[PDF] Top 20 Search for high-mass Zγ resonances in e+e−γ and μ+μ−γ final states in proton-proton collisions at s√=8 and 13 TeV
Has 10000 "Search for high-mass Zγ resonances in e+e−γ and μ+μ−γ final states in proton-proton collisions at s√=8 and 13 TeV" found on our website. Below are the top 20 most common "Search for high-mass Zγ resonances in e+e−γ and μ+μ−γ final states in proton-proton collisions at s√=8 and 13 TeV".
Search for high-mass Zγ resonances in e+e−γ and μ+μ−γ final states in proton-proton collisions at s√=8 and 13 TeV
... CERN, European Organization for Nuclear Research, Geneva, Switzerland D. Abbaneo, E. Auffray, G. Auzinger, M. Bachtis, P. Baillon, A.H. Ball, D. Barney, P. Bloch, A. Bocci, A. Bonato, C. Botta, T. Camporesi, R. ... See full document
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Search for heavy ZZ resonances in the ℓ+ℓ−ℓ+ℓ− and ℓ+ℓ−νν¯ final states using proton–proton collisions at s√=13 TeV with the ATLAS detector
... A. S. Chisholm 32 , A. Chitan 28b , Y. H. Chiu 172 , M. V. Chizhov 68 , K. Choi 64 , A. R. Chomont 37 , S. Chouridou 156 , Y. S. Chow 62a , V. Christodoulou 81 , M. C. Chu 62a , J. Chudoba 129 , A. ... See full document
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Search for heavy ZZ resonances in the l(+) l(-) l(+) l(-) and l(+) l(-) nu(nu)over-bar final states using proton-proton collisions at root s=13 TeV with the ATLAS detector
... K. Kasahara 164 , L. Kashif 176 , R. D. Kass 113 , A. Kastanas 149 , Y. Kataoka 157 , C. Kato 157 , A. Katre 52 , J. Katzy 45 , K. Kawade 70 , K. Kawagoe 73 , T. Kawamoto 157 , G. Kawamura 57 , E. F. Kay 77 , V. ... See full document
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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
... resonance search and also in the non-resonant signal search, both of which target KK graviton signals at the TeV scale, the small number of data events at high m γ γ values does ... See full document
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Search for high-mass new phenomena in the dilepton final state using proton-proton collisions at root s=13 TeV with the ATLAS detector
... We 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; CAS, ... 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 √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 ...The search used 3.2 fb − 1 of √ s = 13 TeV pp collision data col- ... 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 √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 ...The search used 3.2 fb − 1 of √ s = 13 TeV pp collision data col- ... See full document
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Search for high mass resonances decaying to dilepton final states in pp collisions at s√=7 TeV with the ATLAS detector
... In the dimuon channel, the combined uncertainty on the trigger and reconstruction efficiency for muon pairs is estimated to be 6% at 2 TeV. This uncertainty is dominated by a conservative estimate of the impact ... See full document
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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
... inclusive search for supersymmetry with the CMS detector is reported, based on data from pp collisions collected at √ s = 8 TeV, corresponding to an integrated luminosity of 18 ...final ... 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 g √s = 13 TeV source proton–proton collisions
... A search is presented for new phenomena with large jet mul- tiplicities (from ≥ 7 to ≥ 10) and missing transverse ...The search used 3.2 fb − 1 of √ s = 13 TeV pp collision data col- ... See full document
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Search for new phenomena with photon+jet events in proton proton collisions at √s=13 TeV with the ATLAS detector
... A search is performed for the production of high-mass resonances decaying into a photon and a jet in ...of proton-proton collisions at a centre-of-mass energy of √ ... See full document
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Search for high-mass dilepton resonances in pp collisions at s√=8 TeV with the ATLAS detector
... a mass scale just above the (higher-dimensional) Planck scale, which in turn limits the number of particles in the final state ...two-particle final states, it is interesting to look at the ... See full document
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Search for high-mass diphoton resonances in proton-proton collisions at 13 TeV and combination with 8 TeV search
... m γ γ intervals in the search ...the mass spectrum predicted by the simulation and are fit with the chosen background ...m γ γ , which is tuned in such a manner that the absolute ... See full document
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Search for narrow resonances in dilepton mass spectra in proton-proton collisions at root s=13 TeV and combination with 8 TeV data
... the 8 TeV data in ...dilepton mass point, the amplitude of the background shape func- tion is constrained using data within a mass window ± 6 times the mass resolution about the ... See full document
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Searches for the Zγ decay mode of the Higgs boson and for new high mass resonances in pp collisions at s=13 TeV with the ATLAS detector
... The background mainly originates from non-resonant production of a Z boson and a prompt photon (Z+γ), with a smaller contribution from production of Z bosons in associa- tion with jets (Z +jets), with one jet ... See full document
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Search for high mass dilepton resonances in pp collisions at root s = 8 TeV with the ATLAS detector
... a mass scale just above the (higher-dimensional) Planck scale, which in turn limits the number of particles in the final state ...two-particle final states, it is interesting to look at the ... 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
... . Viel 168 , M. Villa 19a,19b , M. Villaplana Perez 167 , E. Vilucchi 47 , M.G. Vincter 28 , E. Vinek 29 , V.B. Vinogradov 64 , M. Virchaux 136,* , J. Virzi 14 , O. Vitells 172 , M. Viti 41 , I. Vi- varelli ... See full document
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Neural Networks Search for Charged Higgs Boson in Two Doublet Higgs Model at the Hadrons Colliders
... invariant mass of electron-muon pair is required to exceed 15 GeV and the electron and the muon are required to have opposite electric ...The search for the fully leptonic final state H H + − → τ ν τ ... See full document
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Search for heavy neutrinos or third-generation leptoquarks in final states with two hadronically decaying τ leptons and two jets in proton-proton collisions at √s=13 TeV
... A similar dilepton plus dijet final state can be realized in other extensions of the SM that predict scalar or vector LQs. The motivation for postulating such particles is to achieve a unified description of ... See full document
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Search for resonant W Z production in the fully leptonic final state in proton-proton collisions at root s=13 TeV with the ATLAS detector
... W.K. Balunas 132 , E. Banas 42 , A. Bandyopadhyay 24 , Sw. Banerjee 179,i , A.A.E. Bannoura 180 , L. Barak 158 , W.M. Barbe 37 , E.L. Barberio 102 , D. Barberis 56b,56a , M. Barbero 99 , T. Barillari 113 , ... See full document
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