Optimisation of the ATLAS $b$-tagging performance for the 2016 LHC Run

By A. Calandri, R. Zaidan, V. Dao, Y. Rodina, R. Kosseifi, M. Ghneimat, M. Cristinziani, E. L. Quilleuc, A. Coccaro, G. Piacquadio and 10 more. 2016

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Measurements of Higgs boson properties in the diphoton decay channel with 36 fb$^{-1}$ of $pp$ collision data at $\sqrt{s} = 13$ TeV with the ATLAS detector (2018, unknown): “Jets consistent with the decay of a b-hadron are identified using a multivariate discriminant, having as input information from track impact parameters and secondary vertices [84, 85].”
Search for electroweak production of supersymmetric particles in final states with two or three leptons at \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\odd (2018, methodology): “Identification of jets containing b-hadrons (b-jets), so called b-tagging, is performed with the MV2c10 algorithm, a multivariate discriminant making use of track impact parameters and reconstructed secondary vertices [84, 85].”
Evidence for the associated production of the Higgs boson and a top quark pair with the ATLAS detector (2017, unknown): “All track pairs within a jet are tested to produce a vertex and such vertices are rejected if they are likely to originate from long lived light quark jets (such as K0 s or Λ0), photon conversions or hadronic interactions [79].”