4 research outputs found

    The Laser calibration of the Atlas Tile Calorimeter during the LHC run 1

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    International audienceThis article describes the Laser calibration system of the ATLAS hadronic Tile Calorimeter that has been used during the run 1 of the LHC . First, the stability of the system associated readout electronics is studied. It is found to be stable with variations smaller than 0.6 %. Then, the method developed to compute the calibration constants, to correct for the variations of the gain of the calorimeter photomultipliers, is described. These constants were determined with a statistical uncertainty of 0.3 % and a systematic uncertainty of 0.2 % for the central part of the calorimeter and 0.5 % for the end-caps. Finally, the detection and correction of timing mis-configuration of the Tile Calorimeter using the Laser system are also presented

    Search for pair production of third-generation leptoquarks decaying into a bottom quark and a τ\tau -lepton with the ATLAS detector

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    International audienceA search for pair-produced scalar or vector leptoquarks decaying into a b-quark and a τ\tau -lepton is presented using the full LHC Run 2 (2015–2018) data sample of 139 fb−1^{-1} collected with the ATLAS detector in proton–proton collisions at a centre-of-mass energy of s=13\sqrt{s} =13 TeV. Events in which at least one τ\tau -lepton decays hadronically are considered, and multivariate discriminants are used to extract the signals. No significant deviations from the Standard Model expectation are observed and 95% confidence-level upper limits on the production cross-section are derived as a function of leptoquark mass and branching ratio B\mathcal {B} into a τ\tau -lepton and b-quark. For scalar leptoquarks, masses below 1460 GeV are excluded assuming B=100\mathcal {B}=100%, while for vector leptoquarks the corresponding limit is 1650 GeV (1910 GeV) in the minimal-coupling (Yang–Mills) scenario

    Luminosity determination in pppp collisions at s=13\sqrt{s}=13 TeV using the ATLAS detector at the LHC

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    The luminosity determination for the ATLAS detector at the LHC during Run 2 is presented, with pppp collisions at s=13\sqrt{s}=13 TeV. The absolute luminosity scale is determined using van der Meer beam separation scans during dedicated running periods in each year, and extrapolated to the physics data-taking regime using complementary measurements from several luminosity-sensitive detectors. The total uncertainties in the integrated luminosities for each individual year of data-taking range from 0.9% to 1.1%, and are partially correlated between years. After standard data-quality selections, the full Run 2 pppp data sample corresponds to an integrated luminosity of 140.1±1.2140.1\pm 1.2 fb−1^{-1}, i.e. an uncertainty of 0.83%. A dedicated sample of low-pileup data recorded in 2017-18 for precision Standard Model physics measurements is analysed separately, and has an integrated luminosity of 338.1±3.1338.1\pm 3.1 pb−1^{-1}.The luminosity determination for the ATLAS detector at the LHC during Run 2 is presented, with pp collisions at a centre-of-mass energy s=13\sqrt{s}=13 TeV. The absolute luminosity scale is determined using van der Meer beam separation scans during dedicated running periods in each year, and extrapolated to the physics data-taking regime using complementary measurements from several luminosity-sensitive detectors. The total uncertainties in the integrated luminosity for each individual year of data-taking range from 0.9% to 1.1%, and are partially correlated between years. After standard data-quality selections, the full Run 2 pp data sample corresponds to an integrated luminosity of 140.1±1.2140.1\pm 1.2 fb−1\hbox {fb}^{-1}, i.e. an uncertainty of 0.83%. A dedicated sample of low-pileup data recorded in 2017–2018 for precision Standard Model physics measurements is analysed separately, and has an integrated luminosity of 338.1±3.1338.1\pm 3.1 pb−1\hbox {pb}^{-1}.The luminosity determination for the ATLAS detector at the LHC during Run 2 is presented, with pppp collisions at s=13\sqrt{s}=13 TeV. The absolute luminosity scale is determined using van der Meer beam separation scans during dedicated running periods in each year, and extrapolated to the physics data-taking regime using complementary measurements from several luminosity-sensitive detectors. The total uncertainties in the integrated luminosities for each individual year of data-taking range from 0.9% to 1.1%, and are partially correlated between years. After standard data-quality selections, the full Run 2 pppp data sample corresponds to an integrated luminosity of 140.1±1.2140.1\pm 1.2 fb−1^{-1}, i.e. an uncertainty of 0.83%. A dedicated sample of low-pileup data recorded in 2017-18 for precision Standard Model physics measurements is analysed separately, and has an integrated luminosity of 338.1±3.1338.1\pm 3.1 pb−1^{-1}

    Search for pair production of third-generation leptoquarks decaying into a bottom quark and a τ\tau-lepton with the ATLAS detector

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    A search for pair-produced scalar or vector leptoquarks decaying into a bb-quark and a τ\tau-lepton is presented using the full LHC Run 2 (2015-2018) data sample of 139 fb−1^{-1} collected with the ATLAS detector in proton-proton collisions at a centre-of-mass energy of s=13\sqrt{s}=13 TeV. Events in which at least one τ\tau-lepton decays hadronically are considered, and multivariate discriminants are used to extract the signals. No significant deviations from the Standard Model expectation are observed and 95% confidence-level upper limits on the production cross-section are derived as a function of leptoquark mass and branching ratio into the τ\tau-lepton. For scalar leptoquarks, masses below 1490 GeV are excluded assuming a 100% branching ratio, while for vector leptoquarks the corresponding limit is 1690 GeV (1960 GeV) in the minimal-coupling (Yang-Mills) scenario.A search for pair-produced scalar or vector leptoquarks decaying into a bb-quark and a τ\tau-lepton is presented using the full LHC Run 2 (2015-2018) data sample of 139 fb−1^{-1} collected with the ATLAS detector in proton-proton collisions at a centre-of-mass energy of s=13\sqrt{s}=13 TeV. Events in which at least one τ\tau-lepton decays hadronically are considered, and multivariate discriminants are used to extract the signals. No significant deviations from the Standard Model expectation are observed and 95% confidence-level upper limits on the production cross-section are derived as a function of leptoquark mass and branching ratio into the τ\tau-lepton. For scalar leptoquarks, masses below 1490 GeV are excluded assuming a 100% branching ratio, while for vector leptoquarks the corresponding limit is 1690 GeV (1960 GeV) in the minimal-coupling (Yang-Mills) scenario
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