Collisions at $\sqrt{s}=7$ TeV with the ATLAS Detector
... of high transverse momentum, four or more jets and large missing transverse ...this final state may arise from a number of Standard Model ...extensions. The results are interpreted in ... See full document
18
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 the CMS ... See full document
29
Search for narrow resonances in dilepton mass spectra in proton-proton collisions at $\sqrt{s}$ = 13 TeV and combination with 8 TeV data
... uncertainty in this analysis is in the parame- ter R ...for the dielectron barrel–barrel chan- nel, 10% for the dielectron barrel–endcap channel, and + − 1 5 % for the dimuon ... See full document
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