527 research outputs found

    Measurement of the total cross section and Ļ -parameter from elastic scattering in pp collisions at āˆšs=13 TeV with the ATLAS detector

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    In a special run of the LHC with Ī²ā‹†= 2.5 km, protonā€“proton elastic-scattering events were recorded at s=13 TeV with an integrated luminosity of 340Ī¼b-1 using the ALFA subdetector of ATLAS in 2016. The elastic cross section was measured differentially in the Mandelstam t variable in the range from - t= 2.5 Ā· 10 - 4 GeV 2 to - t= 0.46 GeV 2 using 6.9 million elastic-scattering candidates. This paper presents measurements of the total cross section Ļƒtot , parameters of the nuclear slope, and the Ļ -parameter defined as the ratio of the real part to the imaginary part of the elastic-scattering amplitude in the limit tā†’ 0 . These parameters are determined from a fit to the differential elastic cross section using the optical theorem and different parameterizations of the t-dependence. The results for Ļƒtot and Ļ are Ļƒtot(ppā†’X)=104.7Ā±1.1mb,Ļ=0.098Ā±0.011. The uncertainty in Ļƒtot is dominated by the luminosity measurement, and in Ļ by imperfect knowledge of the detector alignment and by modelling of the nuclear amplitude

    Search for top-philic heavy resonances in pp collisions at s=13Ā TeV with the ATLAS detector

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    A search for the associated production of a heavy resonance with a top-quark or a top-antitop-quark pair, and decaying into a ttĀÆ pair is presented. The search uses the data recorded by the ATLAS detector in pp collisions at s=13Ā TeV at the Large Hadron Collider during the years 2015ā€“2018, corresponding to an integrated luminosity of 139Ā fb-1. Events containing exactly one electron or muon are selected. The two hadronically decaying top quarks from the resonance decay are reconstructed using jets clustered with a large radius parameter of R=1. The invariant mass spectrum of the two top quark candidates is used to search for a resonance signal in the range of 1.0Ā TeV to 3.2Ā TeV. The presence of a signal is examined using an approach with minimal model dependence followed by a model-dependent interpretation. No significant excess is observed over the background expectation. Upper limits on the production cross section times branching ratio at 95% confidence level are provided for a heavy Zā€² boson based on a simplified model, for Zā€² mass between 1.0Ā TeV and 3.0Ā TeV. The observed (expected) limits range from 21Ā (14)Ā fb to 119Ā (86)Ā fb depending on the choice of model parameters

    Measurement of the Higgs boson mass in the H ā†’ Z Zāˆ— ā†’ 4 decay channel using 139 fbāˆ’1 of āˆšs = 13 TeV pp collisions recorded by the ATLAS detector at the LHC

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    The mass of the Higgs boson is measured in the Hā†’ZZāŽā†’4ā„“ decay channel. The analysis uses protonā€“proton collision data from the Large Hadron Collider at a centre-of-mass energy of 13 TeV recorded by the ATLAS detector between 2015 and 2018, corresponding to an integrated luminosity of 139 fbāˆ’1. The measured value of the Higgs boson mass is 124.99Ā±0.18(stat.)Ā±0.04(syst.) GeV. In final states with muons, this measurement benefits from an improved momentum-scale calibration relative to that adopted in previous publications. The measurement also employs an analytic model that takes into account the invariant-mass resolution of the four-lepton system on a per-event basis and the output of a deep neural network discriminating signal from background events. This measurement is combined with the corresponding measurement using 7 and 8 TeV pp collision data, resulting in a Higgs boson mass of 124.94Ā±0.17(stat.)Ā±0.03(syst.) GeV

    Search for non-resonant Higgs boson pair production in the 2b+2ā„“+ETmiss final state in pp collisions at s = 13 TeV with the ATLAS detector

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    A search for non-resonant Higgs boson pair (HH) production is presented, in which one of the Higgs bosons decays to a b-quark pair (bbĀÆ) and the other decays to WW*, ZZ*, or Ļ„+Ļ„āˆ’, with in each case a final state with ā„“+ā„“āˆ’+ neutrinos (ā„“ = e, Ī¼). The analysis targets separately the gluon-gluon fusion and vector boson fusion production modes. Data recorded by the ATLAS detector in proton-proton collisions at a centre-of-mass energy of 13 TeV at the Large Hadron Collider, corresponding to an integrated luminosity of 140 fbāˆ’1, are used in this analysis. Events are selected to have exactly two b-tagged jets and two leptons with opposite electric charge and missing transverse momentum in the final state. These events are classified using multivariate analysis algorithms to separate the HH events from other Standard Model processes. No evidence of the signal is found. The observed (expected) upper limit on the cross-section for non-resonant Higgs boson pair production is determined to be 9.7 (16.2) times the Standard Model prediction at 95% confidence level. The Higgs boson self-interaction coupling parameter ĪŗĪ» and the quadrilinear coupling parameter Īŗ2V are each separately constrained by this analysis to be within the ranges [āˆ’6.2, 13.3] and [āˆ’0.17, 2.4], respectively, at 95% confidence level, when all other parameters are fixed

    Search for pair production of squarks or gluinos decaying via sleptons or weak bosons in final states with two same-sign or three leptons with the ATLAS detector

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    A search for pair production of squarks or gluinos decaying via sleptons or weak bosons is reported. The search targets a final state with exactly two leptons with same-sign electric charge or at least three leptons without any charge requirement. The analysed data set corresponds to an integrated luminosity of 139 fbāˆ’1 of proton-proton collisions collected at a centre-of-mass energy of 13 TeV with the ATLAS detector at the LHC. Multiple signal regions are defined, targeting several SUSY simplified models yielding the desired final states. A single control region is used to constrain the normalisation of the WZ + jets background. No significant excess of events over the Standard Model expectation is observed. The results are interpreted in the context of several supersymmetric models featuring R-parity conservation or R-parity violation, yielding exclusion limits surpassing those from previous searches. In models considering gluino (squark) pair production, gluino (squark) masses up to 2.2 (1.7) TeV are excluded at 95% confidence level

    Search for new phenomena in multi-body invariant masses in events with at least one isolated lepton and two jets using āˆšs = 13 TeV protonā€“proton collision data collected by the ATLAS detector

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    A search for resonances in events with at least one isolated lepton (e or Ī¼) and two jets is performed using 139 fb āˆ’1 of s = 13 TeV protonā€“proton collision data recorded by the ATLAS detector at the LHC. Deviations from a smoothly falling background hypothesis are tested in three- and four-body invariant mass distributions constructed from leptons and jets, including jets identified as originating from bottom quarks. Model-independent limits on generic resonances characterised by cascade decays of particles leading to multiple jets and leptons in the final state are presented. The limits are calculated using Gaussian shapes with different widths for the invariant masses. The multi-body invariant masses are also used to set 95% confidence level upper limits on the cross-section times branching ratios for the production and subsequent decay of resonances predicted by several new physics scenarios. [Figure not available: see fulltext.]

    Combination of searches for invisible decays of the Higgs boson using 139 fbāˆ’1 of proton-proton collision data at āˆšs = 13 TeV collected with the ATLAS experiment

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    Many extensions of the Standard Model predict the production of dark matter particles at the LHC. Sufficiently light dark matter particles may be produced in decays of the Higgs boson that would appear invisible to the detector. This Letter presents a statistical combination of searches for H ā†’ invisible decays where multiple production modes of the Standard Model Higgs boson are considered. These searches are performed with the ATLAS detector using 139 fbāˆ’1 of protonā€“proton collisions at a centreā€“ofā€“mass energy of āˆšs = 13 TeV at the LHC. In combination with the results at āˆšs = 7 TeV and 8 TeV, an upper limit on the H ā†’ invisible branching ratio of 0.107 (0.077) at the 95% confidence level is observed (expected). These results are also interpreted in the context of models where the 125 GeV Higgs boson acts as a portal to dark matter, and limits are set on the scattering cross-section of weakly interacting massive particles and nucleons

    Measurement of the production cross-section of J/Ļˆ and Ļˆ(2S) mesons in pp collisions at s=13Ā TeV with the ATLAS detector

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    Measurements of the differential production cross-sections of prompt and non-prompt J/Ļˆ and Ļˆ(2S) mesons with transverse momenta between 8 and 360Ā GeV and rapidity in the range |y|<2 are reported. Furthermore, measurements of the non-prompt fractions of J/Ļˆ and Ļˆ(2S), and the prompt and non-prompt Ļˆ(2S)-to-J/Ļˆ production ratios, are presented. The analysis is performed using 140Ā fb-1 of s=13Ā TeV pp collision data recorded by the ATLAS detector at the LHC during the years 2015ā€“2018

    Search for third-generation vector-like leptons in pp collisions at āˆšs = 13 TeV with the ATLAS detector

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    A search for vector-like leptons in multilepton (two, three, or four-or-more electrons plus muons) final states with zero or more hadronic Ļ„-lepton decays is presented. The search is performed using a dataset corresponding to an integrated luminosity of 139 fbāˆ’1 of proton-proton collisions at a centre-of-mass energy of 13 TeV recorded by the ATLAS detector at the LHC. To maximize the separation of signal and background, a machine-learning classifier is used. No excess of events is observed beyond the Standard Model expectation. Using a doublet vector-like lepton model, vector-like leptons coupling to third-generation Standard Model leptons are excluded in the mass range from 130 GeV to 900 GeV at the 95% confidence level, while the highest excluded mass is expected to be 970 GeV. [Figure not available: see fulltext.]
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