The ATLAS Experiment at the CERN Large Hadron Collider
By C. Benchouk, M. Bendel, B. Benedict, N. Benekos, J. Beneš, Y. Benhammou, G. Benincasa, D. Benjamin, J. Bensinger, K. Benslama and 233 more. 2008
5,955 citations recorded by the source corpus.
View Paper: https://www.semanticscholar.org/paper/a0d533492817952818ee8b607e28c77edfff827c
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Citations in the corpus
- Measurement of the Z/ѵ* boson transverse momentum distribution in pp collisions at √s = 7 TeV with the ATLAS detector (2014, background): “ATLAS [26] is a multipurpose detector 2 consisting of an inner tracking system (ID) inside a 2 T superconducting solenoid, electromagnetic and hadronic calorimeters and, outermost, a toroidal large acceptance muon spectrometer (MS), surrounding the interaction point with almost full coverage.”
- The ATLAS Simulation Infrastructure (2010, methodology): “ATLAS [1], one of the general-purpose detectors at the Large Hadron Collider [2], began operation in 2008.”
- Electron reconstruction and identification efficiency measurements with the ATLAS detector using the 2011 LHC proton–proton collision data (2014, methodology): “A detailed description of the detector is provided elsewhere [8].”
- Jet reconstruction and performance using particle flow with the ATLAS Detector (2017, background): “A complication, at the high luminosities encountered by the ATLAS detector [2], is that multiple interactions can contribute to the detector signals associated with a single bunch-crossing (pile-up).”
- The ATLAS Inner Detector commissioning and calibration (2010, background): “Level-2 and Event Filter together form the High Level Trigger (HLT) [1].”
- Performance of the ATLAS muon triggers in Run 2 (2020, background): “Following an L1 accept decision, the pT thresholds and the corresponding detector regions, called regions of interest (RoIs), are sent to the HLT for further consideration [1, 40].”
- Measurement of the Inelastic Proton-Proton Cross Section at root s=13 TeV with the ATLAS Detector at the LHC (2016, background): “The ATLAS detector is a cylindrical particle detector1 composed of several subdetector layers [17].”
- Search for squarks and gluinos with the ATLAS detector in final states with jets and missing transverse momentum using 20.3 $fb^{-1}$ of $\sqrt{s}$ = 8 TeV proton-proton collision data (2014, unknown): “This analysis [3] [4] is searching for supersymmetric particles assuming R-parity conservation (therefore q̃ and g̃ must be produced in pairs (g̃g̃, q̃q̃, q̃g̃)) and that the χ̃01 is the Lightest Supersymmetric Particle (LSP).”
- Measurements of Higgs boson production and couplings in diboson final states with the ATLAS detector at the LHC (2013, methodology): “The results reported here are based on the data samples recorded with the ATLAS detector [11] in 2011 (at √ s = 7 TeV) and 2012 (at √ s = 8 TeV), corresponding to integrated luminosities of about 4.”
- Evidence for light-by-light scattering in heavy-ion collisions with the ATLAS detector at the LHC (2017, unknown): “ATLAS is a cylindrical particle detector composed of several sub-detectors 23 .”
- Study of the spin and parity of the Higgs boson in diboson decays with the ATLAS detector (2015, unknown): “[11].”
- Electron efficiency measurements with the ATLAS detector using 2012 LHC proton–proton collision data (2016, unknown): “In the ATLAS detector [1], electrons in the central detector region are triggered by and reconstructed from energy deposits in the electromagnetic (EM) calorimeter that are matched to a track in the inner detector (ID).”
- Heavy Neutral Leptons at FASER (2018, unknown): “However, they are typically produced with low-pT and therefore will move along the beam pipe and escape detection in the ATLAS [2] and CMS [3] experiments.”
- Performance of b-jet identification in the ATLAS experiment (2015, methodology): “The ATLAS detector is a large, general-purpose collider detector and is described in detail elsewhere [1].”