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This correction is applied at the electromagnetic scale as the first step of the calibration scheme. Further details on the pile-up offset correction can be found in [10]. 3 Vertices are counted using a criterion of having at least 5 associated tracks. 2 Jetorigin Correction Calorimeter jets are reconstructed using the geometrical centre of the ATLAS detector as reference to calculate the direction of jets and their constituents (see Sect. 3). The direction of each topoclusteror tower included in a jet is corrected to point back to the primary vertex with the highest associated sum of track transverse momenta 2 ) in the event.

Phys. J. C 70, 823–874 (2010) 31. A. , Status of Geant4 Hadronic Physics for the Simulation of LHC Experiments at the LHC Physics Program, CERN-LC GAPP-2010-02, CERN, Geneva, May 2010 32. G. P. Wellisch, String parton models in Geant4, arXiv:nucl-th/0306007 33. W. Bertini, Intranuclear-cascade calculation of the secondary nucleon spectra from nucleonnucleus interactions in the energy range 340 to 2,900 mev and comparisons with experiment. Phys. Rev. A 188, 1711–1730 (1969) 34. P. , Measurement of pion and proton response and longitudinal shower profiles up to 20 nuclear interaction lengths with the ATLAS Tile calorimeter.

Track candidates are built from space points in the silicon layers, fitted and then extended to the TRT using the full ID information. A dedicated vertex finder identifies the primary vertex as that with the highest sum of pT of the tracks pointing to it, normalized by the number of tracks. 1 The radius of a drift circle corresponds to the distance of closest approach of the charged particle to the wire as estimated from the time needed for drift electrons to reach the wire. 24 3 The ATLAS Experiment Fig.

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Acoustical Measurements (rev.) by L. Beranek


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