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[PDF] Top 20 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

Has 10000 "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" found on our website. Below are the top 20 most common "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".

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

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

54

A search for $t\bar{t}$ resonances with the ATLAS detector in 2.05 fb$^{-1}$ of proton-proton collisions at $\sqrt{s}=7$ TeV

A search for $t\bar{t}$ resonances with the ATLAS detector in 2.05 fb$^{-1}$ of proton-proton collisions at $\sqrt{s}=7$ TeV

... Model of particle physics (SM) is believed to be an effective theory valid up to energies in the TeV ...to the breaking of the electroweak symmetry, final states ... See full document

25

Search for New Physics in the Dijet Mass Distribution using 1 fb$^{-1}$ of $pp$ Collision Data at $\sqrt{s}=$7 TeV collected by the ATLAS Detector

Search for New Physics in the Dijet Mass Distribution using 1 fb$^{-1}$ of $pp$ Collision Data at $\sqrt{s}=$7 TeV collected by the ATLAS Detector

... taken in 2011. The observed distribution, which ex- tends up to masses of ≈ 4 TeV, is in good agreement with a smooth function representing the SM ...for the ... See full document

20

Search for bottom squark pair production in proton–proton collisions at $\sqrt{s}=13$  TeV with the ATLAS detector

Search for bottom squark pair production in proton–proton collisions at $\sqrt{s}=13$  TeV with the ATLAS detector

... The data used in this analysis were collected by the ATLAS detector in pp collisions at the LHC with a centre-of-mass energy of ... See full document

37

Search for New Phenomena in Dijet Angular Distributions in Proton-Proton Collisions at $\sqrt{s} = 8$ TeV Measured with the ATLAS Detector

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

17

Search for squarks and gluinos with the ATLAS detector in final states with jets and missing transverse momentum using 4.7 fb$^{-1}$ of $\sqrt{s}=7$ TeV proton-proton collision data

Search for squarks and gluinos with the ATLAS detector in final states with jets and missing transverse momentum using 4.7 fb$^{-1}$ of $\sqrt{s}=7$ TeV proton-proton collision data

... produced in pairs {˜ g˜ g, ˜ q ˜ q, ˜ q˜ g}) and can generate the final state of interest through their direct ( ˜ q → q ˜ χ 0 1 and ˜ g → q ¯ q ˜ χ 0 1 ) and cascade ... See full document

36

Search for new phenomena with multiple charged leptons in proton–proton collisions at $\sqrt{s}= 13$ $\,\text {TeV}$

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 ... See full document

42

Search for new physics in the monophoton final state in proton-proton collisions at $ \sqrt{s}=13 $ TeV

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 ...12.9 fb1 of integrated ... See full document

36

Search for resonant $WZ$ production in the fully leptonic final state in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector

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 ... See full document

21

Search for new phenomena in the dijet mass distribution using $p-p$ collision data at $\sqrt{s}=8$ TeV with the ATLAS detector

Search for new phenomena in the dijet mass distribution using $p-p$ collision data at $\sqrt{s}=8$ TeV with the ATLAS detector

... clusters using a dis- tance parameter of R = ...interactions in the same and neighboring bunch cross- ings are corrected for using the calibration procedure described in ... See full document

27

Search for new phenomena in different-flavour high-mass dilepton final states in pp collisions at $\sqrt{s}=13$  Tev with the ATLAS detector

Search for new phenomena in different-flavour high-mass dilepton final states in pp collisions at $\sqrt{s}=13$  Tev with the ATLAS detector

... Pages 13 , L. Pacheco Rodriguez 137 , C. Padilla Aranda 13 , ..., S. Palazzo 39a,39b , S. Palestini 32 , M. Palka 40b , D. Pallin 36 , ... 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

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 ... See full document

24

Search for new phenomena with the $M_{\mathrm {T2}}$ variable in the all-hadronic final state produced in proton–proton collisions at $\sqrt{s} = 13$ $\,\text {TeV}$

Search for new phenomena with the $M_{\mathrm {T2}}$ variable in the all-hadronic final state produced in proton–proton collisions at $\sqrt{s} = 13$ $\,\text {TeV}$

... feature of the CMS apparatus is a superconducting solenoid of 6 m internal diam- eter, providing a magnetic field of ...Within the solenoid volume are a silicon pixel and strip tracker, ... See full document

46

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

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 presence ... See full document

48

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

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

... overlap of selected events in data between the Meff-based and RJR-based ...Each of the axes listing the various SRs are organized in the same order, ... See full document

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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

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

... A search for both resonant and nonresonant production of pairs of Standard Model Higgs bosons has been carried out in the dominant b¯bb¯b channel with ...3.2 fb1 ... 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

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

... reported of a search for new phenomena, such as supersymmetric particle production, that could be observed in high-energy protonproton ...Events with large ... See full document

22

Performance of missing transverse momentum reconstruction with the ATLAS detector using proton-proton collisions at $\sqrt{s}$ = 13 TeV

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 protonproton (pp) collisions measured with the ATLAS detector [ 1 ] at ... 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

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

... between the shapes of the E γ T, iso distributions of real photons and jets faking photons; the latter typically have a large E T, iso γ value due to nearby particles produced in ... See full document

38

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

... Measurements in the inner detector are used to recon- struct tracks from charged ...particles. The resulting tracks are then used to reconstruct collision vertices from pp inter- ... See full document

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