[PDF] Top 20 Combination of searches for heavy resonances decaying into bosonic and leptonic final states using 36 fb$^{-1}$ of proton-proton collision data at $\sqrt{s} = 13$ TeV with the ATLAS detector
Has 10000 "Combination of searches for heavy resonances decaying into bosonic and leptonic final states using 36 fb$^{-1}$ of proton-proton collision data at $\sqrt{s} = 13$ TeV with the ATLAS detector" found on our website. Below are the top 20 most common "Combination of searches for heavy resonances decaying into bosonic and leptonic final states using 36 fb$^{-1}$ of proton-proton collision data at $\sqrt{s} = 13$ TeV with the ATLAS detector".
Combination of searches for heavy resonances decaying into bosonic and leptonic final states using 36 fb$^{-1}$ of proton-proton collision data at $\sqrt{s} = 13$ TeV with the ATLAS detector
... a combination of searches in the VV and VH (with H representing the SM Higgs boson) final states obtained with ...19.7 fb −1 at p ... See full document
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Search for heavy ZZ resonances in the $\ell ^+\ell ^-\ell ^+\ell ^-$ and $\ell ^+\ell ^-\nu \bar{\nu }$ final states using proton–proton collisions at $\sqrt{s}= 13$ $\text {TeV}$ with the ATLAS detector
... tracking detector (ID), covering the region |η| < 2.5, consists of a silicon pixel detector, a silicon microstrip detector and a transition-radiation ...tracker. The ... See full document
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Search for heavy resonances decaying into a $W$ or $Z$ boson and a Higgs boson in final states with leptons and $b$-jets in 36 fb$^{-1}$ of $\sqrt s = 13$ TeV $pp$ collisions with the ATLAS detector
... by the tt background. The contribution from diboson, SM Vh, tth, and ttV production is small in all three ...channels. The multijet background, due to semileptonic hadron decays or ... See full document
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Combination of searches for heavy resonances decaying to WW, WZ, ZZ, WH, and ZH boson pairs in proton–proton collisions at $\sqrt{s}=8$ and 13 TeV
... statistical combination are based on proton–proton (pp) collision data collected by the CMS ex- periment [29] at √ s = 8 and 13 TeV, ... See full document
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Search for resonant $WZ$ production in the fully leptonic final state in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector
... from the Tevatron [ 22 , 23 ] have put limits on the mass of a W boson of an extended gauge model [ 2 ] in the W Z channel between 180 GeV and 690 ...GeV. The present ... See full document
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Searches for supersymmetry with the ATLAS detector using final states with two leptons and missing transverse momentum in $\sqrt{s}=7$ TeV proton-proton collisions
... Results of three searches are presented for the production of supersymmetric particles decaying into final states with missing transverse momentum and ... See full document
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Search for supersymmetry in final states with two same-sign or three leptons and jets using 36 fb$^{-1}$ of $\sqrt{s}=13$ TeV $pp$ collision data with the ATLAS detector
... particles using signatures involving multiple energetic jets and either two isolated same-sign leptons (e or µ), or at least three isolated leptons, is ...presented. The analysis relies on ... See full document
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Search for squarks and gluinos in final states with jets and missing transverse momentum using 36 fb$^{-1}$ of $\sqrt{s}=13$ TeV pp collision data with the ATLAS detector
... , and (b),(d) a fixed m ˜χ 0 1 ¼ 60 GeV and varying values of m ˜g (or m ˜q ) and m ˜χ 1 are ...by using the signal region with the best expected ... See full document
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Search for low mass vector resonances decaying into quark-antiquark pairs in proton-proton collisions at $\sqrt{s} =$ 13 TeV
... vector resonances with masses below 450 GeV and a natural width small relative to the detector ’s mass reso- ...such states. We consider a Lorentz-boosted event topology ... See full document
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Combined measurements of Higgs boson production and decay using up to $80$ fb$^{-1}$ of proton-proton collision data at $\sqrt{s}=$ 13 TeV collected with the ATLAS experiment
... distinguish the t¯tH, VH, VBF, and ggF production modes and to enhance the purity of each kinematic selection, 11 mutually exclusive reconstructed event cat- egories based on the ... See full document
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Search for Z$\gamma$ resonances using leptonic and hadronic final states in proton-proton collisions at $\sqrt{s}=$ 13 TeV
... suite of programs as used for collision ...taken into account by su- perimposing minimum bias events on the hard scattering ...interaction. The simulated samples are reweighted to match ... See full document
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Search for high-mass resonances in dilepton final states in proton-proton collisions at $\sqrt{s}=$ 13 TeV
... high-mass resonances decaying into electron or muon pairs. The search uses proton-proton collision data at a centre-of-mass energy of 13 ... See full document
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Search for massive resonances decaying into pairs of boosted bosons in semi-leptonic final states at $\sqrt{s} =$ 8 TeV
... feature of the CMS detector is a ...solenoid with a 6 m internal diameter. Within the field volume are the silicon tracker, the crystal electromagnetic calorimeter (ECAL), ... See full document
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Search for diphoton events with large missing transverse momentum in fb$^{-1}$ of 7 TeV proton–proton collision data with the ATLAS detector
... V. Kukhtin 65 , Y. Kulchitsky 90 , S. Kuleshov 31b , C. Kummer 98 , M. Kuna 78 , N. Kundu 118 , J. Kunkle 120 , A. Kupco 125 , H. Kurashige 67 , M. Kurata 160 , Y.A. Kurochkin 90 , V. Kus 125 , M. Kuze 157 , J. ... See full document
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Search for narrow resonances in dilepton mass spectra in proton-proton collisions at $\sqrt{s}$ = 13 TeV and combination with 8 TeV data
... to the success of the CMS ...acknowledge the computing centers and personnel of the Worldwide LHC Computing Grid for delivering so effectively the computing ... See full document
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Search for pair-produced resonances each decaying into at least four quarks in proton-proton collisions at $\sqrt{s}=$ 13 TeV
... in the CERN accelerator departments for the excellent performance of the LHC and thank the technical and administrative staffs at CERN and at other ... See full document
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Search for new phenomena in dijet events using 37 fb$^{-1}$ of $pp$ collision data collected at $\sqrt{s}=$13 TeV with the ATLAS detector
... L. Iconomidou-Fayard 119 , Z. Idrissi 137e , P. Iengo 32 , O. Igonkina 109,x , T. Iizawa 174 , Y. Ikegami 69 , M. Ikeno 69 , Y. Ilchenko 11,y , D. Iliadis 156 , N. Ilic 145 , G. Introzzi 123a,123b , P. Ioannou 9,∗ , M. ... See full document
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Measurement of the Inelastic Proton-Proton Cross Section at $\sqrt{s} = 13$ TeV with the ATLAS Detector at the LHC
... D. Delgove 117 , F. Deliot 136 , C.M. Delitzsch 51 , A. Dell’Acqua 32 , L. Dell’Asta 24 , M. Dell’Orso 124a,124b , M. Della Pietra 104a,k , D. della Volpe 51 , M. Delmastro 5 , P.A. Delsart 57 , D.A. DeMarco 158 , ... See full document
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Search for narrow resonances decaying to dijets in proton-proton collisions at $\sqrt(s) =$ 13 TeV
... [42] with a uniform prior for a positive signal cross section; log-normal priors are used to model systematic uncer- tainties in the jet energy scale, jet energy resolution, and integrated ... 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
... 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, ... See full document
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