ATLAS Insertable B-Layer Technical Design Report

By M. Capeans, T. Flick, R. Vuillermet, G. Darbo, H. Pernegger, K. Einsweiller, M. Garcia-Sciveres, M. Elsing, O. Røhne, C. Gemme. 2010

1,052 citations recorded by the source corpus.

View Paper: https://www.semanticscholar.org/paper/bae11e8229d2457862bd86683c7854db1ba30e26

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Citations in the corpus

Search for electroweak production of supersymmetric states in scenarios with compressed mass spectra at √s = 13 TeV with the ATLAS detector (2017, unknown): “The innermost pixel detector layer, the insertable B-layer [50], was added for ﬃﬃﬃ s p ¼ 13 TeV data-taking to improve tracking performance.”
Performance of the ATLAS trigger system in 2015 (2016, background): “A new innermost pixel-detector layer, the insertable B-layer (IBL), was added during LS1 at a radius of 33 mm around a new and thinner beam pipe [7].”
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, background): “One significant upgrade for the √ s = 13 TeV running period is the installation of the insertable B-layer [31], an additional pixel layer close to the interaction pointwhich provides high-resolution hits at small radius to improve the tracking performance.”
Combination of searches for invisible decays of the Higgs boson using 139 fb−1 of proton-proton collision data at s=13 TeV collected with the ATLAS experiment (2023, unknown): “• → or muons ( Z E missT ) [36] • ¯ τ • VBF topology in association with an emitted photon (VBF + • gluon–gluon fusion, in association with a high p jet (Jet + all of which use the full data sample, corresponding to an integrated luminosity of 139 fb − 1 .”
Production and integration of the ATLAS Insertable B-Layer (2018, methodology): “3 The as-built IBL radiation length was evaluated using the ATLAS geometry model, as discussed in the IBL TDR [6].”
Jet energy scale measurements and their systematic uncertainties in proton-proton collisions at √s=13 TeV with the ATLAS detector (2017, methodology): “The track reconstruction was updated in 2015 to include the IBL and uses a neural network clustering algorithm [14], improving the separation of nearby tracks and the reconstruction performance in the high-luminosity conditions of Run 2.”
Evidence for the associated production of the Higgs boson and a top quark pair with the ATLAS detector (2017, unknown): “It includes, for the √ s = 13 TeV running period, a newly installed innermost pixel layer, the insertable B-layer [40].”
Search for a scalar partner of the top quark in the jets plus missing transverse momentum final state at √s=13 TeV with the ATLAS detector (2017, unknown): “The newly installed innermost layer of pixel sensors [35] was operational for the first time during the 2015 data-taking.”
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): “The ID consists of a silicon pixel detector (including the insertable B-layer [15] installed before the start of Run 2), of a silicon microstrip detector, and of a transition radiation tracker (TRT).”
Search for exclusive Higgs and Z boson decays to ϕγ and ργ with the ATLAS detector (2017, background): “A new innermost pixeldetector layer, the insertable B-layer (IBL), was added for data taking in 2015 and 2016 which provides an additional measurement at a radius of about 33mm around a new and thinner beam pipe [30, 31].”
Luminosity determination in $pp$ collisions at $\sqrt{s}=13$ TeV using the ATLAS detector at the LHC (2022, background): “The measurement was derived from randomly sampled colliding-bunch crossings, where only the data from the silicon tracking detectors (i.e. the SCT and pixel detectors, including a new innermost layer, the ‘insertable B-layer’ (IBL) [11, 12] added before Run 2) were read out, typically at 200 Hz duri”
Heavy-flavour and quarkonium production in the LHC era: from proton–proton to heavy-ion collisions (2015, methodology): “During LS1, ATLAS achieved the installation of the Insertable B-Layer (IBL) [814], which is an additional fourth pixel layer, placed closer to the beam pipe at an average radius of 33 mm.”
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 (2019, methodology): “[40] ATLAS Collaboration, ATLAS insertable B-layer technical design report, Report No.”
Performance of the ATLAS track reconstruction algorithms in dense environments in LHC Run 2 (2017, methodology): “The IBL has a mean radius of 33 mm and a typical IBL pixel has a size of 50 µm by 250 µm in the transverse and longitudinal directions with a sensor thickness of 200 µm.”